Publications of Seog Oh    :recent first  alphabetical  combined listing:

%% Papers Published   
@article{fds309849,
   Author = {Kim, YS and Noz, ME and Oh, SH},
   Title = {Representations of the Poincaré group for relativistic
             extended hadrons},
   Journal = {Journal of Mathematical Physics},
   Volume = {20},
   Number = {7},
   Pages = {1341-1344},
   Publisher = {AIP Publishing},
   Year = {1978},
   Month = {January},
   url = {http://dx.doi.org/10.1063/1.524237},
   Abstract = {Representations of the Poincaré group are constructed from
             the relativistic harmonic oscillator wave functions which
             have been effective in describing the physics of internal
             quark motions in the relativistic quark model. These wave
             functions are solutions of the Lorentz-invariant harmonic
             oscillator differential equation in the "cylindrical"
             coordinate system moving with the hadronic velocity in which
             the time-separation variable is treated separately. This
             result enables us to assert that the hadronic mass spectrum
             is generated by the internal quark level excitation, and
             that the hadronic spin is due to the internal orbital
             angular momentum. An addendum relegated to PAPS contains
             discussions of detailed calculational aspects of the Lorentz
             transformation, and of solutions of the oscillator equation
             which are diagonal in the Casimir operators of the
             homogeneous Lorentz group. It is shown there that the
             representation of the homogeneous Lorentz group consists of
             solutions of the oscillator partial differential equation in
             a "spherical" coordinate system in which the
             Lorentz-invariant Minkowskian distance between the
             constituent quarks is the radial variable. © 1979 American
             Institute of Physics.},
   Doi = {10.1063/1.524237},
   Key = {fds309849}
}

@article{fds309845,
   Author = {Hegedus, LL and Herz, RK and Oh, SH and Aris, R},
   Title = {Effect of catalyst loading on the simultaneous reactions of
             NO, CO, and O2},
   Journal = {Journal of Catalysis},
   Volume = {57},
   Number = {3},
   Pages = {513-515},
   Publisher = {Elsevier BV},
   Year = {1979},
   url = {http://dx.doi.org/10.1016/0021-9517(79)90017-4},
   Doi = {10.1016/0021-9517(79)90017-4},
   Key = {fds309845}
}

@article{fds309848,
   Author = {Oh, SH and Baron, K and Sloan, EM and Hegedus, LL},
   Title = {Effects of catalyst particle size on multiple steady
             states},
   Journal = {Journal of Catalysis},
   Volume = {59},
   Number = {2},
   Pages = {272-277},
   Year = {1979},
   url = {http://dx.doi.org/10.1016/S0021-9517(79)80031-7},
   Abstract = {Carbon monoxide oxidation experiments were carried out over
             Pt-alumina catalyst particles of various sizes. The width of
             the conversion-temperature hysteresis loop goes through a
             maximum as the degree of intrapellet diffusion resistances
             (i.e., catalyst particle size) is varied. No hysteresis was
             observed over finely powdered catalysts. The above
             observations are in agreement with the qualitative
             predictions of diffusion-reaction theory, and provide
             further evidence to suggest that the steady-state
             multiplicities observed here were caused by the interactions
             between reaction and intrapellet diffusion resistances. The
             hysteresis loop was found to shift along the temperature
             axis as the pellet size was varied. The hysteresis occurred
             at the lowest temperature when catalyst particles of an
             intermediate size were used. Both larger and smaller
             particles showed multiplicity at higher temperatures. This
             observation is also consistent with diffusion-reaction
             theory. © 1979 Academic Press, Inc. All rights
             reserved.},
   Doi = {10.1016/S0021-9517(79)80031-7},
   Key = {fds309848}
}

@article{fds309847,
   Author = {Kim, YS and Noz, ME and Oh, SH},
   Title = {Lorentz deformation in the O(4) and light-cone coordinate
             systems},
   Journal = {Journal of Mathematical Physics},
   Volume = {21},
   Number = {5},
   Pages = {1224-1228},
   Publisher = {AIP Publishing},
   Year = {1979},
   Month = {January},
   url = {http://dx.doi.org/10.1063/1.524513},
   Abstract = {A formalism is developed for describing Lorentz deformation
             properties of extended hadrons in terms of solutions of the
             harmonic oscillator equation in the O(4) and light-cone
             coordinate systems. The physical hadronic wave function
             discussed in previous papers is written as a linear
             expansion of orthonormal functions in those coordinates
             which form representations of compact groups. The
             separability of the oscillator equation is shown to play the
             essential role in developing the proposed mathematics. ©
             1980 American Institute of Physics.},
   Doi = {10.1063/1.524513},
   Key = {fds309847}
}

@article{fds309844,
   Author = {Brick, D and Shapiro, AM and Widgoff, M and Barreiro, F and Benary, O and Brau, JE and Hafen, ES and Hulsizer, RI and Kistiakowsky, V and Napier,
             A and Oh, SH and Pless, IA and Silverman, JP and Trepagnier, PC and Yamamoto, RK and Kittel, W and Schouten, M and Cohn, HO and Jacques, P and Stamer, P and Watts, TL and Brucker, EB and Koller, EL and Bugg, WM and Handler, T},
   Title = {Inclusive and semi-inclusive charge structure in
             π-p multiparticle production at 147
             GeV/c},
   Journal = {Nuclear Physics, Section B},
   Volume = {152},
   Number = {1},
   Pages = {45-60},
   Publisher = {Elsevier BV},
   Year = {1979},
   Month = {May},
   url = {http://dx.doi.org/10.1016/0550-3213(79)90078-6},
   Abstract = {A new method of analysis (leading charge model) based on the
             zone graph technique is used to separate charged particles
             produced in the target, projectile and central regions of
             phase space. A significant fraction of the centrally
             produced particles follow a Bose momentum distribution with
             temperature of 131 ± 2 MeV. © 1979.},
   Doi = {10.1016/0550-3213(79)90078-6},
   Key = {fds309844}
}

@article{fds309846,
   Author = {Kim, YS and Noz, ME and Oh, SH},
   Title = {Lorentz deformation and the jet phenomenon},
   Journal = {Foundations of Physics},
   Volume = {9},
   Number = {11-12},
   Pages = {947-954},
   Publisher = {Springer Nature},
   Year = {1979},
   Month = {December},
   url = {http://dx.doi.org/10.1007/BF00708703},
   Abstract = {It is shown that the Lorentz-deformation property discussed
             in previous papers is consistent with the hadronic jet
             phenomenon in high-energy production processes. © 1979
             Plenum Publishing Corporation.},
   Doi = {10.1007/BF00708703},
   Key = {fds309846}
}

@article{fds309843,
   Author = {Oh, SH and Kim, YS and Noz, ME},
   Title = {Lorentz deformation and the jet phenomenon. II. Explanation
             of the nearly constant average jet transverse
             momentum},
   Journal = {Foundations of Physics},
   Volume = {10},
   Number = {7-8},
   Pages = {635-639},
   Publisher = {Springer Nature},
   Year = {1980},
   Month = {August},
   url = {http://dx.doi.org/10.1007/BF00715044},
   Abstract = {It is shown that the jet mechanism derivable from the
             Lorentz deformation picture leads to a nearly constant
             average jet transverse momentum. It is pointed out that this
             is consistent with the high-energy experimental data. It is
             pointed out further that this result strengthens the
             physical basis for the minimal time-energy uncertainty
             combined covariantly with Heisenberg's space-momentum
             uncertainty relation. © 1980 Plenum Publishing
             Corporation.},
   Doi = {10.1007/BF00715044},
   Key = {fds309843}
}

@article{fds309841,
   Author = {Brick, D and Shapiro, AM and Widgoff, M and Alyea, ED and Hafen, ES and Hulsizer, RI and Kistiakowsky, V and Levy, A and Lutz, P and Oh, SH and Pless, IA and Silverman, JP and Stoughton, TB and Trepagnier, PC and Yamamoto, RK and Cohn, HO and Plano, RJ and Stamer, P and Brucker, EB and Koller, EL and Bugg, WM and Condo, GT and Ludlam, T and Taft,
             HD},
   Title = {Multiple correlations and high-transverse-momentum jets in
             147-GeV/c -p interactions},
   Journal = {Physical Review D},
   Volume = {24},
   Number = {3},
   Pages = {590-604},
   Publisher = {American Physical Society (APS)},
   Year = {1981},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.24.590},
   Abstract = {We examine multiparticle correlations in a -p experiment at
             147 GeV/c performed by the Proportional Hybrid System
             Consortium. The major aim of this paper is to demonstrate
             the existence of clusters in our data. We use different
             statistical algorithms to assemble into clusters the
             particles in each event which are associated by virtue of
             small relative angles. We find that these clusters are
             stable against different choices of metric and/or algorithm,
             and reproduce the effects previously observed in the data
             corresponding to clusters. Some of these clusters have
             properties similar to high-pT jets. A detailed study of
             these jetlike clusters is described, and comparisons with
             some counter experiments are discussed. © 1981 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.24.590},
   Key = {fds309841}
}

@article{fds309842,
   Author = {Schouten, M and de Bock, H and Crijns, F and Dziembowski, Z and Kittel,
             W and Metzger, W and Pols, C and Van de Walle and R and Brick, D and Rudnicka,
             H and Shapiro, AM and Widgoff, M and Ansorge, RE and Neale, WW and Ward,
             DR and Whyman, BM and Burnstein, RA and Rubin, HA and Alyea, ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Frank, TAJ and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RJ and Kistiakowsky, V and Lutz, P and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Wu, Y and Yamamoto,
             RK and Grard, F and Hanton, J and Henri, V and Herquet, P and Lesceux, JM and Pilette, P and Windmolders, R and Cohn, HO and Bressi, G and Calligarich, E and Castoldi, C and Dolfini, R and Ratti, S and DiMarco,
             R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer, P and Watts,
             TL and Brucker, EB and Koller, EL and Taylor, S and Berny, L and Dado, S and Goldberg, J and Toaff, S and Alexander, G and Benary, O and Grunhaus, J and Heifetz, R and Levy, A and Bugg, WM and Condo, GT and Handler, T and Hart,
             EL and Rogers, AH and Eisenberg, Y and Karshon, U and Ronat, EE and Shapira, A and Yaari, R and Yekutieli, G and Ludlam, TW and Steiner, R and Taft, HD},
   Title = {Inclusive and semi-inclusive ϱ<sup>0</sup>
             production in π<sup>+</sup>/π<sup>-</sup>/K<sup>+</sup>/pp
             interactions at 147 GeV/c},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {9},
   Number = {2},
   Pages = {93-104},
   Publisher = {Springer Nature},
   Year = {1981},
   Month = {January},
   url = {http://dx.doi.org/10.1007/BF01410644},
   Abstract = {In an experiment with the 30-inch Hybrid Spectrometer at
             Fermilab we have obtained the inclusive and semi-inclusive
             production cross sections of the ρ{variant}0 meson using a
             conventional background subtraction technique. Production
             cross sections for the ρ{variant}0 are derived as a
             function of the Feynman scaling variable x, and the
             transverse variables pt2 and Et=(pt2+M2)1/2. The
             longitudinal distributions are compared with the (1-x)
             dependence of the proton and meson valence quark structure
             functions, using various forms of recombination and
             fragmentation models. The transverse distributions are
             compared with thermodynamic models. We give density matrix
             elements for the ρ{variant}0 production from pions in the
             extreme forward region. © 1981 Springer-Verlag.},
   Doi = {10.1007/BF01410644},
   Key = {fds309842}
}

@article{fds309840,
   Author = {Brick, D and Rudnicka, H and Shapiro, AM and Widgoff, M and Ansorge, RE and Neale, WW and Ward, DR and Whyman, BM and Burnstein, RA and Rubin, HA and Alyea, ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Elahy, M and Frank, T and Hafen, ES and Haridas, P and Huang,
             D and Hulsizer, RI and Kistiakowsky, V and Lutz, P and Oh, SH and Pless,
             IA and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier,
             PC and Wu, Y and Yamamoto, RK and Grard, F and Hanton, J and Henri, V and Herquet, P and Lesceux, JM and Pilette, P and Windmolders, R and DeBock,
             H and Crijns, F and Kittel, W and Metzger, W and Pols, C and Schouten, M and van de Walle, R and Cohn, HO and Bressi, G and Calligarich, E and Castoldi, C and Dolfini, R and Ratti, S and DiMarco, R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer, P and Watts, TL and Brucker, EB and Koller, EL and Taylor, S and Berny, L and Dado, S and Goldberg, J and Toaff, S and Alexander, G and Benary, O and Grunhaus, J and Heifetz, R and Levy, A and Bugg, WM and Condo, GT and Handler, T and Hart, EL and Rogers,
             AH and Eisenberg, Y and Hochman, D and Karshon, U and Ronat, EE and Shapira, A and Yaari, R and Yekutieli, G and Ludlam, T and Steiner, R and Taft, H},
   Title = {The effective-energy dependence of the charged particle's
             multiplicity in p/π+/K+ interactions
             on protons at 147 GeV/c},
   Journal = {Physics Letters B},
   Volume = {103},
   Number = {3},
   Pages = {241-246},
   Publisher = {Elsevier BV},
   Year = {1981},
   Month = {July},
   url = {http://dx.doi.org/10.1016/0370-2693(81)90750-4},
   Abstract = {The energy dependence of the average of the charged
             multiplicity and its dispersion in π+/K+/p interaction on
             protons at 147 GeV/c is found to be the same as in e+e-
             annihilations if an "effective energy" variable is used
             instead of the total energy. The effective energy Seff is
             defined as the invariant mass of all secondaries left after
             the two leading particles have been removed. Fitting the
             expression aSeffb to the average charge multiplicity
             〈nch〉, we find the power b to be in good agreement with
             the value of 0.25 predicted by Fermi's statistical model and
             by Landau's hydrodynamical model. © 1981.},
   Doi = {10.1016/0370-2693(81)90750-4},
   Key = {fds309840}
}

@article{fds309832,
   Author = {Brick, D and Rudnicka, H and Shapiro, AM and Widgoff, M and Ansorge, RE and Neale, WW and Ward, DR and Whyman, BM and Burnstein, RA and Rubin, HA and Alyea, ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Dolfini, R and Frank, T and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RI and Kistiakowsky, V and Lutz, P and Noguchi,
             S and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow, V and Tether,
             S and Trepagnier, PC and Wu, Y and Yamamoto, RK and Grard, F and Hanton, J and Henri, V and Herquet, P and Lesceux, JM and Pilette, P and Windmolders,
             R and Debock, H and Crijns, F and Kittel, W and Metzger, W and Pols, C and Schouten, M and Van De Walle and R and Cohn, HO and Bressi, G and Calligarich, E and Castoldi, C and Ratti, S and Dimarco, R and Jacques,
             PF and Kalelkar, M and Plano, RJ and Stamer, P and Watts, TL and Brucker,
             EB and Koller, EL and Taylor, S and Berny, L and Dado, S and Goldberg, J and Toaff, S and Alexander, G and Benary, O and Grunhaus, J and Heifetz, R and Levy, A and Bugg, WM and Condo, GT and Handler, T and Hart, EL and Rogers,
             AH and Eisenberg, Y and Hochman, D and Karshon, U and Ronat, EE and Shapira, A and Yaari, R and Yekutieli, G and Ludlam, T and Steiner, R and Taft, H},
   Title = {Topological, total, and elastic cross sections for K+p, +p,
             and pp interactions at 147 GeV/c},
   Journal = {Physical Review D},
   Volume = {25},
   Number = {11},
   Pages = {2794-2806},
   Publisher = {American Physical Society (APS)},
   Year = {1982},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.25.2794},
   Abstract = {The Fermilab hybrid 30-in. bubble-chamber spectrometer was
             exposed to a tagged 147-GeV/c positive beam containing +,
             K+, and p. A sample of 3003 K+p, 19 410 pp, and 20 745 +p
             interactions is used to derive fn, n, f2cc, and ncD for each
             beam particle. These values are compared to values obtained
             at other, mostly lower, beam momenta. The overall dependence
             of on Ea, the available center-of-mass energy, for these
             three reactions as well as -p and pp interactions has been
             determined. © 1982 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.25.2794},
   Key = {fds309832}
}

@article{fds309833,
   Author = {Brick, D and Rudnicka, H and Shapiro, AM and Widgoff, M and Ansorge, RE and Neale, WW and Ward, DR and Whyman, BM and Burnstein, RA and Rubin, HA and Alyea, ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Dolfini, R and Frank, TAJ and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RI and Kistiakowsky, V and Lutz, P and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Wu, Y and Yamamoto, RK and Grard, F and Hanton, J and Henri, V and Herquet, P and Lesceux, JM and Pilette, P and Windmolders,
             R and de Bock, H and Crijns, F and Kittel, W and Metzger, W and Pols, C and Schouten, M and Van de Walle and R and Cohn, HO and Bressi, G and Calligarich, E and Castoldi, C and Ratti, S and DiMarco, R and Jacques,
             PF and Kalelkar, M and Plano, RJ and Stamer, P and Watts, TL and Brucker,
             EB and Koller, EL and Taylor, S and Berny, L and Dado, S and Goldberg, J and Toaff, S and Alexander, G and Benary, O and Grunhaus, J and Heifetz, R and Levy, A and Bugg, WM and Condo, GT and Handler, T and Hart, EL and Rogers,
             AH and Eisenberg, Y and Hochman, D and Karshon, U and Ronat, EE and Shapira, A and Yaari, R and Yekutieli, G and Ludlam, TW and Steiner, R and Taft, HD},
   Title = {Approach to scaling in inclusive π+-
             ratios at 147 GeV/c},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {13},
   Number = {1},
   Pages = {11-17},
   Publisher = {Springer Nature},
   Year = {1982},
   Month = {January},
   url = {http://dx.doi.org/10.1007/BF01553627},
   Abstract = {The ratio of hadronic π+/π- production has been studied in
             the target fragmentation region of π+p, π-p, K+p and p p
             collisions at 147 GeV/c beam momentum. The difference
             between this ratio in the π+p and π-p data is less than at
             lower energies but still present. No difference exists
             anymore for the π+/π- ratio at this energy between K+p and
             pp collisions. Exclusion of diffraction dissociation and
             resonance production does not change the main conclusions.
             The energy dependence of the ratio for π+p and π-p
             collisions gives evidence for a universal asymptotic ratio
             for all beams. The pt-dependence at low-pt is in agreement
             with the expectation from geometrical correlation of the
             valence quarks. © 1982 Springer-Verlag.},
   Doi = {10.1007/BF01553627},
   Key = {fds309833}
}

@article{fds309834,
   Author = {Brick, D and Rudnicka, H and Shapiro, AM and Widgoff, M and Alyea, ED and Hafen, ES and Hulsizer, RI and Kistiakowsky, V and Levy, A and Lutz, P and Oh, SH and Pless, IA and Silverman, JP and Stoughton, TB and Trepagnier,
             PC and Yamamoto, RK and Cohn, HO and Kalelkar, M and Plano, RJ and Stamer,
             PE and Watts, TL and Brucker, EB and Koller, EL and Bugg, WM and Ludlam, T and Taft, HD},
   Title = {Comparison of 147 GeV/c π-p low transverse
             momentum hadron production with deep-inelastic
             leptoproduction},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {11},
   Number = {4},
   Pages = {335-341},
   Publisher = {Springer Nature America, Inc},
   Year = {1982},
   Month = {January},
   url = {http://dx.doi.org/10.1007/BF01578282},
   Abstract = {Distributions with respect to z and zR for the fastest and
             second fastest particles produced in both beam and target
             hemispheres from 147 GeV/c π- interactions are compared
             with each other and with the distributions for the fastest
             and second fastest particles from deepinelastic
             leptoproduction and Field-Feynman curves. The distributions
             and curves for the fastest particles are very similar, with
             the exception of the identified protons. Those for the
             second fastest are in agreement. Distributions with respect
             to z′R for the first through fourth fastest particles
             (excepting the protons) are all similar, suggesting that the
             shape of the distributions may be determined by the
             available longitudinal phase space. © 1982
             Springer-Verlag.},
   Doi = {10.1007/BF01578282},
   Key = {fds309834}
}

@article{fds309836,
   Author = {Brick, DH and Rudnicka, H and Shapiro, AM and Widgoff, M and Ansorge,
             RE and Neale, WW and Ward, DR and Burnstein, RA and Rubin, HA and Alyea,
             ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Elahy, M and Frank, T and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RI and Kistiakowsky, V and Lutz, P and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Wu, Y and Yamamoto, RK and Grard, F and Hanton, J and Henri, V and Herquet,
             P and Lesccux, JM and Pilette, P and Windmolders, R and Crijns, F and De
             Bock, H and Kittel, W and Metzger, W and Pols, C and Schouten, M and Van de
             Walle, R and Cohn, HO and Bressi, G and Calligarich, E and Castoldi, C and Dolfini, R and Di Marco and R and Jacques, PF and Kalelkar, M and Plano,
             RJ and Ratti, S and Stamer, PE and Watts, TL and Brucker, EB and Koller,
             EL and Taylor, S and Berny, L and Dado, S and Goldberg, J and Toaff, S and Alexander, G and Benary, O and Grunhaus, J and Heifetz, R and Levy, A and Bugg, WM and Condo, GT and Handler, T and Hart, EL and Rogers, AH and Eisenberg, Y and Hochman, D and Karshon, U and Ronat, EE and Shapira, A and Yaari, R and Yekutieli, G and Ludlam, T and Steiner, R and Taft,
             H},
   Title = {Hadron production in π+, K+p and pp
             collisions at 147 GeV/c and properties of jet-like
             multiparticle systems - International hybrid spectrometer
             consortium},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {15},
   Number = {1},
   Pages = {1-10},
   Publisher = {Springer Nature America, Inc},
   Year = {1982},
   Month = {January},
   url = {http://dx.doi.org/10.1007/BF01573420},
   Abstract = {The gross features of the data are reviewed and the momentum
             tensor components, 〈S〉, and 〈T〉 are studied.
             Evidence for coplanarity effects is observed. A
             probabilistic method to search for jets is proposed. The
             jets found by this method are seen to be similar to high pT
             jets from pp interactions e+e- annihilations and vp
             interactions. The effect of subtracting the leading
             particles and the effect of low pT diffractive and non
             diffractive components are investigated. © 1982
             Springer-Verlag.},
   Doi = {10.1007/BF01573420},
   Key = {fds309836}
}

@article{fds309837,
   Author = {Bugg, WM and Condo, GT and Handler, T and Hart, EL and Cohn, HO and Kitagaki, T and Tanaka, S and Yuta, H and Abe, K and Hasegawa, K and Yamaguchi, A and Nozaki, T and Tamai, K and Maruyama, T and Kikuchi, R and Unno, Y and Otani, Y and Barreiro, F and Benary, O and Brau, JE and Dolfini, R and Hafen, ES and Haridas, P and Hochman, D and Hodous, MF and Hulsizer, RI and Kistiakowsky, V and Napier, A and Noguchi, S and Oh,
             SH and Pless, IA and Silverman, JP and Trepagnier, PC and Wolfson, J and Wu, Y and Yamamoto, RK},
   Title = {Some g(1700) decay modes},
   Journal = {Physical Review D},
   Volume = {26},
   Number = {9},
   Pages = {2183-2189},
   Publisher = {American Physical Society (APS)},
   Year = {1982},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.26.2183},
   Abstract = {From a study of 8-GeV/c-p interactions, the various two-pion
             and four-pion decay channels available to the g- meson have
             been investigated. Our results indicate that the dominant 4
             decay modes involve intermediate and production without
             significant A2 formation. © 1982 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.26.2183},
   Key = {fds309837}
}

@article{fds309838,
   Author = {Kitagaki, T and Tanaka, S and Yuta, H and Abe, K and Hasegawa, K and Yamaguchi, A and Nozaki, T and Tamai, K and Maruyama, T and Kikuchi, R and Unno, Y and Otani, Y and Barreiro, F and Benary, O and Brau, JE and Dolfini, R and Hafen, ES and Haridas, P and Hochman, D and Hodous, MF and Hulsizer, RI and Kistiakowsky, V and Napier, A and Noguchi, S and Oh,
             SH and Pless, IA and Silverman, JP and Trepagnier, PC and Wolfson, J and Wu, Y and Yamamoto, RK and Cohn, HO and Bugg, WM and Condo, GT and Handler,
             T and Hart, EL},
   Title = {Elastic scattering and particle production in two-prong -p
             interactions at 8 GeV/c},
   Journal = {Physical Review D},
   Volume = {26},
   Number = {7},
   Pages = {1572-1587},
   Publisher = {American Physical Society (APS)},
   Year = {1982},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.26.1572},
   Abstract = {Results of a high-statistics study of elastic scattering and
             meson resonances produced by -p interactions at 8 GeV/c are
             presented. Large statistics and small systematic errors
             permit examination of the complete kinematic region. Total
             differential cross sections are given for 0,-, f0, g0, -, 0,
             and N* resonances. Spin-density matrix elements and
             Legendre-polynomial moments are given for f resonances. The
             results for 0 and f0 resonances are compared with the
             predictions of a Regge-pole-exchange model. Properties of
             the above resonances are compared and discussed. In
             particular, we present evidence that the 0 and f0 production
             mechanisms are similar. The similarity of the g0 t
             distribution to that of the 0 and f0 suggests a common
             production mechanism for all three resonances. © 1982 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.26.1572},
   Key = {fds309838}
}

@article{fds309839,
   Author = {Kitagaki, T and Tanaka, S and Yuta, H and Abe, K and Hasegawa, K and Yamaguchi, A and Nozaki, T and Tamai, K and Maruyama, T and Kikuchi, R and Unno, Y and Otani, Y and Barreiro, F and Benary, O and Brau, JE and Dolfini, R and Hafen, ES and Haridas, P and Hochman, D and Hodous, MF and Hulsizer, RI and Kistiakowsky, V and Napier, A and Noguchi, S and Oh,
             SH and Pless, IA and Silverman, JP and Trepagnier, PC and Wolfson, J and Wu, Y and Yamamoto, RK and Cohn, HO and Bugg, WM and Condo, GT and Handler,
             T and Hart, EL},
   Title = {Reaction p+-p at 8 GeV/c},
   Journal = {Physical Review D},
   Volume = {26},
   Number = {7},
   Pages = {1554-1571},
   Publisher = {American Physical Society (APS)},
   Year = {1982},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.26.1554},
   Abstract = {Results from a high-statistics experiment involving an
             exposure of the SLAC 82-in. hydrogen bubble chamber to a
             beam of 8-GeV/c yielding a final state of -p are presented.
             Copious production of f is found. Considerable
             quasi-two-body production in which one particle decays to
             one of the above resonances is also observed. Some
             double-resonance production involving baryon and meson
             resonances is also seen. The production properties of f
             mesons are well described by a double-Regge model. © 1982
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.26.1554},
   Key = {fds309839}
}

@article{fds309835,
   Author = {Brick, DH and Rudnicka, H and Shapiro, AM and Smith, W and Widgoff, M and Beillière, P and Lutz, P and Narjoux, JL and Gelfand, N and Alyea, ED and Bober, JT and Busza, W and Dolfini, R and Frank, TAJ and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RI and Kistiakowsky, V and Noguchi, S and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow,
             V and Tether, S and Trepagnier, PC and Wadsworth, BF and Wu, Y and Yamamoto, RK and Debock, H and Crijns, F and Schouten, M and Van de
             Walle, R and Dimarco, R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer, PE and Vogel, A and Brucker, EB and Koller, EL and Alexander, G and Grunhaus, J and Levy, A and Milstene, C and Bugg, WM and Condo, GT and Handler, T and Hargis, HJ and Hart, EL and Rafatian, A and Rogers, AH and Kitagaki, T and Tanaka, S and Yuta, H and Abe, K and Hasegawa, K and Yamaguchi, A and Tamai, K and Hayashino, Y and Otani, Y and Higuchi, M and Sato, M and Ludlam, T and Steiner, R and Taft, HD},
   Title = {Measurement of the multiplicities in the collision of
             hadrons with heavy nuclei at 200 GeV/c},
   Journal = {Nuclear Physics, Section B},
   Volume = {201},
   Number = {2},
   Pages = {189-196},
   Publisher = {Elsevier BV},
   Year = {1982},
   Month = {June},
   url = {http://dx.doi.org/10.1016/0550-3213(82)90428-X},
   Abstract = {We report on the interactions of an incident 200 GeV / c
             beam composed of 33% protons, 16% kaons, and 48% pions on
             targets of silver and gold mounted in the Fermilab 30″
             bubble chamber. Within our limited statistics, we find the
             total cross sections and average multiplicities to agree
             with previously published data. We find the KNO scaling
             distribution curve to be broader for heavy nuclei than for
             hydrogen. We present the first data for V0 production on
             gold and silver. We also present, for the first time,
             evidence for a positive charge excess among the sample of
             relativistic tracks from interactions on gold and silver. We
             observe a trend where the positive charge excess increases
             with target atomic number and with increasing charged
             particle multiplicity. We find the charge excess to exist
             among the sample of particles having greater than 2 GeV / c
             momentum and to persist in the sample with momentum greater
             than 4 GeV / c. © 1982.},
   Doi = {10.1016/0550-3213(82)90428-X},
   Key = {fds309835}
}

@article{fds309831,
   Author = {Brick, DH and Rudnicka, H and Shapiro, AM and Widgoff, M and Ansorge,
             RE and Neale, WW and Ward, DR and Whyman, BM and Burnstein, RA and Rubin,
             HA and Alyea, ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Dolfini, R and Frank, TAJ and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RI and Kistiakowsky, V and Lutz, P and Noguchi,
             S and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow, V and Tether,
             S and Trepagnier, PC and Wu, Y and Yamamoto, RK and Grard, F and Hanton, J and Henri, V and Herquet, P and Lesceux, JM and Pilette, P and Windmolders,
             R and de Bock, H and Crijns, F and Kittel, W and Metzger, W and Pols, C and Schouten, M and Van de Walle and R and Cohn, HO and Bressi, G and Calligarich, E and Castoldi, C and Ratti, S and DiMarco, R and Jacques,
             PF and Kalelkar, M and Plano, RJ and Stamer, PE and Watts, TL and Brucker,
             EB and Koller, EL and Taylor, S and Berny, L and Dado, S and Goldberg, J and Toaff, S and Alexander, G and Benary, O and Grunhaus, J and Heifetz, R and Levy, A and Bugg, WM and Condo, GT and Handler, T and Hart, EL and Rogers,
             AH and Eisenberg, Y and Hochman, D and Karshon, U and Ronat, EE and Shapira, A and Yaari, R and Yekutieli, G and Ludlam, TW and Steiner, RV and Taft, HD},
   Title = {The reactions pp→ppπ+π-,
             K+p→K++π-π,
             π+p→ π+,pπ+π-
             and π-p →π+π- at 147
             GeV/c},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {19},
   Number = {1},
   Pages = {1-9},
   Publisher = {Springer Nature},
   Year = {1983},
   Month = {March},
   url = {http://dx.doi.org/10.1007/BF01572330},
   Abstract = {We have studied the reactions pp→ppπ+π-,
             K+p→K+pπ+π-π, π+p→ π+,pπ+π- and π-p →π+π- at
             147 GeV/c using the 30-inch Fermilab hybrid system. All four
             reactions were detected with the same apparatus and analyzed
             in the same way. The energy dependence of the channel cross
             section was found to be Ap-0.6+B for the pp reaction and
             Ap-1+B for the other three. About 90% of the cross section
             at 147 GeV/c can be accounted for by either beam or target
             diffraction. Some of the remaining cross section may come
             from double Pomeron exchange reactions which we tried to
             isolate. We have tested the hypothesis of a factorizable
             Pomeron and our data indicates a violation of this
             hypothesis. We show that the 3π mass enhancement in the
             mass region 1.2-1.4 GeV is diffractively produced in the
             π± beam reactions. Fourprong, four-constraint and
             six-prong, four-constraint cross sections are reported. ©
             1983 Springer-Verlag.},
   Doi = {10.1007/BF01572330},
   Key = {fds309831}
}

@article{fds309829,
   Author = {Brick, D and Rudnicka, H and Shapiro, AM and Widgoff, M and Ansorge, RE and Neale, WW and Ward, DR and Whyman, BM and Burnstein, RA and Rubin, HA and Alyea, ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Frank, T and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RI and Kistiakowsky, V and Lutz, P and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Von Randow and M and Wu, Y and Yamamoto, RK and Grard, F and Hanton, J and Henri, V and Herquet, P and Lesceux, JM and Windmolders, R and DeBock,
             H and Crijns, F and Kittel, W and Metzger, W and Pols, C and Schouten, M and De Walle and RV and Cohn, HO and Carminati, F and Dolfini, R and Ratti, S and DiMarco, R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer, P and Watts, TL and Brucker, EB and Koller, EL and Taylor, S and Dado, S and Goldberg, J and Alexander, G and Benary, O and Grunhaus, J and Heifetz,
             R and Levy, A and Brau, JE and Bugg, WM and Condo, GT and Handler, T and Hart,
             EL and Rogers, AH and Eisenberg, Y and Karshon, U and Shapira, A and Ludlam, T and Steiner, R and Taft, H},
   Title = {Search for long-lived charge +2 hadrons},
   Journal = {Physical Review D},
   Volume = {30},
   Number = {5},
   Pages = {1134-1136},
   Publisher = {American Physical Society (APS)},
   Year = {1984},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.30.1134},
   Abstract = {We have searched for the production of long-lived R-Δ++
             hadrons, which contain a gluino in addition to three up
             quarks, in pp, π+p, and K+p interactions at 147 GeV/c. For
             R-Δ++'s of lifetime greater than 10-9 sec, and laboratory
             momentum greater than 2 GeV/c, we place 90%-confidence-level
             upper limits of 6.1 μ b in pp collisions, 4.4 μ b in π+p,
             and 29 μ b in K+p. © 1984 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.30.1134},
   Key = {fds309829}
}

@article{fds309830,
   Author = {Brick, DH and Rudnicka, H and Shapiro, AM and Widgoff, M and Ansorge,
             RE and Neale, WW and Ward, DR and Whyman, BM and Burnstein, KA and Rubin,
             HA and Alyea, ED and Bachman, L and Chien, CY and Lucas, P and Pevsner, A and Bober, JT and Frank, TAJ and Hafen, ES and Haridas, P and Huang, D and Hulsizer, RI and Kistiakowsky, V and Lutz, P and Oh, SH and Pless, IA and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Wu, Y and Yamamoto, RK and Grard, F and Hanton, J and Henri, V and Herquet,
             P and Lesceux, JM and Pilette, P and Windmolders, R and Crijns, F and De
             Bock, H and Kittel, W and Metzger, W and Pols, C and Schouten, M and Van de
             Walle, R and Cohn, HO and Carminati, F and Dolfini, R and Ratti, S and DiMarco, R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer, PE and Watts, TL and Brucker, EB and Koller, EL and Taylor, S and Berny, L and Dado, S and Goldberg, J and Toaff, S and Alexander, G and Benary, O and Grunhaus, J and Heifetz, R and Levy, A and Brau, JE and Bugg, WM and Condo,
             GT and Handler, T and Hart, EL and Rogers, AH and Eisenberg, Y and Karshon,
             U and Shapira, A and Ludlam, T and Steiner, R and Taft,
             H},
   Title = {Planar events produced in hadron-proton collisions at 147
             GeV/c and their jet-like structures},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {24},
   Number = {1},
   Pages = {19-29},
   Publisher = {Springer Nature},
   Year = {1984},
   Month = {January},
   url = {http://dx.doi.org/10.1007/BF01576283},
   Abstract = {An analysis is presented of the production of jets in
             low-ptπ±p, k+p, pp collisions at 147 GeV/c collected at
             Fermilab in the rapid cycling hydrogen bubble chamber hybrid
             spectrometer. It is shown that selected events are more
             planar than predicted by a cylindrical phase space, but that
             3-jet and 4-jet like structures seen in the momentum flows
             are reasonably reproduced by the cylindrical phase space
             events subjected to the same mathematical manipulation
             required to build momentum flows. © 1984
             Springer-Verlag.},
   Doi = {10.1007/BF01576283},
   Key = {fds309830}
}

@article{fds309828,
   Author = {Oh, SH and Cavendish, JC},
   Title = {MATHEMATICAL MODELING OF CATALYTIC CONVERTER LIGHTOFF. PART
             II: MODEL VERIFICATION BY ENGINE-DYNAMOMETER
             EXPERIMENTS.},
   Journal = {AIChE Journal},
   Volume = {31},
   Number = {6},
   Pages = {935-942},
   Year = {1985},
   Abstract = {A transient mathematical model has been developed which
             describes the behavior of packed-bed catalytic converters
             during warmup. Model predictions agree very well with the
             results of engine-dynamometer experiments for three
             Pt-alumina catalysts of widely different properties, thus
             demonstrating the validity of the model.},
   Key = {fds309828}
}

@article{fds309827,
   Author = {Goloskie, D and Kistiakowsky, V and Oh, S and Pless, IA and Stoughton,
             T and Suchorebrow, V and Wadsworth, B and Murphy, O and Steiner, R and Taft, HD},
   Title = {The performance of crisis and its calibration},
   Journal = {Nuclear Inst. and Methods in Physics Research,
             A},
   Volume = {238},
   Number = {1},
   Pages = {61-73},
   Publisher = {Elsevier BV},
   Year = {1985},
   Month = {July},
   url = {http://dx.doi.org/10.1016/0168-9002(85)91027-7},
   Abstract = {We describe the calibration of CRISIS, a charge sensitive
             drift chamber which makes possible the identification of
             charged particles with momentum between 5 and 100 GeV/c.
             Results indicate an optimum resolution of (7.1 ± 0.2)%
             fwhm, which is an improvement over the predicted value of
             7.8%. We characterize the efficiency for particle
             identification by the ratio b = (separation between π and
             p)/(σπ + σp. We achieve a value of (0.94 ± 0.02), which
             compares favorably with the theoretical value of 0.87 at 200
             GeV. In addition to particle identification, the data from
             this detector will augment the other components of the
             Fermilab hybrid spectrometer to reconstruct particle
             trajectories in real space. © 1985.},
   Doi = {10.1016/0168-9002(85)91027-7},
   Key = {fds309827}
}

@article{fds309826,
   Author = {Murphy, T and Chang, Z and Mao, CC and Tai, YS and Wang, S and Wu, YR and Xu,
             SW and Zhao, CZ and Goloskie, D and Harton, J and Oh, S and Pless, IA and Wadsworth, BF and Yamamoto, RK},
   Title = {Hadron showers in iron and muon identification},
   Journal = {Nuclear Inst. and Methods in Physics Research,
             A},
   Volume = {251},
   Number = {3},
   Pages = {478-492},
   Publisher = {Elsevier BV},
   Year = {1986},
   Month = {November},
   url = {http://dx.doi.org/10.1016/0168-9002(86)90642-X},
   Abstract = {We report on measurements of the punchthrough probability of
             high energy hadrons as a function of iron depth and hadron
             energy. These measurements were made in the Fermilab Meson
             Bottom test beam. The hadron momentum range was from 12 to
             200 GeV/c and the maximum iron depth explored was 250 cm.
             Hadron shower characteristics as a function of iron depth
             and hadron energy are shown and compared with other data.
             Characteristics of a proportional tube detector and the use
             of such a detector in a muon identification system are
             described. The muon identification efficiency is studied for
             several configurations. Each configuration differs in the
             thickness of the steel absorbers and their locations among
             chambers. © 1986.},
   Doi = {10.1016/0168-9002(86)90642-X},
   Key = {fds309826}
}

@article{fds309823,
   Author = {Chen, DKS and Bissett, EJ and Oh, SH and Ostrom, DLV},
   Title = {A three-dimensional model for the analysis of transient
             thermal and conversion characteristics of monolithic
             catalytic converters},
   Journal = {SAE Technical Papers},
   Year = {1988},
   url = {http://dx.doi.org/10.4271/880282},
   Abstract = {A transient three-dimensional model has been developed to
             simulate the thermal and conversion characteristics of
             nonadiabatic monolithic converters operating under flow
             maldistribution conditions. The model accounts for
             convective heat and mass transport, gas-solid heat and mass
             transfer, axial and radial heat conduction, chemical
             reactions and the attendant heat release, and heat loss to
             the surroundings. The model was used to analyze the
             transient response of an axisymmetric ceramic monolith
             system (catalyzed monolith, mat, and steel shell) during
             converter warm-up, sustained heavy load, and engine
             misfiring. The simulation indicates that high solid
             temperatures are encountered during sustained heavy load or
             engine misfiring, while steep temperature gradients are
             developed during the converter warm-up period. Flow
             maldistribution and radial heat loss are major sources for
             the thermal gradients. The predicted temperature profiles
             provide a basis for the analysis of thermal stresses and
             fatigue in the monolith converter assembly. Copyright ©1988
             Society of Automotive Engineers, Inc.},
   Doi = {10.4271/880282},
   Key = {fds309823}
}

@article{fds309824,
   Author = {Oh, SH},
   Title = {Thermal response of monolithic catalytic converters during
             sustained engine misfiring: A computational
             study},
   Journal = {SAE Technical Papers},
   Year = {1988},
   url = {http://dx.doi.org/10.4271/881591},
   Abstract = {The thermal response characteristics of automobile
             monolithic converters during sustained engine misfiring have
             been studied using a mathematical model which accounts for
             the simultaneous processes of heat transfer, mass transfer,
             and catalytic reaction. Particular attention was given to
             the effects of converter properties and inlet exhaust
             conditions on the location and magnitude of the temperature
             peak developed during the transient. Our simulation results
             show that the temperature excursions in typical monolith
             converters during engine misfiring are generally
             characterized by an ignition zone (where a steep exothermic
             temperature rise occurs as a result of rapid reaction)
             preceded by a relatively short, unreactive region near the
             inlet. Also, the predicted maximum wall temperature
             correlates well with the adiabatic reaction temperature, and
             the melting point of the monolith substrate would not be
             exceeded unless the extent of engine misfiring is 40% or
             higher. Copyright © 1988 Society of Automotive Engineers,
             Inc.},
   Doi = {10.4271/881591},
   Key = {fds309824}
}

@article{fds309825,
   Author = {Peden, CHF and Goodman, DW and Blair, DS and Berlowitz, PJ and Fisher,
             GB and Oh, SH},
   Title = {Kinetics of CO oxidation by O2 or NO on Rh(111)
             and Rh(100) single crystal},
   Journal = {Journal of Physical Chemistry},
   Volume = {92},
   Number = {6},
   Pages = {1563-1567},
   Year = {1988},
   Abstract = {The oxidation of CO by O2 or NO over Rh(111) and Rh(100)
             single crystals has been studied in a high-pressure
             reaction-high-vacuum surface analysis apparatus.
             Steady-state catalytic activity as a function of temperature
             and partial pressures of CO, O2, and NO has been measured.
             The CO-O2 reaction was found to be insensitive to the
             structure of the surface as evidenced by the identical
             rates, activation energies, and partial pressure
             dependencies measured on the two single-crystal surfaces.
             Both surfaces deactivated at high O2 partial pressures due
             to the formation of a near-surface oxide (probably Rh2O3)
             which is catalytically inactive for this reaction. The
             deactivation occurred at a slightly lower O2 partial
             pressure on Rh(100), likely due to the relative ease of
             oxygen diffusion through this surface leading to more rapid
             bulk oxidation. Unlike the CO-O2 reaction, CO oxidation by
             NO was very sensitive to the geometric structure of the
             surface. This behavior was evident in all kinetic parameters
             measured on the two surfaces. The kinetic data obtained on
             Rh(111) agree quantitatively with a surface chemistry model
             previously developed for this reaction. The model predicts
             that the rate is limited by the formation of N2 from the
             recombination of adsorbed N atoms, and that the surface,
             under steady-state reaction conditions, is covered largely
             with adsorbed N atoms and smaller amounts of adsorbed NO. On
             Rh(100) the data are consistent with a reaction rate limited
             by the formation of N2 from the surface reaction of adsorbed
             NO and N atoms. © 1988 American Chemical
             Society.},
   Key = {fds309825}
}

@article{fds309822,
   Author = {Abe, K and Alexander, G and Alyea, ED and Badiak, M and Beilliere, P and Bloomer, M and Bober, T and Brau, JE and Brick, DH and Brucker, EB and Bugg, WM and Busza, W and Castoldi, C and Cole, B and Cohn, HO and Condo,
             GT and Dimarco, R and Dolfini, R and Frank, TA and Fuess, TA and Galligarich, E and Gel'fand, N and Grodzins, L and Grunhaus, J and Hafen, ES and Handler, T and Hargis, HJ and Haridas, P and Hart, EL and Hasegawa, K and Hayashino, Y and Higuchi, M and Huang, D and Huang, HZ and Hulsizer, R and Introzzi, L and Jacques, PF and Kalelkar, M and Kistiakowsky, V and Kitagaki, T and Koller, EL and Ledoux, RJ and Levy,
             A and Ludlam, T and Lutz, P and Milstene, C and Narjoux, JL and Noguchi, S and Oh, SH and Otani, Y and Plano, RJ and Pless, IA and Ratti, S and Rafatian,
             A and Rogers, AH and Sato, M and Stamer, PE and Steadman, SG and Steiner,
             R and Stoughton, TB and Suchorebrow, V and Taft, B and Tamai, K and Tanaka,
             S and Tether, S and Trepagnier, PC and Wadsworth, BF and Widgoff, M and Wu,
             Y and Yamaguchi, A and Yamamoto, RK and Yuta, H},
   Title = {Leading particle distributions in 200 GeV/c p+A
             interactions},
   Journal = {Physics Letters B},
   Volume = {200},
   Number = {3},
   Pages = {266-271},
   Publisher = {Elsevier BV},
   Year = {1988},
   Month = {January},
   url = {http://dx.doi.org/10.1016/0370-2693(88)90769-1},
   Abstract = {Distributions of the leading positive particle have been
             measured in collisions of a 200 GeV/c proton beam with
             hydrogen, Mg, Ag and Au targets using the FNAL Hybrid
             Spectrometer. Estimates of the rapidity loss of the
             projectile have been obtained as a function of the target
             mass, the multiplicity of negative particles and the number
             of recoil protons. We obtained a lower limit of the rapidity
             loss of 2.0±0.2 for central p+Au collisions. The impact
             parameter dependence of the momenta of the first few leading
             particles has also been investigated with important
             implications to estimates of energy densities obtained in
             central collisions. © 1988.},
   Doi = {10.1016/0370-2693(88)90769-1},
   Key = {fds309822}
}

@article{fds309821,
   Author = {Alexopoulos, T and Allen, C and Anderson, EW and Areti, H and Banerjee,
             S and Beery, PD and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Cole, P and Choi, Y and Debonte, R and Erwin, A and Findeisen, C and Goshaw, AT and Gutay, LJ},
   Title = {Multiplicity dependence of the transverse-momentum spectrum
             for centrally produced hadrons in antiproton-proton
             collisions at square-root-s=1.8 tev},
   Journal = {Physical Review Letters},
   Volume = {60},
   Number = {16},
   Pages = {1622-1625},
   Year = {1988},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.60.1622},
   Doi = {10.1103/physrevlett.60.1622},
   Key = {fds309821}
}

@article{fds309819,
   Author = {Banerjee, S and Beery, PD and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Choi, Y and Findeisen, C and Goshaw, AT and Hojvat, C and Lindsey, CS and Losecco, JM and McManus, AP and Morgan, N and Nelson, K and Oh, SH and Piekarz, J and Reeves, D and Stampke, SR and Thompson, M and Turkot, F and Walker, WD and Wang, CH and Wesson,
             DK},
   Title = {0 and »0 Production from Proton-Antiproton Collisions at
             s=1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {62},
   Number = {1},
   Pages = {12-15},
   Year = {1989},
   url = {http://dx.doi.org/10.1103/PhysRevLett.62.12},
   Abstract = {The transverse-momentum spectra of lambdas (0, »0) produced
             in the central region has been measured in p»p collisions
             at s=1.8 TeV at the Fermilab Collider. We find that the
             average transverse momentum of the lambdas increases more
             rapidly with center-of-mass energy than that of charged
             particles, and the ratio of lambdas to charged particles
             increases as a function of center-of-mass energy. © 1988
             The American Physical Society.},
   Doi = {10.1103/PhysRevLett.62.12},
   Key = {fds309819}
}

@article{fds309818,
   Author = {Alexopoulos, T and Allen, C and Anderson, EW and Areti, H and Banerjee,
             S and Beery, PD and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Cole, P and Choi, Y and DeBonte, R and Erwin, A and Findeisen, C and Goshaw, AT and Gutay, LJ and Hirsch, AS and Hojvat, C and Kenney, VP and Koltick, D and Lindsey, CS and LoSecco, JM and McMahon, T and McManus,
             AP and Morgan, N and Nelson, K and Oh, SH and Piekarz, J and Porile, NT and Reeves, D and Scharenberg, RP and Stampke, SR and Stringfellow, BC and Thompsons, M and Turkot, F and Walker, WD and Wang, CH and Wesson,
             DK},
   Title = {Recent results from E-735 at the Fermilab Tevatron
             proton-antiproton collider with √s = 1.8TeV},
   Journal = {Nuclear Physics, Section A},
   Volume = {498},
   Number = {C},
   Pages = {181-192},
   Publisher = {Elsevier BV},
   Year = {1989},
   Month = {January},
   url = {http://dx.doi.org/10.1016/0375-9474(89)90598-8},
   Abstract = {E-735 is searching for signs of the quark-gluon-plasma phase
             transition in minimum bias proton-antiproton events. Results
             from the 1987 run at the Tevatron Collider at √s = 1.8TeV
             are presented. Included are distributions of the average Pt
             versus multiplicity dependence for charged particles, and
             preliminary particle identification analysis using time of
             flight. © 1989.},
   Doi = {10.1016/0375-9474(89)90598-8},
   Key = {fds309818}
}

@article{fds309820,
   Author = {Brick, DH and Widgoff, M and Beilliere, P and Lutz, P and Narjoux, JL and Gelfand, N and Alyea, ED and Bloomer, M and Bober, J and Busza, W and Cole,
             B and Frank, TA and Fuess, TA and Grodzins, L and Hafen, ES and Haridas, P and Huang, D and Huang, HZ and Hulsizer, R and Kistiakowsky, V and Ledoux,
             RJ and Milstene, C and Noguchi, S and Oh, SH and Pless, IA and Steadman, S and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Wadsworth, BF and Wu, Y and Yamamoto, RK and Cohn, HO and Calligarich,
             E and Castoldi, C and Dolfini, R and Introzzi, L and Ratti, S and Badiak,
             M and Dimarco, R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer,
             PE and Brucker, EB and Koller, EL and Alexander, G and Grunhaus, J and Levy, A and Brau, JE and Bugg, WM and Condo, GT and Handler, T and Hargis,
             HJ and Hart, EL and Rafatian, A and Rogers, AH and Kitagaki, T and Tanaka,
             S and Yuta, H and Abe, K and Hasegawa, K and Yamaguchi, A and Tamai, K and Hayaschino, Y and Otani, Y and Higuchi, M and Sato, M and Ludlam, T and Steiner, R and Taft, H},
   Title = {Multiparticle production by 200-GeV/c hadrons on gold,
             silver, and magnesium targets},
   Journal = {Physical Review D},
   Volume = {39},
   Number = {9},
   Pages = {2484-2493},
   Publisher = {American Physical Society (APS)},
   Year = {1989},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.39.2484},
   Abstract = {We have used the Fermilab 30-in. bubble-chamber hybrid
             spectrometer to study multiparticle production in the
             interactions of 200-GeV/c protons and + and K+ mesons with
             nuclei of gold, silver, and magnesium. We find that the
             multiplicities of produced particles and negative particles
             increase linearly with the number of projectile collisions,
             with no beam or target dependence. The number of secondary
             collisions in the nucleus increases significantly less
             rapidly with the number of projectile collisions than has
             been reported by a streamer chamber experiment. The
             properties of secondary collisions suggest that they arise
             from rescattering of recoil nucleons rather than
             intranuclear cascade of produced particles. Dispersions of
             multiplicity distributions at fixed impact parameter are in
             better agreement with a model of independent sources than
             with Koba-Nielsen-Olesen scaling. © 1989 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.39.2484},
   Key = {fds309820}
}

@article{fds358019,
   Author = {Carter, T and Goshaw, AT and Oh, SH and Walker, WD and Wesson, DK and Areti, H and Hojvat, C and Reeves, D and Turkot, F and Anderson, EW and Lindsey, CS and Wang, CH and Banerjee, S and Beery, PD and Biswas, NN and Kenney, VP and LoSecco, JM and McManus, AP and Piekarz, J and Stampke,
             SR and Allen, C and Bujak, A and Carmony, DD and Cole, P and Choi, Y and Bonte, RD and Gutay, LJ and Hirsch, AS and McMahon, T and Morgan, N and Porile, NT and Scharenberg, RP and Stringfellow, BC and Alexopoulos,
             T and Erwin, A and Findeisen, C and Nelson, K and Thompson,
             M},
   Title = {Deconfinement Signature, Mass Dependence of Transverse Flow
             and Time Evolution in Antiproton-Proton Collisions at s =
             1.8 TeV},
   Journal = {Physica Scripta},
   Volume = {1990},
   Number = {T32},
   Pages = {122-125},
   Year = {1990},
   Month = {January},
   url = {http://dx.doi.org/10.1088/0031-8949/1990/T32/018},
   Abstract = {The yields and the transverse momentum distributions of
             pions, kaons, and antiprotons produced in the central region
             of pp collisions at surd;;s = 1.8 TeV at the Fermilab
             Tevatron collider have been measured up to a charged
             particle pseudo-rapidity density of approximately 20. The
             average transverse momentum 〈pt〉 as a function of
             〈dNc/dη〉 for all three types of particles is presented.
             We find that transverse flow does not explain the 〈pt〉
             separation. The most plausible interpretation is that the
             〈pt〉 vs. Nc spectra represent in isobar in the two phase
             region. © 1990 IOP Publishing Ltd.},
   Doi = {10.1088/0031-8949/1990/T32/018},
   Key = {fds358019}
}

@article{fds309816,
   Author = {Alexopoulos, T and Allen, C and Anderson, EW and Areti, H and Banerjee,
             S and Bhat, P and Bishop, J and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Cole, P and Choi, Y and Debonte, R and Erwin, A and Findeisen, C and Goshaw, AT and Gutay, LJ and Hirsch, AS and Hojvat, C and Kenney, VP and Koltick, D and Lindsey, CS and Loomis, C and Losecco, JM and McMahon, T and McManus, AP and Morgan, NK and Nelson, K and Oh, SH and Piekarz, J and Porile, NT and Reeves, D and Robertson, WR and Scharenberg, RP and Stampke, SR and Stringfellow, BC and Thompson, M and Turkot, F and Walker, WD and Wang, CH and Wesson, DK and Zuong,
             H},
   Title = {Recent results from E-735 at the Fermilab tevatron
             proton-antiproton collider at √S = 1.8
             TeV},
   Journal = {Nuclear Physics B (Proceedings Supplements)},
   Volume = {12},
   Number = {C},
   Pages = {267-276},
   Publisher = {Elsevier BV},
   Year = {1990},
   Month = {January},
   url = {http://dx.doi.org/10.1016/0920-5632(90)90196-2},
   Abstract = {E-735 is designed to study charged particle production in
             the central region of rapidity in proton-antiproton
             collisions at √s = 1.8 TeV. Variations in transverse
             momentum and particle production ratios versus particle
             density are measured as a possible signature for a
             quack-gluon-plasma (QGP) phase transition. Preliminary
             results from the 1987 run are presented. ©
             1990.},
   Doi = {10.1016/0920-5632(90)90196-2},
   Key = {fds309816}
}

@article{fds309817,
   Author = {Brick, DH and Widgoff, M and Beilliere, P and Lutz, P and Narjoux, JL and Gelfand, N and Alyea, ED and Bloomer, M and Bober, J and Busza, W and Cole,
             B and Frank, TA and Fuess, TA and Grodzins, L and Hafen, ES and Haridas, P and Huang, D and Huang, HZ and Hulsizer, R and Kistiakowsky, V and Ledoux,
             RJ and Milstene, C and Noguchi, S and Oh, SH and Pless, IA and Steadman, S and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Wadsworth, BF and Wu, Y and Yamamoto, RK and Cohn, HO and Calligarich,
             E and Castoldi, C and Dolfini, R and Introzzi, G and Ratti, S and Badiak,
             M and Dimarco, R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer,
             PE and Brucker, EB and Koller, EL and Alexander, G and Grunhaus, J and Levy, A and Brau, JE and Bugg, WM and Condo, GT and Handler, T and Hargis,
             HJ and Hart, EL and Rafatian, A and Rogers, AH and Kitagaki, T and Tanaka,
             S and Yuta, H and Abe, K and Hasegawa, K and Yamaguchi, A and Tamai, K and Hayaschino, Y and Otani, Y and Higuchi, M and Sato, M and Ludlam, T and Steiner, R and Taft, H},
   Title = {Rapidities of produced particles in 200-GeV/c +/p/K+
             interactions on Au, Ag, and Mg},
   Journal = {Physical Review D},
   Volume = {41},
   Number = {3},
   Pages = {765-773},
   Publisher = {American Physical Society (APS)},
   Year = {1990},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.41.765},
   Abstract = {We have used the Fermilab 30-in. bubble chamberhybrid
             spectrometer to study the rapidities of produced particles
             in the interactions of 200-GeV/c protons and + and K+ mesons
             with nuclei of gold, silver, and magnesium. The average
             rapidity decreases linearly with the number of projectile
             collisions p (up to p=5) with no A dependence and little
             beam dependence. The ratio R of normalized rapidity
             distributions for hadron-nucleus to hadron-proton
             interactions shows a plateau in the central region, and
             becomes much larger in the target region. However, the
             increase is significantly less than has been reported in
             previous experiments. As a function of p, the ratio R rises
             linearly in the target region, more gently in the central
             region, and decreases slowly in the projectile region, in
             all cases with no A dependence. Some discrepancies with a
             previous experiment are observed in the central region.
             Long-range rapidity correlations are observed in
             hadron-nucleus events, but not in hadron-proton events. For
             the former, it is shown that the correlations exist only for
             those events with multiple projectile collisions, as
             expected in the multichain dual parton model. © 1990 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.41.765},
   Key = {fds309817}
}

@article{fds309815,
   Author = {Alexopoulos, T and Allen, C and Anderson, EW and Areti, H and Banerjee,
             S and Beery, PD and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Cole, P and Choi, Y and Debonte, RJ and Erwin, AR and Findeisen, C and Goshaw, AT and J, L},
   Title = {Mass-identified particle yields in antiproton-proton
             collisions at square-root-s=1.8 tev},
   Journal = {Physical Review Letters},
   Volume = {64},
   Number = {9},
   Pages = {991-994},
   Year = {1990},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.64.991},
   Doi = {10.1103/physrevlett.64.991},
   Key = {fds309815}
}

@article{fds309814,
   Author = {Turkot, F and Alexopoulos, T and Allen, C and Anderson, EW and Areti, H and Banerjee, S and Beery, PD and Bhat, P and Bishop, J and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Cole, P and Choi, Y and DeBonte,
             R and DeCarlo, V and Erwin, AR and Findeisen, C and Goshaw, AT and Gutay,
             LJ and Hirsch, AS and Hojvat, C and Kenney, VP and Koltick, D and Lindsey,
             CS and Loomis, C and LoSecco, JM and McMahon, T and McManus, AP and Morgan,
             NK and Nelson, K and Oh, SH and Piekarz, J and Porile, NT and Reeves, D and Robertson, WR and Scharenberg, RP and Stampke, SR and Stringfellow,
             BC and Thompson, MA and Walker, WD and Wang, CH and Wesson, DK and Zuong,
             H},
   Title = {A quark-gluon plasma search in p̄-p at s = 1.8
             TeV},
   Journal = {Nuclear Physics, Section A},
   Volume = {525},
   Number = {C},
   Pages = {165-170},
   Publisher = {Elsevier BV},
   Year = {1991},
   Month = {January},
   url = {http://dx.doi.org/10.1016/0375-9474(91)90323-X},
   Abstract = {We present a survey of the recent results of E-735 in its
             search for QGP signals at the Fermilab Collider. The basic
             data are the inclusive Pt distributions of centrally
             produced π, K, p̄ and Λ0 as a function of total charged
             multiplicity in the collision; the variation of 〈Pt〉 and
             particle ratios are derived. Preliminary results on π-π
             correlations and inclusive photon production are also
             presented. © 1991.},
   Doi = {10.1016/0375-9474(91)90323-X},
   Key = {fds309814}
}

@article{fds309813,
   Author = {Oh, SH and Wesson, DK and Cooke, J and Goshaw, AT and Robertson, WJ and Walker, WD},
   Title = {Design and performance of a straw tube drift
             chamber},
   Journal = {Nuclear Inst. and Methods in Physics Research,
             A},
   Volume = {303},
   Number = {2},
   Pages = {277-284},
   Publisher = {Elsevier BV},
   Year = {1991},
   Month = {June},
   url = {http://dx.doi.org/10.1016/0168-9002(91)90794-Q},
   Abstract = {The design and performance of the straw drift chambers used
             in E735 is reported. The chambers are constructed from 2.5
             cm radius aluminized mylar straw tubes with wall thickness
             less than 0.2 mm. Also, presented are the results of tests
             with 2 mm radius straw tubes. The small tube has a direct
             detector application at the Superconducting Super Collider.
             © 1991.},
   Doi = {10.1016/0168-9002(91)90794-Q},
   Key = {fds309813}
}

@article{fds309812,
   Author = {Oh, SH and Goshaw, AT and Robertson, WJ},
   Title = {Construction and performance of a 2.7 m long straw drift
             tube prototype chamber for the SSC},
   Journal = {Nuclear Inst. and Methods in Physics Research,
             A},
   Volume = {309},
   Number = {3},
   Pages = {368-376},
   Publisher = {Elsevier BV},
   Year = {1991},
   Month = {November},
   url = {http://dx.doi.org/10.1016/0168-9002(91)90240-Q},
   Abstract = {We report the construction and testing of a 2.7 m long straw
             tube drift chamber consisting of 60 channels. The straw
             tubes with 2 mm radius are stacked in a pyramid shape up to
             eight tube layers. There are two wire supports inside each
             tube for electrostatic stability. 28 tubes out of 60 are
             instrumented for measurement of resolution, gas gain, and
             attenuation length. Resolution of close to 110 μm and
             attenuation length of 500 cm are obtained. ©
             1991.},
   Doi = {10.1016/0168-9002(91)90240-Q},
   Key = {fds309812}
}

@article{fds309809,
   Author = {Alexopoulos, T and Allen, C and Anderson, EW and Areti, H and Banerjee,
             S and Beery, PD and Bhat, P and Bishop, J and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Cole, P and Choi, Y and Debonte, R and DeCarlo, V and Erwin, AR and Findeisen, C and Goshaw, AT and Gutay, LJ and Hirsch, AS and Hojvat, C and Jennings, JR and Kenney, VP and Lindsey,
             CS and Loomis, C and LoSecco, JM and McMahon, T and McManus, AP and Morgan,
             NK and Nelson, K and Oh, SH and Piekarz, J and Porile, NT and Reeves, D and Rimai, A and Robertson, WR and Scharenberg, RP and Stample, SR and Stringfellow, BC and Thompson, MA and Turkot, F and Walker, WD and Wang,
             CH and Wesson, DK and Zuong, H},
   Title = {Average transverse momentum vs. dNc dη for
             mass-identified particles at tevatron energies},
   Journal = {Nuclear Physics B (Proceedings Supplements)},
   Volume = {25},
   Number = {C},
   Pages = {40-47},
   Publisher = {Elsevier BV},
   Year = {1992},
   Month = {January},
   url = {http://dx.doi.org/10.1016/0920-5632(92)90373-Z},
   Abstract = {The transverse momentum of charged mesons and p's produced
             within the pseudorapidity range of η = -0.36 to η = +1.0
             and azimuthal range of φ = +2° to φ = +18° has been
             measured in pp collisions at √s = 1.8 TeV. The charged
             multiplicity of each event was measured by either the 240
             element cylindrical hodoscope covering the range -3.25 < η
             < +3.25 or the central drift chamber, which spans a
             pseudorapidity range of 3.2 units. The average transverse
             momentum as a function of the pseudorapidity density for
             mass-identified particles is presented. We have observed
             pseudorapidity densities as high as 30 particles per unit
             pseudorapidity. © 1992.},
   Doi = {10.1016/0920-5632(92)90373-Z},
   Key = {fds309809}
}

@article{fds309810,
   Author = {Brick, DH and Widgoff, M and Beilliere, P and Lutz, P and Narjoux, JL and Gelfand, N and Alyea, ED and Bloomer, M and Bober, J and Busza, W and Cole,
             B and Frank, TA and Fuess, TA and Grodzins, L and Hafen, ES and Haridas, P and Huang, D and Huang, HZ and Hulsizer, R and Kistiakowsky, V and Ledoux,
             RJ and Milstene, C and Noguchi, S and Oh, SH and Pless, IA and Steadman, S and Stoughton, TB and Suchorebrow, V and Tether, S and Trepagnier, PC and Wadsworth, BF and Wu, Y and Yamamoto, RK and Cohn, HO and Calligarich,
             E and Corti, G and Dolfini, R and Gianini, G and Introzzi, G and Ratti, S and Badiak, M and Dimarco, R and Jacques, PF and Kalelkar, M and Plano, RJ and Stamer, PE and Brucker, EB and Koller, EL and Alexander, G and Grunhaus,
             J and Levy, A and Brau, JE and Bugg, WM and Condo, GT and Handler, T and Hargis, HJ and Hart, EL and Rafatian, A and Rogers, AH and Kitagaki, T and Tanaka, S and Yuta, H and Abe, K and Hasegawa, K and Yamaguchi, A and Tamai, K and Hayaschino, Y and Otani, Y and Higuchi, M and Sato, M and Ludlam, T and Steiner, R and Taft, H},
   Title = {Neutral-strange-particle production in 200-Gev/c p+K+
             interactions on Au, Ag, and Mg},
   Journal = {Physical Review D},
   Volume = {45},
   Number = {3},
   Pages = {734-742},
   Publisher = {American Physical Society (APS)},
   Year = {1992},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.45.734},
   Abstract = {We have used the Fermilab 30-in. bubble-chamber-hybrid
             spectrometer to study neutral-strange-particle production in
             the interactions of 200-GeV/c protons and + and K+ mesons
             with nuclei of gold, silver, and magnesium. Average
             multiplicities and inclusive cross sections for K0 and are
             measured, and a power law is found to give a good
             description of their A dependence. The exponent
             characterizing the A dependence is consistent with being the
             same for K0 and production, and also the same for proton and
             + beams. Average K0 and multiplicities, as well as their
             ratio, have been measured as functions of the numbers of
             projectile collisions p and secondary collisions s in the
             nucleus, and indicate that rescattering contributes
             significantly to enhancement of production but not to K0
             production. The properties of events with multiple K0's or
             also corroborate this conclusion. K0 rapidities are in the
             central region and decrease gently with increasing p, while
             rapidities are in the target-fragmentation region and are
             independent of p. K0 and multiplicities increase with the
             rapidity loss of the projectile, but their rapidities do
             not. © 1992 The American Physical Society.},
   Doi = {10.1103/PhysRevD.45.734},
   Key = {fds309810}
}

@article{fds309811,
   Author = {al, CSLE},
   Title = {Results from e735 at the tevatron proton-antiproton collider
             with root-s=1.8 tev},
   Journal = {Nucl. Phys. A},
   Volume = {544},
   Number = {1-2},
   Pages = {C343-C356},
   Publisher = {Elsevier BV},
   Year = {1992},
   Month = {July},
   url = {http://dx.doi.org/10.1016/0375-9474(92)90585-8},
   Abstract = {Experiment E735 searched for evidence of the transition to
             quark-gluon plasma in pp collisions at √s = 1.8 TeV. Using
             data from a high statistics run in 1988-1989, results are
             presented on multiplicity distributions, hyperon and phi
             production, and Bose-Einstein correlations. Some data were
             also taken at lower collision energies and results will be
             compared to previous experiments. © 1992.},
   Doi = {10.1016/0375-9474(92)90585-8},
   Key = {fds309811}
}

@article{fds309808,
   Author = {al, TAE},
   Title = {Hyperon production from proton-antiproton collisions at
             root-s = 1.8 tev},
   Journal = {Phys. Rev. D},
   Volume = {46},
   Number = {7},
   Pages = {2773-2786},
   Year = {1992},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevd.46.2773},
   Doi = {10.1103/physrevd.46.2773},
   Key = {fds309808}
}

@article{fds309805,
   Author = {Oh, SH and Bissett, EJ},
   Title = {Mathematical modeling of monolith warmup behavior in
             variable-fuel vehicle exhaust},
   Journal = {SAE Technical Papers},
   Year = {1993},
   url = {http://dx.doi.org/10.4271/932721},
   Abstract = {The transient, one-dimensional monolith model previously
             developed for gasoline emission control applications has
             been extended to study converter warmup behavior in the
             exhaust from a variable-fuel vehicle (VFV) running on
             mixtures of methanol and gasoline by including the catalytic
             oxidation of methanol which involves the formation of stable
             gaseous formaldehyde as a reaction intermediate. The model
             calculations show that the aldehyde formation increases
             gradually at the early stages of converter lightoff (when
             methanol conversions are low), peaks at ∼50% methanol
             conversion, and then declines rapidly with a further
             increase in methanol conversion. Consequently, for all cases
             of practical interest, the total amount of aldehyde produced
             during the converter warmup period correlates well with the
             time to converter lightoff, with lower aldehyde emissions
             predicted at faster converter lightoff. In recent years
             methanol has received considerable attention as an
             alternative fuel for motor vehicles largely because of its
             potential for improving air quality in certain areas of the
             country [1, 2]. Conversion from gasoline to methanol would
             replace a large portion of the reactive hydrocarbons (HC) in
             gasoline exhaust with less reactive methanol, and thus can
             lower the ozone-forming potential of the exhaust. However,
             methanol-fueled vehicle exhaust also contains significant
             amounts of photochemically reactive aldehydes (primarily
             formaldehyde). Previous studies [2, 3 and 4] have clearly
             shown that maximum air quality benefit from methanol fuel
             can be obtained provided that exhaust emissions of
             formaldehyde are kept to very low levels. The California Air
             Resources Board has recently enacted a 15 mg/mile
             formaldehyde emission standard for methanol-fueled vehicles,
             and the requirement that this standard be met for at least 5
             years or 50,000 miles of vehicle use presents a challenging
             emission control problem. Given the prospect that methanol
             would not be uniformly available among service stations
             during the transition period, General Motors has developed
             and produced variable-fuel vehicles (VFVs) that can operate
             on mixtures of gasoline and methanol. This will allow the
             customer the flexibility to select either fuel based on
             price and availability. Variable-fuel vehicle exhaust
             contains a broad range of hydrocarbon species as well as
             unburned methanol and formaldehyde. Catalytic control of
             exhaust emissions from VFVs poses an interesting problem
             because many catalysts have been shown to exhibit tendencies
             to partially oxidize unburned methanol to formaldehyde at
             temperatures typically encountered during the converter
             warmup period [5, 6]. Thus, the ideal exhaust catalyst for
             VFVs must possess both high activity and high selectivity
             for the complete oxidation of methanol, in addition to the
             usual requirements related to the control of
             gasoline-derived exhaust pollutants. This study was
             undertaken to mathematically analyze the emission
             performance characteristics of a monolithic catalytic
             converter operating in the exhaust environment of VFVs. We
             focus on the converter warmup period because the first few
             minutes after a cold start contribute up to 80% of the total
             exhaust emissions of HC, methanol, and formaldehyde
             collected over the FTP cycle [7]. Since formaldehyde
             emissions are of particular concern with VFVs, the primary
             objective here is to identify important factors affecting
             formaldehyde emission levels and to gain insight into the
             mode of formaldehyde production over the catalyst during
             converter warmup. To this end, it is instructive to consider
             the simplest of transient inputs - a cold converter
             subjected to a step change in inlet exhaust gas conditions.
             Such approximation, though an idealization of reality,
             captures the essential features of the converter warmup
             process and affords better understanding of the relationship
             between converter design/operating parameters and its
             cold-start emission performance. It is hoped that the
             understanding generated from this simulation study would aid
             in the development of monolithic converters which
             efficiently and selectively oxidize exhaust pollutants
             produced by VFVs. © Copyright 1993 Society of Automotive
             engineers, Inc.},
   Doi = {10.4271/932721},
   Key = {fds309805}
}

@article{fds309806,
   Author = {Oh, SH and Sinkevitch, RM},
   Title = {Carbon Monoxide Removal from Hydrogen-Rich Fuel Cell
             Feedstreams by Selective Catalytic Oxidation},
   Journal = {Journal of Catalysis},
   Volume = {142},
   Number = {1},
   Pages = {254-262},
   Publisher = {Elsevier BV},
   Year = {1993},
   url = {http://dx.doi.org/10.1006/jcat.1993.1205},
   Abstract = {Indirect methanol fuel cells currently being investigated at
             General Motors for transportation applications require
             removal of carbon monoxide from the hydrogen-rich gas stream
             produced by the fuel processing section. A variety of
             catalytic materials, including noble metals (Pt, Pd, Rh, and
             Ru) and base metals (Co/Cu, Ni/Co/Fe, Ag, Cr, Fe, and Mn),
             were evaluated in a laboratory reactor feedstream containing
             CO, H2, and O2 in order to identify alternate catalysts
             which are more effective than currently used Pt/Al2O3 in
             selectively oxidizing CO in the presence of excess H2. Both
             Ru/Al2O3 and Rh/Al2O3 are among the most active catalysts
             for CO oxidation, achieving nearly complete CO conversion at
             temperatures as low as l00°C (compared to ∼200°C
             required for currently used Pt/Al2O3. Furthermore, the
             Ru/Al2O3 and Rh/Al2O3 catalysts were found to be
             exceptionally selective for CO oxidation, making it possible
             to purify the fuel cell feedstream with a minimum loss of
             the energy content associated with H2. © 1993 Academic
             Press. All rights reserved.},
   Doi = {10.1006/jcat.1993.1205},
   Key = {fds309806}
}

@article{fds309807,
   Author = {Oh, SH and Wang, C and Yin, M},
   Title = {A technique to measure the positions of sense wires in low
             mass drift chambers},
   Journal = {Nuclear Inst. and Methods in Physics Research,
             A},
   Volume = {325},
   Number = {1-2},
   Pages = {142-146},
   Publisher = {Elsevier BV},
   Year = {1993},
   Month = {February},
   url = {http://dx.doi.org/10.1016/0168-9002(93)91014-E},
   Abstract = {In this paper we report on a technique to measure the
             positions of sense wires in low mass drift chambers using
             electrons from a collimated 90Sr source. With this technique
             a sense wire position can be determined to an accuracy of
             less than 50 μm. © 1993.},
   Doi = {10.1016/0168-9002(93)91014-E},
   Key = {fds309807}
}

@article{fds309804,
   Author = {al, TAE},
   Title = {Mass-identified particle-production in proton-antiproton
             collisions at root-s = 300, 540, 1000, and 1800
             gev},
   Journal = {Phys. Rev. D},
   Volume = {48},
   Number = {3},
   Pages = {984-997},
   Year = {1993},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevd.48.984},
   Doi = {10.1103/physrevd.48.984},
   Key = {fds309804}
}

@article{fds309802,
   Author = {al, TAE},
   Title = {Inclusive photon production from p(p)over-bar collisions at
             root-s = 1.8 tev},
   Journal = {Phys. Rev. Lett.},
   Volume = {71},
   Number = {10},
   Pages = {1490-1493},
   Year = {1993},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.71.1490},
   Doi = {10.1103/physrevlett.71.1490},
   Key = {fds309802}
}

@article{fds309803,
   Author = {al, TAE},
   Title = {Study of source size in p-(p)over-bar collisions at root-s =
             1.8 tev using pion interferometry},
   Journal = {Phys. Rev. D},
   Volume = {48},
   Number = {5},
   Pages = {1931-1942},
   Year = {1993},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevd.48.1931},
   Doi = {10.1103/physrevd.48.1931},
   Key = {fds309803}
}

@article{fds309794,
   Author = {Abe, F and Albrow, M and Amidei, D and Anway-Wiese, C and Apollinari, G and Areti, H and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and al, E},
   Title = {Measurement of the ratio σB(W→eν)σB(Z0→e+e-) in p̄p
             collisions at s=1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {73},
   Number = {2},
   Pages = {220-224},
   Year = {1994},
   ISSN = {0031-9007},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:A1994NW18400002&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We present a measurement of the ratio σB(W→eν)σB(Z0→e+e-)
             in p̄p collisions at s=1.8 TeV The data represent an
             integrated luminosity of 21.7 pb-1 from the 1992-1993 run of
             the Collider Detector at Fermilab. We find
             σB(W→eν)σB(Z0→e+e-)=10.90±0.32(stat)±0. 29(syst).
             From this value, we extract a value for the W width,
             Γ(W)=2.064±0.061(stat)±0.059(syst) GeV, and the branching
             ratio, Γ(W→eν)Γ(W)=0.1094±0.0033(stat)±0.0031(syst),
             and we set a decay-mode-independent limit on the top quark
             mass mtop&gt;62 GeV/c2 at the 95% C.L. © 1994 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.73.220},
   Key = {fds309794}
}

@article{fds309799,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and al, E},
   Title = {W Boson + Jet Angular distribution in pp̄ collsions at
             s=1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {73},
   Number = {17},
   Pages = {2296-2300},
   Year = {1994},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.73.2296},
   Abstract = {The W+jet angular distribution is measured using W→eν
             events recorded with the Collider Detector at Fermilab (CDF)
             during the 1988-89 and 1992-93 Tevatron runs. The data agree
             well with both a leading order and a next-to-leading order
             theoretical prediction. The shape of the angular
             distribution is similar to that observed in photon + jet
             data and significantly different from that observed in dijet
             data. © 1994 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.73.2296},
   Key = {fds309799}
}

@article{fds309801,
   Author = {al, NTPE},
   Title = {Recent results from e735 - search for quark-gluon plasma in
             p-(p)over-bar collisions at 0.3-1.8 tev},
   Journal = {Nucl. Phys. A},
   Volume = {566},
   Number = {C},
   Pages = {C431-C434},
   Publisher = {Elsevier BV},
   Year = {1994},
   Month = {January},
   url = {http://dx.doi.org/10.1016/0375-9474(94)90662-9},
   Abstract = {Preliminary results on photon production and
             forward-backward multiplicity correlations in pp collisions
             at √s = 1.8 TeV are presented. Some additional results
             obtained at lower energies are also shown. ©
             1994.},
   Doi = {10.1016/0375-9474(94)90662-9},
   Key = {fds309801}
}

@article{fds309795,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Auchincloss, P and Austern, M and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bolognesi, V and Bortoletto, D and Boswell,
             C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman, J and Cheng, M},
   Title = {Evidence for top quark production in p-barp collisions at
             sqrt s =1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {73},
   Number = {2},
   Pages = {225-231},
   Publisher = {American Physical Society (APS)},
   Year = {1994},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.73.225},
   Abstract = {We summarize a search for the top quark with the Collider
             Detector at Fermilab (CDF) in a sample of p̄p collisions at
             s =1.8 TeV with an integrated luminosity of 19.3 pb-1. We
             find 12 events consistent with either two W bosons, or a W
             boson and at least one b jet. The probability that the
             measured yield is consistent with the background is 0.26%.
             Though the statistics are too limited to establish firmly
             the existence of the top quark, a natural interpretation of
             the excess is that it is due to tt̄ production. Under this
             assumption, constrained fits to individual events yield a
             top quark mass of 174±10-12+13 GeV/c2. The tt̄ production
             cross section is measured to be 13.9-4.8+6.1 pb. © 1994 The
             American Physical Society.},
   Doi = {10.1103/physrevlett.73.225},
   Key = {fds309795}
}

@article{fds309796,
   Author = {al, FAE},
   Title = {Evidence for top-quark production in (p)over-bar-p
             collisions at root-s=1.8 tev},
   Journal = {Phys. Rev. D},
   Volume = {50},
   Number = {5},
   Pages = {2966-3026},
   Publisher = {American Physical Society (APS)},
   Year = {1994},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevd.50.2966},
   Abstract = {© 1994 The American Physical Society. We present the
             results of a search for the top quark in 19.3 pb-1 of p̄p
             collisions at s =1.8 TeV. The data were collected at the
             Fermilab Tevatron collider using the Collider Detector at
             Fermilab (CDF). The search includes standard model tt̄
             decays to final states eeνν̄, eμνν̄, and μμνν̄
             as well as e+ν+jets or μ+ν+jets. In the (e,μ)+ν+jets
             channel we search for b quarks from t decays via secondary
             vertex identification and via semileptonic decays of the b
             and cascade c quarks. In the dilepton final states we find
             two events with a background of 0.56-0.13+0.25 events. In
             the e,μ+ν+jets channel with a b identified via a secondary
             vertex, we find six events with a background of 2.3±0.3.
             With a b identified via a semileptonic decay, we find seven
             events with a background of 3.1±0.3. The secondary vertex
             and semileptonic-decay samples have three events in common.
             The probability that the observed yield is consistent with
             the background is estimated to be 0.26%. The statistics are
             too limited to firmly establish the existence of the top
             quark; however, a natural interpretation of the excess is
             that it is due to tt̄ production. We present several
             cross-checks. Some support this hypothesis; others do not.
             Under the assumption that the excess yield over background
             is due to tt̄, constrained fitting on a subset of the
             events yields a mass of 174±10-12+13 GeV/c2 for the top
             quark. The tt̄ cross section, using this top quark mass to
             compute the acceptance, is measured to be 13.9-4.8+6.1
             pb.},
   Doi = {10.1103/physrevd.50.2966},
   Key = {fds309796}
}

@article{fds309800,
   Author = {al, TAE},
   Title = {Multiplicity dependence of transverse-momentum spectra of
             centrally produced hadrons in (p)overbar-p collisions at
             0.3, 0.54, 0.9, and 1.8 tev center-of-mass
             energy},
   Journal = {Phys. Lett. B},
   Volume = {336},
   Number = {3-4},
   Pages = {599-604},
   Publisher = {Elsevier BV},
   Year = {1994},
   Month = {September},
   url = {http://dx.doi.org/10.1016/0370-2693(94)90578-9},
   Abstract = {Transverse momentum spectra of charged particles produced
             within the pseudo-rapidity range of η= - 0.36 to + 1.0 have
             been measured in pp collisions at √s=0.3, 0.54, 1.0, and
             1.8 TeV. The spectra are presented as a function of event
             charged multiplicity within the range -3.25<η<3.25. We
             found that the slope in the low pt region is independent of
             center-of-mass energy and multiplicity while the slope at
             the high pt region shows a strong energy and multiplicity
             dependence. © 1994.},
   Doi = {10.1016/0370-2693(94)90578-9},
   Key = {fds309800}
}

@article{fds309797,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
             Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
             S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
             JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
             J},
   Title = {Precision measurement of the prompt photon cross section in
             pp-bar collisions at sqrt s =1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {73},
   Number = {20},
   Pages = {2662-2666},
   Publisher = {American Physical Society (APS)},
   Year = {1994},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.73.2662},
   Abstract = {A prompt photon cross section measurement from the Collider
             Detector at Fermilab experiment is presented. Detector and
             trigger upgrades, as well as 6 times the integrated
             luminosity compared with our previous publication, have
             contributed to a much more precise measurement and extended
             PT range. As before, QCD calculations agree qualitatively
             with the measured cross section, but the data has a steeper
             slope than the calculations. © 1994 The American Physical
             Society.},
   Doi = {10.1103/physrevlett.73.2662},
   Key = {fds309797}
}

@article{fds309798,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
             Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
             S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
             JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cen, Y and Cervelli, F and Chapman, J and Cheng,
             M},
   Title = {Search for the top quark decaying to a charged Higgs boson
             in p-barp collisions at sqrt s =1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {73},
   Number = {20},
   Pages = {2667-2671},
   Publisher = {American Physical Society (APS)},
   Year = {1994},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.73.2667},
   Abstract = {We present the results of a search in p̄p collisions at
             s=1.8 TeV for the top quark decaying to a charged Higgs
             boson (H±). We search for dilepton final states from the
             decay chain tt̄→HH (or HW, or WW) + bb̄→ll+X. In a
             sample of 19.3 pb-1 collected during 1992-93 with the
             Collider Detector at Fermilab, we observe 2 events with a
             background estimation of 3.0 ± 1.0 events. Limits at 95%
             C.L. in the (Mtop,MH±) plane are presented. For the case
             Mtop<MW+Mb, we exclude at 95% C.L. the entire (Mtop,MH±)
             plane for the branching ratio B(H→τν) larger than 75%.
             We also interpret the results in terms of the parameter tan
             β of two-Higgs-doublet models. © 1994 The American
             Physical Society.},
   Doi = {10.1103/physrevlett.73.2667},
   Key = {fds309798}
}

@article{fds309780,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and al, E},
   Title = {Production in pp» collisions at s=1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {75},
   Number = {24},
   Pages = {4358-4363},
   Year = {1995},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.4358},
   Abstract = {We report on measurements of the (1S), (2S), and (3S)
             differential, (d2 dPtdy)y=0, and integrated cross sections
             in pp» collisions at s=1.8 TeV using a sample of 16.6 0.6
             pb-1 collected by the Collider Detector at Fermilab. The
             three resonances were reconstructed through the decay.
             Comparison is made to a leading order QCD prediction. ©
             1995 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.75.4358},
   Key = {fds309780}
}

@article{fds309787,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
             Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
             S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
             JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
             J},
   Title = {Direct measurement of the W boson width.},
   Journal = {Physical review letters},
   Volume = {74},
   Number = {3},
   Pages = {341-345},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.74.341},
   Abstract = {This Letter describes a direct measurement of the W boson
             decay width, Γ(W), using the high-mass tail of the
             transverse mass spectrum of W→eν decays recorded by the
             Collider Detector at Fermilab. We findΓ(W)=2.11±0.28(stat)±0.16(syst)
             GeV and compare this direct measurement with indirect means
             of obtaining the width. © 1995 The American Physical
             Society.},
   Doi = {10.1103/physrevlett.74.341},
   Key = {fds309787}
}

@article{fds309791,
   Author = {al, FAE},
   Title = {Charge asymmetry in w-boson decays produced in p(p)over-bar
             collisions at root-s=1.8 tev},
   Journal = {Phys. Rev. Lett.},
   Volume = {74},
   Number = {6},
   Pages = {850-854},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevLett.74.850},
   Abstract = {Charge asymmetry has been measured using 19 039 W decays
             recorded by the Collider Detector at Fermilab during the
             1992-93 run of the Tevatron Collider. The asymmetry is
             sensitive to the ratio of d and u quark distributions to
             x<0.01 at Q2MW2, where nonperturbative effects are minimal.
             It is found that of the two current sets of parton
             distributions, those of Martin, Roberts, and Stirling are
             favored over the sets most recently produced by the CTEQ
             Collaboration. The W asymmetry data provide stronger
             constraints on du ratio than the recent measurements of
             F2μnF2μp which are limited by uncertainties originating
             from deuteron corrections. © 1995 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.74.850},
   Key = {fds309791}
}

@article{fds309785,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
             Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
             S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
             JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
             J},
   Title = {Limits on Z-photon couplings from p-p-bar interactions at
             sqrt s=1.8TeV.},
   Journal = {Physical review letters},
   Volume = {74},
   Number = {11},
   Pages = {1941-1945},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.74.1941},
   Abstract = {We report limits on anomalous ZZ and Z couplings derived
             from an analysis of Z+photon production based upon
             approximately 20 pb-1 of the pp collision data recorded by
             the Collider Detector at Fermilab. We observe good agreement
             with the standard model expectation that all Z couplings are
             zero. Confidence level intervals for individual couplings
             and contours for pairs of CP-conserving/violating ZZ and Z
             couplings are presented. © 1995 The American Physical
             Society.},
   Doi = {10.1103/physrevlett.74.1941},
   Key = {fds309785}
}

@article{fds309786,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
             Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
             S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
             JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
             J},
   Title = {Measurement of W-photon couplings in p-p-bar collisions at
             sqrt s=1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {74},
   Number = {11},
   Pages = {1936-1940},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.74.1936},
   Abstract = {We report on a study of W + photon production in
             approximately 20 pb-1 of p-p collisions at s=1.8 TeV
             recorded with the Collider Detector at Fermilab. Our results
             are in good agreement with standard model expectations and
             are used to obtain limits on anomalous CP-conserving WW
             couplings of -2.3<<2.2 for =0 and -0.7<<0.7 for =0 at 95%
             C.L. We obtain the same limits for CP-violating couplings.
             These results provide limits on the higher-order
             electromagnetic moments of the W boson of 0.8<gW<3.1 for
             qWe=1 and -0.6<qWe<2.7 for gW=2 at 95% C.L. © 1995 The
             American Physical Society.},
   Doi = {10.1103/physrevlett.74.1936},
   Key = {fds309786}
}

@article{fds309771,
   Author = {al, FAE},
   Title = {Observation of top-quark production in (p)over-bar-p
             collisions with the collider detector at
             fermilab},
   Journal = {Phys. Rev. Lett.},
   Volume = {74},
   Number = {14},
   Pages = {2626-2631},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.74.2626},
   Abstract = {We establish the existence of the top quark using a 67 pb-1
             data sample of p̄p collisions at s=1.8 TeV collected with
             the Collider Detector at Fermilab (CDF). Employing
             techniques similar to those we previously published, we
             observe a signal consistent with tt̄ decay to WWbb̄, but
             inconsistent with the background prediction by 4.8σ.
             Additional evidence for the top quark is provided by a peak
             in the reconstructed mass distribution. We measure the top
             quark mass to be 176±8(stat)±10(syst) GeV/c2, and the tt̄
             production cross section to be 6.8-2.4+3.6 pb. © 1995 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.74.2626},
   Key = {fds309771}
}

@article{fds309788,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de
             Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
             S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
             JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman,
             J},
   Title = {Search for charged bosons heavier than the W boson in pp-bar
             collisions at sqrt s=1800 GeV.},
   Journal = {Physical review letters},
   Volume = {74},
   Number = {15},
   Pages = {2900-2904},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.74.2900},
   Abstract = {We have searched for new, heavy, charged bosons W′ through
             the decay W′→eν in pp̄ collisions at s=1.8 TeV. The
             data used in the search represent 19.7 pb-1 collected by the
             Collider Detector at Fermilab. Limits are placed on
             σB(pp̄→W′→eν) as a function of MW′. Assuming
             standard couplings of the W′ to fermions, we establish the
             limit MW′>652 GeV /c2 (95% C.L.). © 1995 The American
             Physical Society.},
   Doi = {10.1103/physrevlett.74.2900},
   Key = {fds309788}
}

@article{fds309775,
   Author = {al, FAE},
   Title = {Search for new particles decaying to dijets in p(p)over-bar
             collisions at root-s=1.8 tev},
   Journal = {Phys. Rev. Lett.},
   Volume = {74},
   Number = {18},
   Pages = {3538-3543},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevLett.74.3538},
   Abstract = {We have used 19 pb-1 of data collected with the Collider
             Detector at Fermilab to search for new particles decaying to
             dijets. We exclude at 95% confidence level models containing
             the following new particles: axigluons with mass between 200
             and 870 GeV/ c2, excited quarks with mass between 80 and 570
             GeV/ c2, and color octet technirhos with mass between 320
             and 480 GeV/ c2. © 1995 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.74.3538},
   Key = {fds309775}
}

@article{fds309784,
   Author = {al, FAE},
   Title = {Kinematic evidence for top-quark pair production in w plus
             multijet events in p(p)over-bar collisions at root-s=1.8
             tev},
   Journal = {Phys. Rev. D},
   Volume = {51},
   Number = {9},
   Pages = {4623-4637},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevd.51.4623},
   Abstract = {© 1995 The American Physical Society We present a study of
             W+multijet events that compares the kinematics of the
             observed events with expectations from direct QCD W+jet
             production and from production and decay of top quark pairs.
             The data were collected in the 1992-93 run with the Collider
             Detector at Fermilab (CDF) from 19.3 pb-1 of
             proton-antiproton collisions at s =1.8 TeV. A W+2 jet sample
             and a W+3 jet sample are selected with the requirement that
             at least the two or three jets have energy transverse with
             respect to the beam axis in excess of 20 GeV. The jet energy
             distributions for the W+2 jet sample agree well with the
             predictions of direct QCD W production. From the W+3 jet
             events, a "signal sample" with an improved ratio of tt̄ to
             QCD produced W events is selected by requiring each jet to
             be emitted centrally in the event center of mass frame. This
             sample contains 14 events with unusually hard jet ET
             distributions not well described by expectations for jets
             from direct QCD W production and other background processes.
             Using expected jet ET distributions, a relative likelihood
             is defined and used to determine if an event is more
             consistent with the decay of tt̄ pairs, with Mtop=170
             GeV/c2, than with direct QCD W production. Eight of the 14
             signal sample events are found to be more consistent with
             top-quark than direct QCD W production, while only 1.7 such
             top-quark-like events are expected in the absence of tt̄.
             The probability that the observation is due to an upward
             fluctuation of the number of background events is found to
             be 0.8%. The robustness of the result was tested by varying
             the cuts defining the signal sample, and the largest
             probability for such a fluctuation found was 1.9%. Good
             agreement in the jet spectra is obtained if jet production
             from tt̄ pair decays is included. For those events
             kinematically more consistent with tt̄ we find evidence for
             a b-quark content in their jets to the extent expected from
             top quark decay, and larger than expected for background
             processes. For events with four or more jets, the
             discrepancy with the predicted jet distributions from direct
             QCD W production, and the associated excess of b-quark
             content, is more pronounced.},
   Doi = {10.1103/physrevd.51.4623},
   Key = {fds309784}
}

@article{fds309774,
   Author = {al, FAE},
   Title = {Measurement of the b-s meson lifetime},
   Journal = {Phys. Rev. Lett.},
   Volume = {74},
   Number = {25},
   Pages = {4988-4992},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevLett.74.4988},
   Abstract = {The lifetime of the Bs meson is measured using the
             semileptonic decay Bs→Ds-+νX. The data sample consists of
             19.3 pb-1 of pp̄ collisions at s=1.8 TeV collected by the
             Collider Detector at Fermilab during 1992-1993. There are
             76±8 +Ds- signal events where the Ds is identified via the
             decay Ds-→φπ-, φ→K+K-. Using these events, the Bs
             meson lifetime is determined to be τs=1.42-0.23+0.27(stat)±0.11(syst)
             ps. A measurement of the Bs lifetime in a low statistics
             sample of exclusive Bs→J/ψ φ decays is also presented in
             this paper. © 1995 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.74.4988},
   Key = {fds309774}
}

@article{fds310559,
   Author = {Alexopoulos, T and Allen, C and Anderson, EW and Balamurali, V and Banerjee, S and Beery, PD and Bhat, P and Bishop, JM and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Choi, Y and Cole, P and DeBonte,
             R and DeCarlo, V and Erwin, AR and Findeisen, C and Goshaw, AT and Gutay,
             LJ and Hirsch, AS and Hojvat, C and Jennings, JR and Kenny, VP and Lindsey,
             CS and Loomis, C and LoSecco, JM and McMahon, T and McManus, AP and Morgan,
             N and Nelson, K and Oh, SH and Porile, NT and Reeves, D and Rimai, A and Robertson, WJ and Scharenberg, RP and Stampke, SR and Stringfellow,
             BC and Thompson, M and Turkot, F and Walker, WD and Wang, CH and Warchol,
             J and Wesson, DK and Zhan, Y},
   Title = {Charged particle multiplicity correlations in pp̄
             collisions at s=0.3-1.8 TeV},
   Journal = {Physics Letters B},
   Volume = {353},
   Number = {1},
   Pages = {155-160},
   Publisher = {Elsevier BV},
   Year = {1995},
   Month = {June},
   url = {http://dx.doi.org/10.1016/0370-2693(95)00554-X},
   Abstract = {The correlations between charged particle multiplicitie
             produced in forward and backward pseudorapidity regions in
             pp̄ interactions have been measured with a 240 element
             scintillator hodoscope. The correlation coefficient and the
             variance of the difference of multiplicities in the two
             pseudorapidity regions were deterermined for s=0.3-1.8 TeV.
             These results have been interpreted in terms of a cluster
             model of particle production. © 1995.},
   Doi = {10.1016/0370-2693(95)00554-X},
   Key = {fds310559}
}

@article{fds309778,
   Author = {al, FAE},
   Title = {Properties of high-mass multijet events at the fermilab
             proton-antiproton collider},
   Journal = {Phys. Rev. Lett.},
   Volume = {75},
   Number = {4},
   Pages = {608-612},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.608},
   Abstract = {The properties of two-, three-, four-, five-, and six-jet
             events with multijet masses >600 GeV /c2 are compared with
             QCD predictions. The shapes of the multijet-mass and
             leading-jet-angular distributions are approximately
             independent of jet multiplicity and are well described by
             the NJETS matrix element calculation and the HERWIG parton
             shower Monte Carlo predictions. The observed jet transverse
             momentum distributions for three- and four-jet events
             discriminate between the matrix element and parton shower
             predictions, the data favoring the matrix element
             calculation. © 1995 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.75.608},
   Key = {fds309778}
}

@article{fds309779,
   Author = {al, FAE},
   Title = {Measurement of the w-boson mass},
   Journal = {Phys. Rev. Lett.},
   Volume = {75},
   Number = {1},
   Pages = {11-16},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.11},
   Abstract = {We present a measurement of the mass of the W boson using
             data collected with the Collider Detector at Fermilab during
             the 1992-93 collider run at the Fermilab Tevatron. A fit to
             the transverse mass spectrum of a sample of 3268 W→μν
             events recorded in an integrated luminosity of 19.7 pb-1
             gives a mass MWμ=80.310±0.205(stat)±0.130(syst) GeV/c2. A
             fit to 5718 W→eν events recorded in 18.2 pb-1 gives
             MWe=80.490±0.145(stat) ±0.175syst GeV/c2. Combining these
             results, accounting for correlated uncertainties, yields
             MW=80.410±0.180 GeV/c2. © 1995 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.75.11},
   Key = {fds309779}
}

@article{fds309793,
   Author = {Aoki, S and Bahk, SY and Chung, KS and Chung, SH and Funahashi, H and Hahn,
             CH and Hara, T and Hirata, S and Hoshino, K and Ieiri, M and Ijima, T and Imai, K and Itow, Y and Jin-ya, T and Kazuno, M and Kikuchi, K and Kim, CO and Kim, DC and Kim, JY and Kodama, K and Maeda, Y and Masaike, A and Masuoka,
             A and Matsuda, Y and Nagoshi, C and Nakamura, M and Nakanishi, S and Nakano, T and Nakazawa, K and Niwa, K and Oda, H and Ogawa, S and Oh, SH and Okabe, H and Ozaki, R and Park, IG and Park, MS and Sato, Y and Shibuya, H and Shimizu, HM and Sim, YB and Song, JS and Sugimoto, M and Tajima, H and Takashima, R and Takeutchi, F and Tanaka, KH and Tanaka, R and Teranaka,
             M and Tezuka, I and Togawa, H and Ushida, N and Watanabe, T and Yasuda, N and Yokota, J and Yoon, CS},
   Title = {Production of a twin single hypernuclei and the
             Ξ--nuclear interaction},
   Journal = {Physics Letters B},
   Volume = {355},
   Number = {1-2},
   Pages = {45-51},
   Publisher = {Elsevier BV},
   Year = {1995},
   Month = {July},
   url = {http://dx.doi.org/10.1016/0370-2693(95)00688-H},
   Abstract = {An event accompanied by two single hyperfragments emitted
             from a Ξ- nuclear capture at rest was found in a nuclear
             emulsion. It is interpreted as a Ξ--12C bound system
             decaying into either a) Λ4H + Λ9Be, b) Λ4H + Λ9Be* or c)
             Λ4H* + Λ9Be. The binding energy of the Ξ-12C system is
             obtained as a) 3.70-0.19+0.18 MeV, b) 0.62-0.19+0.18 MeV and
             c) 2.66-0.19+0.18 MeV, respectively. The system is
             considered as a Ξ- hypernucleus in the cases a) and c). In
             case b), this event and another event of the same type
             (Yokohama event) can both be interpreted as a decay from the
             Ξ-12C system in 2P state when a shallow Ξ--nuclear
             potential is assumed. © 1995.},
   Doi = {10.1016/0370-2693(95)00688-H},
   Key = {fds309793}
}

@article{fds309776,
   Author = {al, FAE},
   Title = {Limits on wwz and ww-gamma couplings from ww and wz
             production in p(p)over-bar collisions at root-s=1.8
             tev},
   Journal = {Phys. Rev. Lett.},
   Volume = {75},
   Number = {6},
   Pages = {1017-1022},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.1017},
   Abstract = {Direct limits are set on WWZ and WW three-boson couplings in
             a search for WW and WZ production with high transverse
             momentum in pp» collisions at s=1.8 TeV, using the Collider
             Detector at Fermilab. The results are in agreement with the
             SU(2) × U(1) model of electroweak interactions. Assuming
             standard model WW couplings, the limits are interpreted as
             direct evidence for a nonzero WWZ coupling at subprocess
             energies near 500 GeV. Alternatively, assuming identical WWZ
             and WW couplings, bounds -0.11< <2.27 and -0.81< <0.84 are
             obtained at 95% C.L. for a form factor scale 1000 GeV. ©
             1995 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.75.1017},
   Key = {fds309776}
}

@article{fds309777,
   Author = {al, FAE},
   Title = {Measurement of the b-meson differential cross-section
             d-sigma/dp(t) in p(p)over-bar collisions at root-s=1.8
             tev},
   Journal = {Phys. Rev. Lett.},
   Volume = {75},
   Number = {8},
   Pages = {1451-1455},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.1451},
   Abstract = {This paper presents the first direct measurement of the B
             meson differential cross section dσ/dpT in pp̄ collisions
             at s=1.8 TeV using a sample of 19.3±0.7 pb-1 accumulated by
             the Collider Detector at Fermilab. The cross section is
             measured in the central rapidity region |y|<1 for pTB>6.0
             GeV /c by fully reconstructing the B meson decays
             B+→J/ψK+ and B0→J/ψK*0892, where J/ψ→μ+μ- and
             K*0→K+π-. A comparison is made to the theoretical QCD
             prediction calculated at next-to-leading order. © 1995 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.75.1451},
   Key = {fds309777}
}

@article{fds309781,
   Author = {al, FAE},
   Title = {Search for 2nd-generation leptoquarks in p(p)over-bar
             collisions at root-s=1.8 tev},
   Journal = {Phys. Rev. Lett.},
   Volume = {75},
   Number = {6},
   Pages = {1012-1016},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.1012},
   Abstract = {We present the results of a search for second generation
             leptoquarks S2 using 19.3 pb-1 of data collected at the
             Collider Detector at Fermilab (CDF) in pp» collisions at
             s=1.8 TeV during the 1992 93 collider run. We have searched
             for S2S2» pairs assuming that each leptoquark decays to a
             muon + quark with a branching ratio. We find two candidate
             events, consistent with an expected background of 1.11 0.48.
             We obtain upper limits on (pp» S2S2») 2 as a function of
             MS2. Using a Monte Carlo prediction for S2S2» pair
             production, we exclude MS2<131GeV/c2 for =1 and MS2<96GeV/c2
             for =0.5 at 95% C.L. © 1995 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.75.1012},
   Key = {fds309781}
}

@article{fds309773,
   Author = {al, FAE},
   Title = {Identification of top quarks using kinematic
             variables},
   Journal = {Phys. Rev. D},
   Volume = {52},
   Number = {5},
   Pages = {R2605-R2609},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.52.R2605},
   Abstract = {We have used a kinematic technique to distinguish top quark
             pair production from background in pp collisions at s=1.8
             TeV, applied to 67 pb-1 of data. We define a sample of W+3
             jet events in which the jets are produced at large angles
             relative to the incident beams. In this sample, we find an
             excess of events with large jet transverse energies relative
             to expectations from background. The excess is consistent
             with top quark production; a large fraction of events in
             this kinematic region contains b jets. We interpret these
             results as evidence that most of the selected events are
             from tt decay.},
   Doi = {10.1103/PhysRevD.52.R2605},
   Key = {fds309773}
}

@article{fds309783,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cen, Y},
   Title = {Measurement of the ratio sigma B(pp-bar-->W-->e nu )/ sigma
             B(pp-bar-->Z0-->ee) in pp-bar collisions at sqrt s =1800
             GeV.},
   Journal = {Physical review. D, Particles and fields},
   Volume = {52},
   Number = {5},
   Pages = {2624-2655},
   Year = {1995},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevd.52.2624},
   Abstract = {© 1995 The American Physical Society We present an analysis
             of data from p p collisions at a center-of-mass energy of s
             =1800 GeV. A measurement is made of the ratio RB(p pWe)/B(p
             pZ0ee). The data represent 19.6 pg-1 collected by the
             Collider Detector at Fermilab during the 19921993 collider
             run of the Fermilab Tevatron. We find R=10.900.32(stat)0.29(syst),
             and from this value we extract a measurement of the We
             branching ratio (We)/(W)=0.10940.0033(stat)0.0031(syst).
             From this branching ratio we set a limit on the top quark
             mass of mt>62 GeV/c2 at the 95% confidence level. In
             contrast with direct searches for the top quark, this limit
             makes no assumptions about the allowed decay modes of the
             top quark. In addition, we use a calculation of the leptonic
             width (We) to obtain a value for the W total decay width:
             (W)=2.0640.060(stat)0.059(syst) GeV.},
   Doi = {10.1103/physrevd.52.2624},
   Key = {fds309783}
}

@article{fds309792,
   Author = {Alexopoulos, T and Allen, C and Anderson, EW and Balamurali, V and Banerjee, S and Beery, PD and Bhat, P and Bishop, JM and Biswas, NN and Bujak, A and Carmony, DD and Carter, T and Cole, P and Choi, Y and DeBonte,
             R and DeCarlo, V and Erwin, AR and Findeisen, C and Goshaw, AT and Gutay,
             LJ and Hirsch, AS and Hojvat, C and Jennings, JR and Kenney, VP and Lindsey, CS and Loomis, C and LoSecco, JM and McMahon, T and McManus,
             AP and Morgan, N and Nelson, K and Oh, SH and Porile, NT and Rimai, A and Reeves, D and Robertson, WJ and Scharenberg, RP and Stringfellow, BC and Stampke, SR and Thompson, M and Turkot, F and Walker, WD and Wang, CH and Warchol, J and Wesson, DK and Zhan, Y},
   Title = {φ meson production from {Mathematical expression}
             collisions at {Mathematical expression} TeV},
   Journal = {Zeitschrift für Physik C Particles and Fields},
   Volume = {67},
   Number = {3},
   Pages = {411-416},
   Publisher = {Springer Nature},
   Year = {1995},
   Month = {September},
   url = {http://dx.doi.org/10.1007/BF01624584},
   Abstract = {Fermilab experiment E735 located at the CO intersection
             region of the {Mathematical expression} TeV {Mathematical
             expression} collider analysed over 900 Φ→K+K- events.
             Measured were the transverse momentum spectrum, the
             correlation between the average transverse momentum <pt> and
             the charged particle multiphcity Nc, as well as the
             probability of Φ production per charged track, NΦ/Nc,
             versus Nc. We have also made an estinate of the total
             inclusive cross section for Φ mesons, {Mathematical
             expression}. © 1995 Springer-Verlag.},
   Doi = {10.1007/BF01624584},
   Key = {fds309792}
}

@article{fds309782,
   Author = {al, FAE},
   Title = {Measurement of the polarization in the decays
             b-d-]j/psi-k-(asterisk-0) and bs-]j/psi-phi},
   Journal = {Phys. Rev. Lett.},
   Volume = {75},
   Number = {17},
   Pages = {3068-3072},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.3068},
   Abstract = {This Letter reports on measurements of the longitudinal
             polarization fractions in the decays Bd→J/ψ K*0 and
             Bs→J/ψ φ using data collected with the Collider Detector
             at Fermilab. Bd mesons are reconstructed through the decay
             chain Bd→J/ψ K*0, J/ψ→μ+μ-, K*0→K+π-. A sample of
             65±10 Bd events is used to obtain a longitudinal
             polarization fraction of γL/γ=0.65±0.10(stat)±0.04(syst).
             Bs mesons are reconstructed through the decay chain
             Bs→J/ψ φ, J/ψ→μ+μ-, φ→K+K-. A sample of 19±5 Bs
             events is used to obtain the result γL/γ=0.56±0.21(stat)-0.04+0.
             02(syst). © 1995 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.75.3068},
   Key = {fds309782}
}

@article{fds309772,
   Author = {al, FAE},
   Title = {Study of t(t)over-bar production in p(p)over-bar collisions
             using total transverse energy},
   Journal = {Phys. Rev. Lett.},
   Volume = {75},
   Number = {22},
   Pages = {3997-4002},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.75.3997},
   Abstract = {We analyze a sample of W+jet events collected with the
             Collider Detector at Fermilab (CDF) in pp» collisions at
             s=1.8 TeV to study tt» production. We employ a simple
             kinematical variable H, defined as the scalar sum of the
             transverse energies of the lepton, neutrino, and jets. For
             events with a W boson and four or more jets, the shape of
             the H distribution deviates by 3.8 standard deviations from
             that expected from known backgrounds to tt» production.
             However, this distribution agrees well with a linear
             combination of background and tt» events, the agreement
             being best for a top mass of 180 GeV/c2. © 1995 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.75.3997},
   Key = {fds309772}
}

@article{fds309789,
   Author = {al, FAE},
   Title = {Measurement of the w-boson mass},
   Journal = {Phys. Rev. D},
   Volume = {52},
   Number = {9},
   Pages = {4784-4827},
   Publisher = {American Physical Society (APS)},
   Year = {1995},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevd.52.4784},
   Abstract = {© 1995 The American Physical Society This paper presents a
             measurement of the mass of the W boson using data collected
             with the CDF detector during the 1992-1993 collider run at
             the Fermilab Tevatron. A fit to the transverse mass spectrum
             of a sample of 3268 W→μν events recorded in an
             integrated luminosity of 19.7 pb-1 gives MWμ=80.310±0.205
             (stat)±0.130 (syst) GeV/c2. A fit to the transverse mass
             spectrum of a sample of 5718 W→eν events recorded in 18.2
             pb-1 gives MWe=80.490±0.145 (stat)±0.175 (syst) GeV/c2.
             Combining the muon and electron results, accounting for
             correlated uncertainties, yields MW=80.410±0.180
             GeV/c2.},
   Doi = {10.1103/physrevd.52.4784},
   Key = {fds309789}
}

@article{fds309790,
   Author = {Abe, F and Albrow, MG and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and De
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends,
             S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge,
             JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boswell, C and Boulos, T and Brandenburg, G and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cen, Y and Cervelli, F and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Cihangir, S and Clark,
             AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli,
             M and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias, JE and Ely, R and Engels, E and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I},
   Title = {Erratum: Precision measurement of the prompt photon cross
             section in pp collisions at s=1.8 TeV (Physical Review
             Letters(1995) 74, 10 (1891-1893))},
   Journal = {Physical Review Letters},
   Volume = {74},
   Number = {10},
   Pages = {1891-1893},
   Year = {1995},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.74.1891},
   Doi = {10.1103/PhysRevLett.74.1891},
   Key = {fds309790}
}

@article{fds309752,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Bondreau, J and Breccia, L and Bromberg,
             C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
             D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
             F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Dunn, A and Eddy,
             N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Errede, D and Errede, S and Fan, Q and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman,
             J and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti,
             S and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Hardman, AD and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Hayashi, E and Heinrich, J and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes, R and Huston, J and Huth, J and Hylen, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and Jensen, H and Joshi, U and Kadel, RW and Kajfasz,
             E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato,
             Y and Keaffaber, TA and Keeble, L and Kelley, K and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian,
             H and Keyvan, F and Kharadia, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
             SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Korytov, A and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuwabara, T and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca,
             N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis,
             JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lu, J and Lucchesi, D and Lukens, P and Lusin,
             S and Lys, J and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin,
             A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Mitsushio, H and Miyamoto, T and Miyashita, S and Moggi, N and Morita,
             Y and Mueller, J and Mukherjee, A and Muller, T and Murat, P and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ninomiya, M and Nodulman, L and Oh, SH and Ohl, KE and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Oliveira, R and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Park, S and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett,
             R and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Romano, J and Rosenson, L and Roser, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scribano, A and Segler,
             S and Seidel, S and Seiya, Y and Sganos, G and Shapiro, MD and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Snider,
             FD and Song, T and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
             A and Strahl, K and Strait, J and Ströhmer, R and Stuart, D and Sullivan,
             G and Soumarokov, A and Sumorok, K and Suzuki, J and Takada, T and Takahashi, T and Takano, T and Takikawa, K and Tamura, N and Tartarelli,
             F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk,
             S and Toback, D and Tollefson, K and Tollestrup, A and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Uemura, N and Ukegawa, F and Unal, G and Vails, J and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, N and Wang, C and Wang, CH and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yu, L and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, W and Zucchelli,
             S},
   Title = {Measurement of the branching fraction B(Bu+→J/ψπ+)
             and search for Bc+→J/ψπ+},
   Journal = {Physical Review Letters},
   Volume = {77},
   Number = {26},
   Pages = {5176-5181},
   Year = {1996},
   url = {http://dx.doi.org/10.1103/PhysRevLett.77.5176},
   Abstract = {We report on a measurement of the branching fraction of the
             Cabibbo-suppressed decay Bu+→J/ψπ+ , where
             J/ψ→μ+μ-. The data were collected by the Collider
             Detector at Fermilab during 1992-1995 and correspond to an
             integrated luminosity of 110 pb-1 in p̄p collisions at √s
             = 1.8 TeV. A signal of 289+10 events is observed and we
             determine the ratio of branching fractions
             B(Bu+→J/ψπ+)/B(Bu+→J/ψK+) to be [5.0-1.7+1.9(stat) ±
             0.1(syst)]%. Using the world average value for
             B(Bu+→J/ψK+), we calculate the branching fraction
             B(Bu+→J/ψπ+) to be (5.0-1.9+2.1) × 10-5. We also search
             for the decay Bc+→J/ψπ+ and report a 95% confidence
             level limit on σ(Bc+)B(Bc+→ J/ψπ+)/σ(Bu+)B(Bu+→J/ψK+)
             as a function of the Bc+ lifetime.},
   Doi = {10.1103/PhysRevLett.77.5176},
   Key = {fds309752}
}

@article{fds309756,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
             R and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Dunn, A and Eddy, N and Einsweiler,
             K and Elias, JE and Ely, R and Jr, EE and Errede, D and Errede, S and Fan, Q and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi,
             M and Freeman, J and Friedman, J and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold,
             M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Guo,
             RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Hardman, AD and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Hayashi, E and Heinrich, J and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
             L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes, R and Huston, J and Huth, J and Hylen, J and Ikeda, H and Incagli,
             M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and Jensen, H and Joshi, U and Kadel, RW and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Keeble, L and Kelley, K and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kharadia,
             B and Kim, BJ and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuwabara, T and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lu, J and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi,
             E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Mitsushio, H and Miyamoto,
             T and Miyashita, S and Moggi, N and Morita, Y and Mueller, J and Mukherjee,
             A and Muller, T and Murat, P and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ninomiya, M and Nodulman, L and Oh, SH and Ohl, KE and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Oliveira, R and Olsen, J and Pagliarone, C and Paoletti,
             R and Papadimitriou, V and Pappas, SP and Park, S and Parri, A and Patrick,
             J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters,
             MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Romano, J and Rosenson, L and Roser, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Scarpine, V and Schlabach, P and Schmidt, EE and Schmidt, MP and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Sganos, G and Shapiro, M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Snider, FD and Song, T and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strahl, K and Strait, J and Ströhmer, R and Stuart, D and Sullivan, G and Soumarokov, A and Sumorok, K and Suzuki, J and Takada, T and Takahashi, T and Takano, T and Takikawa, K and Tamura, N and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Uemura, N and Ukegawa, F and Unal, G and Brink, SVD and III, SV and Velev, G and Vidal,
             R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
             J and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel,
             H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, D and Wolinski,
             J and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh,
             GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yu, L and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, W and Zucchelli, S},
   Title = {Measurement of the Λb0 lifetime using
             Λb0 → Λc+l-
             ν̄},
   Journal = {Physical Review Letters},
   Volume = {77},
   Number = {8},
   Pages = {1439-1443},
   Year = {1996},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.77.1439},
   Abstract = {The lifetime of Λb0^ is measured using the semileptonic
             decay Λb0 → Λc+l-ν-, where the Λc+ is reconstructed
             through its decay Λc+ → pK- π+. The data were collected
             by the CDF detector at the Tevatron Collider during
             1992-1995 and correspond to an integrated luminosity of 110
             pb-1 of pp̄ collisions at √s = 1.8 TeV. From a fit to the
             decay length distribution of the Λc-lepton system from 197
             ± 25 signal events, the lifetime of Λb0 is measured to be
             1.32 ± 0.15 ± 0.07 ps.},
   Doi = {10.1103/physrevlett.77.1439},
   Key = {fds309756}
}

@article{fds309758,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
             R and Cunningham, JD and Daniels, T and Jongh, FD and Delchamps, S and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Dunn, A and Eddy, N and Einsweiler,
             K and Elias, JE and Ely, R and Jr, EE and Errede, D and Errede, S and Fan, Q and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi,
             M and Freeman, J and Friedman, J and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold,
             M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Guo,
             RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Hardman, AD and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Hayashi, E and Heinrich, J and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
             L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes, R and Huston, J and Huth, J and Hylen, J and Ikeda, H and Incagli,
             M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and Jensen, H and Joshi, U and Kadel, RW and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Keeble, L and Kelley, K and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kharadia,
             B and Kim, BJ and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Korytov, A and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuwabara, T and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lu, J and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi,
             E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Mitsushio, H and Miyamoto,
             T and Miyashita, S and Moggi, N and Morita, Y and Mueller, J and Mukherjee,
             A and Muller, T and Murat, P and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ninomiya, M and Nodulman, L and Oh, SH and Ohl, KE and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Oliveira, R and Olsen, J and Pagliarone, C and Paoletti,
             R and Papadimitriou, V and Pappas, SP and Park, S and Parri, A and Patrick,
             J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters,
             MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Romano, J and Rosenson, L and Roser, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Scarpine, V and Schlabach, P and Schmidt, EE and Schmidt, MP and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Sganos, G and Shapiro, MD and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Snider, FD and Song, T and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strahl, K and Strait, J and Ströhmer, R and Stuart, D and Sullivan, G and Soumarokov, A and Sumorok, K and Suzuki, J and Takada, T and Takahashi, T and Takano, T and Takikawa, K and Tamura, N and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and III, SV and Velev, G and Vidal,
             R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
             J and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel,
             H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, D and Wolinski,
             J and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh,
             GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yu, L and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, W and Zucchelli, S},
   Title = {Measurement of the lifetime of the Bs0
             meson using the exclusive decay mode Bs0
             → J/ψ φ},
   Journal = {Physical Review Letters},
   Volume = {77},
   Number = {10},
   Pages = {1945-1949},
   Year = {1996},
   url = {http://dx.doi.org/10.1103/PhysRevLett.77.1945},
   Abstract = {The lifetime of the Bs0 meson is measured using the
             exclusive decay mode Bs0 → J / ψ φ, where J/ψ →
             μ+μ- and φ → K+K-. The data sample consists of 110 pb-1
             of p p̄ collisions at √s = 1.8 TeV, collected by the CDF
             detector at the Fermilab Tevatron collider during 1992-1995.
             We find 58 ± 12 signal events, and the Bs0 meson lifetime
             is determined to be τBs0; = 1.34-0.19+0.23(stat) ±
             0.05(syst) ps. This result is consistent with previous
             measurements of the Bs0, B+, and Bd0 meson lifetimes and
             with theoretical predictions.},
   Doi = {10.1103/PhysRevLett.77.1945},
   Key = {fds309758}
}

@article{fds309761,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, M-T and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
             JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
             JE and Ely, R and Engels, E and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Frisch, H and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti,
             P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
             C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Holscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
             R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
             CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
             S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
             LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
             T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos,
             F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto, WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler,
             S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro,
             M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding,
             J and Spiegel, L and Sphicas, P and Stanco, L and Steele, J and Stefanini,
             A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Swartz, RL and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov,
             A and Tkaczyk, S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and Vejcik, S and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and Wester, WC and Westhusing, T and Wicklund,
             AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef, C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli, S},
   Title = {Measurement of the mass of the Bs0
             meson},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {53},
   Number = {7},
   Pages = {3496-3505},
   Year = {1996},
   url = {http://dx.doi.org/10.1103/physrevd.53.3496},
   Abstract = {We measure the mass of the B0s meson by reconstructing the
             decay chain B0s→J/ψφ, J/ψ→µ+µ-, and φ→K+K-. The
             data are obtained from 19.3 pb-1 of integrated luminosity of
             pp collisions at √s=1.8 TeV using the Collider Detector at
             Fermilab. A sample of 80 000 inclusive J/ψ→µ+µ- events
             is used to study systematic biases in track reconstruction
             and to calibrate the momentum scale. We reconstruct the
             kinematically similar decays B+→J/ψK+ and B0→J/ψK*0 to
             study the mass measurement technique used for the B0s meson.
             Based on the observation of 32 ± 6 candidates, the mass of
             the B0s meson is measured to be 5369.9 ± 2.3 ± 1.3 MeV/c2
             and the mass difference between B0s and the average mass of
             B+ and B0 is determined to be 89.7 ± 2.7 ± 1.2 MeV/c2. ©
             1996 The American Physical Society.},
   Doi = {10.1103/physrevd.53.3496},
   Key = {fds309761}
}

@article{fds309763,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
             JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
             JE and Ely, R and Jr, EE and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Frisch, H and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti,
             P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
             C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
             R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
             CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
             S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
             LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
             T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto,
             WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro, M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding, J and Spiegel, L and Sphicas, P and Spies, A and Stanco, L and Steele, J and Stefanini, A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Jr, RLS and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor,
             W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov, A and Tkaczyk,
             S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and III, SV and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Westhusing, T and Wicklund, AB and Wicklund,
             E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef,
             C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli,
             S},
   Title = {Measurement of σB(W→ev) and σB(Z0→e+e-)
             in pp̄ collisions at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {76},
   Number = {17},
   Pages = {3070-3075},
   Year = {1996},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.76.3070},
   Abstract = {We present a measurement of σB(W → ev) and σB(Z0 →
             e+e-) in proton-antiproton collisions at √s = 1.8 TeV
             using a significantly improved understanding of the
             integrated luminosity. The data represent an integrated
             luminosity of 19.7 pb-1 from the 1992-1993 run with the
             Collider Detector at Fermilab. We find σB(W → ev) = 2.49
             ± 0.12 nb and σB(Z0 ?→ e+e- = 0.231 ± 0.012
             nb.},
   Doi = {10.1103/physrevlett.76.3070},
   Key = {fds309763}
}

@article{fds309764,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and DeJongh, F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
             JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
             JE and Ely, R and Jr, EE and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro,
             M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold,
             M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
             C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
             R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
             CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
             S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
             LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
             T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos,
             F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto, WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler,
             S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro,
             M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding,
             J and Spiegel, L and Sphicas, P and Stanco, L and Steele, J and Stefanini,
             A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Swartz, RL and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov,
             A and Tkaczyk, S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and III, SV and Vidal, R and Vondracek, M and Vucunic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Westhusing, T and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer,
             BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef,
             C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli,
             S},
   Title = {Reconstruction of B0 → J/ψ
             KS0 and measurement of ratios of
             branching ratios involving B → J/ψK* and B+
             → J/ψK+},
   Journal = {Physical Review Letters},
   Volume = {76},
   Number = {12},
   Pages = {2015-2020},
   Year = {1996},
   url = {http://dx.doi.org/10.1103/PhysRevLett.76.2015},
   Abstract = {We report on the reconstruction of the decay mode B0 →
             J/ψKS0 using 19.3 pb-1 of data collected by the Collider
             Detector at Fermilab in p̄p collisions at s√ = 1.8 TeV. A
             signal of 41.8 ± 6.9 events, with a signal-to-background
             ratio of 9:1, is observed. Three additional decay modes B+
             → J/ψ K +, B0 → J/ψK* (892)0 and B+ → J/ψ K* (892)+
             are reconstructed. We measure three ratios of branching
             ratios, each one relative to the B+ → J/ψ K+ mode. We
             also report the ratio of decay rates, Γ(B → J/ψ K*)/Γ(B
             → J/ψ K), for the vector-vector relative to the
             vector-pseudoscalar modes, to be 1.32 ± 0.23(stat) ±
             0.16(syst).},
   Doi = {10.1103/PhysRevLett.76.2015},
   Key = {fds309764}
}

@article{fds309765,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cen, Y and Cervelli, F and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cunningham, JD and Daniels, T and Jongh, FD and Delchamps, S and dell'Agnello, S and dell'Orso, M and Demortier, L and Denby, B and Deninno, M and Derwent, PF and Devlin, T and Dickson, M and Dittmann,
             JR and Donati, S and Drucker, RB and Dunn, A and Einsweiler, K and Elias,
             JE and Ely, R and Jr, EE and Eno, S and Errede, D and Errede, S and Fan, Q and Farhat, B and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Frautschi, M and Freeman, J and Friedman, J and Frisch, H and Fry, A and Fuess, TA and Fukui, Y and Funaki, S and Gagliardi, G and Galeotti, S and Gallinaro, M and Garfinkel, AF and Geer, S and Gerdes, DW and Giannetti,
             P and Giokaris, N and Giromini, P and Gladney, L and Glenzinski, D and Gold, M and Gonzalez, J and Gordon, A and Goshaw, AT and Goulianos, K and Grassmann, H and Grewal, A and Groer, L and Grosso-Pilcher, C and Haber,
             C and Hahn, SR and Hamilton, R and Handler, R and Hans, RM and Hara, K and Harral, B and Harris, RM and Hauger, SA and Hauser, J and Hawk, C and Heinrich, J and Cronin-Hennessy, D and Hollebeek, R and Holloway, L and Hölscher, A and Hong, S and Houk, G and Hu, P and Huffman, BT and Hughes,
             R and Hurst, P and Huston, J and Huth, J and Hylen, J and Incagli, M and Incandela, J and Iso, H and Jensen, H and Jessop, CP and Joshi, U and Kadel, RW and Kajfasz, E and Kamon, T and Kaneko, T and Kardelis, DA and Kasha, H and Kato, Y and Keeble, L and Kennedy, RD and Kephart, R and Kesten, P and Kestenbaum, D and Keup, RM and Keutelian, H and Keyvan, F and Kim, DH and Kim, HS and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Koehn, P and Kondo, K and Konigsberg, J and Kopp, S and Kordas, K and Koska, W and Kovacs, E and Kowald, W and Krasberg, M and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Laasanen, AT and Labanca, N and Lammel, S and Lamoureux, JI and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Lockyer, N and Loomis, C and Long, O and Loreti, M and Low, EH and Lu, J and Lucchesi, D and Luchini,
             CB and Lukens, P and Lys, J and Maas, P and Maeshima, K and Maghakian, A and Maksimovic, P and Mangano, M and Mansour, J and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mattingly, R and McIntyre, P and Melese, P and Menzione, A and Meschi, E and Michail, G and Mikamo, S and Miller, M and Miller, R and Mimashi, T and Miscetti, S and Mishina, M and Mitsushio, H and Miyashita, S and Morita, Y and Moulding,
             S and Mueller, J and Mukherjee, A and Muller, T and Musgrave, P and Nakae,
             LF and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Nodulman, L and Ogawa, S and Oh, SH and Ohl, KE and Oishi, R and Okusawa,
             T and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Park, S and Patrick, J and Pauletta, G and Paulini, M and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Plunkett, R and Pondrom, L and Produit, N and Proudfoot, J and Ptohos,
             F and Punzi, G and Ragan, K and Rimondi, F and Ristori, L and Roach-Bellino, M and Robertson, WJ and Rodrigo, T and Romano, J and Rosenson, L and Sakumoto, WK and Saltzberg, D and Sansoni, A and Scarpine, V and Schindler, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schneider, O and Sciacca, GF and Scribano, A and Segler,
             S and Seidel, S and Seiya, Y and Sganos, G and Sgolacchia, A and Shapiro,
             M and Shaw, NM and Shen, Q and Shepard, PF and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Skarha, J and Sliwa, K and Smith, DA and Snider, FD and Song, L and Song, T and Spalding,
             J and Spiegel, L and Sphicas, P and Stanco, L and Steele, J and Stefanini,
             A and Strahl, K and Strait, J and Stuart, D and Sullivan, G and Sumorok, K and Swartz, RL and Takahashi, T and Takikawa, K and Tartarelli, F and Taylor, W and Teng, PK and Teramoto, Y and Tether, S and Theriot, D and Thomas, J and Thomas, TL and Thun, R and Timko, M and Tipton, P and Titov,
             A and Tkaczyk, S and Tollefson, K and Tollestrup, A and Tonnison, J and Troconiz, JFD and Tseng, J and Turcotte, M and Turini, N and Uemura, N and Ukegawa, F and Unal, G and Brink, SCVD and Vejcik, S and Vidal, R and Vondracek, M and Vucinic, D and Wagner, RG and Wagner, RL and Wainer, N and Walker, RC and Wang, C and Wang, CH and Wang, G and Wang, J and Wang, MJ and Wang, QF and Warburton, A and Watts, G and Watts, T and Webb, R and Wei, C and Wendt, C and Wenzel, H and III, WCW and Westhusing, T and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer,
             BL and Wolinski, J and Wu, DY and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Ye, Y and Yeh, GP and Yeh, P and Yin, M and Yoh, J and Yosef,
             C and Yoshida, T and Yovanovitch, D and Yu, I and Yun, JC and Zanetti, A and Zetti, F and Zhang, L and Zhang, S and Zhang, W and Zucchelli,
             S},
   Title = {Search for the rare decay W± → π
             ± + γ},
   Journal = {Physical Review Letters},
   Volume = {76},
   Number = {16},
   Pages = {2852-2857},
   Year = {1996},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.76.2852},
   Abstract = {We have searched for the rare decay W± → π± + γ in
             16.7 pb-1 of data taken in proton-antiproton collisions at
             ∫s = 1.8 TeV with the CDF detector at Fermilab. We find
             one event consistent with the expected signal, and estimate
             the background to be 2.6 ± 1.0(stat) ± 1.3(syst) events.
             Without background subtraction, we find the ratio of partial
             widths to be Γ(W± → π± + γ)/Γ(W± → e± + ν) ≤
             2.0 × 103 at the 95% confidence level.},
   Doi = {10.1103/physrevlett.76.2852},
   Key = {fds309765}
}

@article{fds309769,
   Author = {Oh, SH and Bissett, EJ and Brown, DB and Ament, F},
   Title = {Mathematical modeling of electrically heated monolith
             converters: Power and energy reduction strategies},
   Journal = {SAE Technical Papers},
   Year = {1996},
   url = {http://dx.doi.org/10.4271/961213},
   Abstract = {A transient heated converter model, coupled with vehicle
             emission testing with a prototype Park Avenue, has been used
             to develop strategies for reducing electrical power and
             energy requirements for electrically heated monolith
             converters (EHCs). The following two strategies were
             examined in detail: open-loop fuel-rich engine operation and
             use of low-thermal-mass electric heaters. It is found that
             although effective individually, a combination of these
             strategies provides even greater reductions in electrical
             power and energy requirements. For example, using a
             small-volume electric heater with fuel-rich engine
             calibration is predicted to give a 3-fold reduction in power
             and a 5-fold reduction in energy required to meet a
             cold-start HC emission target, compared to early prototype
             EHC systems operating with the baseline (fuel-lean) engine
             calibration. It is also found that a small-volume heater in
             an optimized EHC system serves primarily as a heat transfer
             medium/ignitor rather than a catalytic conversion device.
             This function of a small electric heater can be augmented by
             coupling it with an unheated "lightoff" catalyst containing
             high concentrations of noble metals. © 1996 Society of
             Automotive Engineers, Inc.},
   Doi = {10.4271/961213},
   Key = {fds309769}
}

@article{fds309768,
   Author = {Convery, M and Davis, WL and DelSignore, K and Jenkins, TL and Kangas,
             E and Knepley, M and Kowalski, KL and Taylor, CC and Wang, CH and Oh, SH and Walker, WD and Colestock, PL and Hanna, B and Martens, MA and Streets,
             JM and Ball, RC and Gustafson, HR and Jones, LW and Longo, MJ and Bjorken,
             JD and Morgan, N and Pruneau, C},
   Title = {MiniMax: What has been learned thus far},
   Journal = {Nuovo Cimento della Societa Italiana di Fisica
             C},
   Volume = {19},
   Number = {6},
   Pages = {1045-1049},
   Publisher = {Springer Nature},
   Year = {1996},
   Month = {January},
   url = {http://dx.doi.org/10.1007/BF02508149},
   Abstract = {A small experiment, «MiniMax», has been set up in the C0
             intersection region of the Fermilab Tevatron to seek
             evidence for disoriented chiral condensates and to study
             other forward physics phenomena. The experiment consists of
             a proportional wire chamber telescope accompanied by
             scintillation (trigger) counters, a lead converter, and
             followed by an electromagnetic calorimeter. The solid angle
             accepted is a cone centered at pseudorapidity (η) of 4.1
             and of radius (in η-φ space) of about 0.6. Over 2.5
             million events thus far have demonstrated the successful
             operation of the apparatus, however to date the analysis has
             not progressed sufficiently to permit any conclusions
             concerning disoriented chiral condensates.},
   Doi = {10.1007/BF02508149},
   Key = {fds309768}
}

@article{fds309770,
   Author = {Oh, SH and Wang, CH and Wesson, DK},
   Title = {High rate test of a straw drift chamber},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {369},
   Number = {1},
   Pages = {37-44},
   Publisher = {Elsevier BV},
   Year = {1996},
   Month = {January},
   url = {http://dx.doi.org/10.1016/0168-9002(95)00728-8},
   Abstract = {The response of a straw drift chamber subjected to extremely
             high rates is reported. An average background rate of up to
             10 MHz was obtained using ten 10 mCi Sr90 radioactive
             sources. We have studied the efficiency, resolution, pulse
             shape and the response of the front end electronics as a
             function of the rate. Using Monte Carlo generated data, the
             effect of pulse shadowing and electronic performance is
             studied separately.},
   Doi = {10.1016/0168-9002(95)00728-8},
   Key = {fds309770}
}

@article{fds309762,
   Author = {Abe, F and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Apollinari, G and Areti, H and Atac, M and Auchincloss, P and Azfar, F and Azzi, P and Bacchetta, N and Badgett, W and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartalini, P and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Bertolucci, S and Bhatti, A and Biery, K and Binkley, M and Bird, F and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boswell, C and Boulos, T and Brandenburg, G and Bromberg, C and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cen, Y},
   Title = {Measurement of correlated micro-b-bar jet cross sections in
             pp-bar collisions at s=1.8 TeV.},
   Journal = {Physical review. D, Particles and fields},
   Volume = {53},
   Number = {3},
   Pages = {1051-1065},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevd.53.1051},
   Abstract = {We report on measurements of differential µ-b- cross
             sections, where the muon is from a semileptonic b decay and
             the b- is identified using precision track reconstruction in
             jets. The semidifferential correlated cross sections
             dσ/(formula presented), and dσ/dδφ(µ-b-) for (formula
             presented) 10 GeV, (formula presented)<1.5 are presented and
             compared to next-to-leading order QCD calculations. © 1996
             The American Physical Society.},
   Doi = {10.1103/physrevd.53.1051},
   Key = {fds309762}
}

@article{fds309750,
   Author = {al, FAE},
   Title = {Search for gluino and squark cascade decays at the Fermilab
             tevatron collider},
   Journal = {Phys. Rev. Lett.},
   Volume = {76},
   Number = {12},
   Pages = {2006-2010},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevLett.76.2006},
   Abstract = {We report on a search for supersymmetry using dilepton
             events which complements the classic missing ET plus
             multijet analyses. Using 19pb-1 of pp collisions at √s =
             1.8TeV recorded with the Collider Detector at Fermilab we
             have searched for squarks and gluinos decaying into
             charginos and producing events with two leptons. We observe
             one candidate event. In comparison, the expected number of
             background events from standard model processes is
             2.39±0.63(stat)+0.77-0.42(syst). Hence we set limits on
             gluino and squark production based on predictions from the
             supergravity inspired minimal supersymmetric extension of
             the standard model. © 1996 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.76.2006},
   Key = {fds309750}
}

@article{fds309749,
   Author = {al, FAE},
   Title = {Search for chargino-neutralino production in p(p)over-bar
             collisions at root s=1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {76},
   Number = {23},
   Pages = {4307-4311},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevLett.76.4307},
   Abstract = {We have searched for chargino-neutralino production
             (χ±1χ02) in 1.8 TeV pp collisions, followed by their
             leptonic decays χ±1 → χ01ℓ±ν and
             χ02→χ01ℓ+ℓ-. These trilepton events are expected
             within a framework of the minimal supersymmetric standard
             model (MSSM). In a 19.1pb-1 data sample collected with a
             Collider Detector at Fermilab, no trilepton events were
             observed. Upper limits on σ(pp → χ±1χ02)BR(χ±1→02→3ℓ
             + X) were obtained for various MSSM parameter space regions,
             yielding new 95% confidence level lower limits for the
             neutralino (χ02) mass which extend as high as 49GeV/c2. ©
             1996 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.76.4307},
   Key = {fds309749}
}

@article{fds309754,
   Author = {al, FAE},
   Title = {Measurement of the B- and (B)over-bar(0) meson lifetimes
             using semileptonic decays},
   Journal = {Phys. Rev. Lett.},
   Volume = {76},
   Number = {24},
   Pages = {4462-4467},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevLett.76.4462},
   Abstract = {The lifetimes of the B- and B−0 mesons are measured using
             the partially reconstructed semileptonic decays
             B−→D1-v−X, where D is either a D0 or D*+ meson. The
             data were collected by the CDF detector at the Fermilab
             Tevatron collider during 1992-1993 and correspond to 19.3
             pb−1 of p−p collisions at s = 1.8 TeV. We measure the
             decay length distributions and find the lifetimes to be
             τ(B−) = 1.56±0.13±0.06 ps and τ(B−0) =
             1.54±0.08±0.06 ps, and the ratio of lifetimes to be
             τ(B−)/τ(B−0) = 1.01±0.11±0.02, where the first
             uncertainties are statistical and the second are systematic.
             © 1996 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.76.4462},
   Key = {fds309754}
}

@article{fds309760,
   Author = {al, FAE},
   Title = {Search for flavor-changing neutral current B meson decays in
             p(p)over-bar collisions at root s=1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {76},
   Number = {25},
   Pages = {4675-4680},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevLett.76.4675},
   Abstract = {We report on a search for the flavor-changing neutral
             current decays B0d, s→μ+μ−, B+→μ+μ−K+, and
             B0→μ+μ−K*0 using data from pp- collisions at s = 1.8
             TeV, collected with the Collider Detector at Fermilab during
             the 1992-1993 running period. We find no indication of such
             decays, and we set the following 90% confidence level upper
             limits on branching ratios: B\(B0→μ+μ−\)<1.6×10−6,
             B(B0s→μ+μ−\)<8.4×10−6, B\(B+→μ+μ−K+\)<1.0×10−5,
             and B\(B0→μ+μ−K*0\)<2.5×10−5. © 1996 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.76.4675},
   Key = {fds309760}
}

@article{fds309747,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Auchincloss, P and Azfar,
             F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov,
             S and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
             A and Berge, JP and Berryhill, J and Bertolucci, S and Bhatti, A and Biery,
             K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner,
             A},
   Title = {Search for charged Higgs boson decays of the top quark using
             hadronic tau decays.},
   Journal = {Physical review. D, Particles and fields},
   Volume = {54},
   Number = {1},
   Pages = {735-742},
   Year = {1996},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevd.54.735},
   Abstract = {We present the result of a search for charged Higgs boson
             decays of the top quark, produced in p-p collisions at
             √s=1.8 TeV. When the charged Higgs boson is heavy and
             decays to a τ lepton, which subsequently decays
             hadronically, the resulting events have a unique signature:
             large missing transverse energy and the low-charged-multiplicity
             τ. Data collected in 1992 and 1993 at the Collider Detector
             at Fermilab, corresponding to 18.7±0.7 pb-1, exclude new
             regions of combined top quark and charged Higgs boson mass,
             in extensions to the standard model with two Higgs doublets.
             © 1996 The American Physical Society.},
   Doi = {10.1103/physrevd.54.735},
   Key = {fds309747}
}

@article{fds309748,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Auchincloss, P and Azfar,
             F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov,
             S and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bortoletto,
             D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M},
   Title = {Inclusive Jet Cross Section in p-barp Collisions at sqrt
             s=1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {77},
   Number = {3},
   Pages = {438-443},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.77.438},
   Abstract = {The inclusive jet differential cross section has been
             measured for jet transverse energies, ET, from 15 to 440
             GeV, in the pseudorapidity region 0.1 [Formula preented].
             The results are based on 19.5 pb−1 of data collected by
             the CDF collaboration at the Fermilab Tevatron collider. The
             data are compared with QCD predictions for various sets of
             parton distribution functions. The cross section for jets
             with ET > 200 GeV is significantly higher than current
             predictions based on O(α3s) perturbative QCD calculations.
             Various possible explanations for the high-ET excess are
             discussed. © 1996 The American Physical
             Society.},
   Doi = {10.1103/physrevlett.77.438},
   Key = {fds309748}
}

@article{fds309757,
   Author = {al, FAE},
   Title = {Properties of jets in Z boson events from 1.8 TeV
             (p)over-bar-p collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {77},
   Number = {3},
   Pages = {448-453},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.77.448},
   Abstract = {We present a study of events with Z bosons and hadronic jets
             produced in ¯p p collisions at a center-of-mass energy of
             1.8 TeV. The data consist of 6708 Z → e+e- decays from
             106pb-1 of integrated luminosity collected using the CDF
             detector at the Fermilab Tevatron Collider. The Z+ ≥ n jet
             cross sections and jet production properties have been
             measured for n = 1 to 4. The data are compared to
             predictions of leading-order QCD matrix element calculations
             with added gluon radiation and simulated parton
             fragmentation. © 1996 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.77.448},
   Key = {fds309757}
}

@article{fds309759,
   Author = {al, FAE},
   Title = {Forward-backward charge asymmetry of electron Paris above
             the Z(0) pole},
   Journal = {Phys. Rev. Lett.},
   Volume = {77},
   Number = {13},
   Pages = {2616-2621},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.77.2616},
   Abstract = {We present a measurement of the forward-backward charge
             asymmetry of the process pp¯ → Z0/γ + X, Z0/γ →
             e+e− at Mee > MZ using 110 pb−1 of data at √ s = 1.8
             TeV collected at the Collider Detector at Fermilab. The
             measured charge asymmetries are 0.43 ± 0.10 in the
             invariant mass region Mee > 105 GeV/c2, and 0.070 ± 0.016
             in the region 75 < Mee < 105 GeV/c2. These results are
             consistent with the standard model values of 0.528 ± 0.009
             and 0.052 ± 0.002, respectively. © 1996 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.77.2616},
   Key = {fds309759}
}

@article{fds309755,
   Author = {al, FAE},
   Title = {Further properties of high-mass multijet events at the
             Fermilab proton-antiproton collider},
   Journal = {Phys. Rev. D},
   Volume = {54},
   Number = {7},
   Pages = {4221-4233},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevd.54.4221},
   Abstract = {The properties of high-mass multijet events produced at the
             Fermilab proton-antiproton collider are compared with
             leading order QCD matrix element predictions, QCD parton
             shower Monte Carlo predictions, and the predictions from a
             model in which events are distributed uniformly over the
             available multibody phase space. Multijet distributions
             corresponding to ([Formula presented]) variables that span
             the [Formula presented]-body parameter space are found to be
             well described by the QCD calculations for inclusive
             three-jet, four-jet, and five-jet events. The agreement
             between data, QCD matrix element calculations, and QCD
             parton shower Monte Carlo predictions suggests that 2→2
             scattering plus gluon radiation provides a good first
             approximation to the full LO QCD matrix element for events
             with three, four, or even five jets in the final state. ©
             1996 The American Physical Society.},
   Doi = {10.1103/physrevd.54.4221},
   Key = {fds309755}
}

@article{fds309766,
   Author = {al, YAE},
   Title = {A modular straw drift tube tracking system for the
             solenoidal detector collaboration experiment .2.
             Performance},
   Journal = {Nucl. Instr. & Meth.},
   Volume = {381},
   Number = {2-3},
   Pages = {372-384},
   Publisher = {Elsevier BV},
   Year = {1996},
   Month = {November},
   url = {http://dx.doi.org/10.1016/S0168-9002(96)00729-2},
   Abstract = {Several investigations were conducted to demonstrate the
             capabilities of a straw drift tube outer tracking system for
             the SDC detector as described in the previous article. These
             include electrical properties and aging properties of the
             tubes as well as measurements of electron drift times in a 2
             T magnetic field. Measurements characterizing the radiation
             hardness of the processes used to fabricate the front-end
             electronics are also included. We present the performance
             characteristics of prototype straw modules read out through
             this front-end electronics as well as some data on the
             performance of the track trigger system.},
   Doi = {10.1016/S0168-9002(96)00729-2},
   Key = {fds309766}
}

@article{fds309767,
   Author = {al, YAE},
   Title = {A modular straw drift tube tracking system for the
             solenoidal detector collaboration experiment .1.
             Design},
   Journal = {Nucl. Instr. & Meth.},
   Volume = {381},
   Number = {2-3},
   Pages = {355-371},
   Publisher = {Elsevier BV},
   Year = {1996},
   Month = {November},
   url = {http://dx.doi.org/10.1016/S0168-9002(96)00728-0},
   Abstract = {We have developed the baseline design for a straw drift tube
             tracking system for the Solenoidal Detector Collaboration
             (SDC) detector. The system was designed to operate in the
             high-rate environment of a high luminosity hadron collider.
             We present an overview of the tracking system and the
             requirements it was expected to fulfill. We describe the
             construction and properties of the straw drift tubes. We
             discuss the design of the carbon-fiber foam-laminate shell,
             which supported the wire tension and held the straws in
             alignment. We also present descriptions of the designs of
             the front-end and digitization electronics as well as the
             electronics associated with the level 1 track
             trigger.},
   Doi = {10.1016/S0168-9002(96)00728-0},
   Key = {fds309767}
}

@article{fds309751,
   Author = {al, FAE},
   Title = {Ratios of bottom meson branching fractions involving J/psi
             mesons and determination of b quark fragmentation
             fractions},
   Journal = {Phys. Rev. D},
   Volume = {54},
   Number = {11},
   Pages = {6596-6609},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevd.54.6596},
   Abstract = {We report a measurement of the ratios of the decay rates of
             the B+, B0, and B0s mesons into exclusive final states
             containing a J/Ψ meson. The final states were selected from
             19.6 pb-1 of pp collisions recorded by the Collider Detector
             at Fermilab. These data are interpreted to determine the b
             quark fragmentation fractions fu, fd, and fs. We also
             determine the branching fractions for the decay modes
             (formula presented). We discuss the implications of these
             measurements to B meson decay models. © 1996 The American
             Physical Society.},
   Doi = {10.1103/physrevd.54.6596},
   Key = {fds309751}
}

@article{fds309753,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro P, and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
             C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C},
   Title = {Measurement of the gamma +D*+/- Cross Section in p-barp
             Collisions at sqrt s=1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {77},
   Number = {25},
   Pages = {5005-5010},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.77.5005},
   Abstract = {We have measured the cross section of γ + D* ± production
             in pp collisions at √ = 1.8 TeV using the Collider
             Detector at Fermilab. In this kinematic region, the Compton
             scattering process (gc → γ c) is expected to dominate and
             thus provide a direct link to the charm quark density in the
             proton. From the 45 ± 18 γ + D* ± candidates in a 16.4
             pb− 1 data sample, we have determined the production cross
             section to be 0.38 ± 0.15 ± (stat) ± 0.11(syst)nb for the
             rapidity range | y(D* ±)| < 1.2 and | y (γ) | < 0.9, and
             for the transverse momentum range pT(D* ±) > 6GeV/c and 16
             < pT(γ) < 40 GeV/c. The measured cross section is compared
             to a theoretical prediction. © 1996 The American Physical
             Society.},
   Doi = {10.1103/physrevlett.77.5005},
   Key = {fds309753}
}

@article{fds330400,
   Author = {al, FAE},
   Title = {Measurement of Dijet angular distributions by the Collider
             Detector at Fermilab},
   Journal = {Phys. Rev. Lett.},
   Volume = {77},
   Number = {27},
   Pages = {5336-5341},
   Publisher = {American Physical Society (APS)},
   Year = {1996},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.77.5336},
   Abstract = {We have used 106pb of data collected in pp collisions at
             √s = 1.8 TeV by the Collider Detector at Fermilab to
             measure jet angular distributions in events with two jets in
             the final state. The angular distributions agree with next
             to leading order predictions of QCD in all dijet invariant
             mass regions. The data exclude at 95% CL a model of quark
             substructure in which only up and down quarks are composite
             and the contact interaction scale is ⩘ ≤1.6 TeV or ⩘
             ≤1.4 TeV. For a model in which all quarks are composite
             the excluded regions are ⩘ ≤1.8 TeV and ⩘ ≤1.6 TeV.
             © 1996 The American Physical Society. -1 + - + - ud
             ud},
   Doi = {10.1103/PhysRevLett.77.5336},
   Key = {fds330400}
}

@article{fds309727,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
             C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
             D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
             F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L},
   Title = {Observation of [Formula presented]→J/ψ Λ at the Fermilab
             proton-antiproton collider},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {55},
   Number = {3},
   Pages = {1142-1152},
   Year = {1997},
   Month = {January},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.55.1142},
   Abstract = {The decay [Formula presented]→J/ψ Λ is observed in 110
             [Formula presented] of pp¯ collisions taken at [Formula
             presented] TeV. These data are used to measure a Λ[Formula
             presented] mass of 5621±4(stat)±3(syst) MeV/[Formula
             presented], and a mass difference between the Λ[Formula
             presented] and the [Formula presented] of
             340±5(stat)±1(syst) MeV/[Formula presented]. The
             production cross-section times branching fraction for the
             decay [Formula presented]→J/ψ Λ relative to that for the
             decay [Formula presented]→J/ψ [Formula presented] has
             been measured to be 0.27±0.12(stat)±0.05(syst). © 1997
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.55.1142},
   Key = {fds309727}
}

@article{fds309729,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
             C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
             D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
             F and Delchamps, S and Dell’Agnello, S and Dell’Orso, M and Demina,
             R and Demortier, L},
   Title = {Measurement of [Formula presented] production correlations,
             [Formula presented] mixing, and a limit on [Formula
             presented] in [Formula presented] collisions at [Formula
             presented] TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {55},
   Number = {5},
   Pages = {2546-2558},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.55.2546},
   Abstract = {We present measurements of correlated [Formula presented]
             cross sections, [Formula presented] correlations, the
             average [Formula presented] mixing parameter [Formula
             presented], and a limit on the CP-violating parameter
             [Formula presented] For these measurements, we use muon
             pairs from [Formula presented] double semileptonic decays.
             The data used in this analysis were taken with the Collider
             Detector at Fermilab and represent an integrated luminosity
             of [Formula presented] pb[Formula presented]. The results
             concerning [Formula presented] production correlations are
             compared to predictions of next-to-leading order QCD
             computations. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.55.2546},
   Key = {fds309729}
}

@article{fds309741,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi Bacchetta and P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro Galtieri and A and Barnes, VE and Barnett, BA and Barone, M and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
             A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner,
             N and Buckley Geer and E and Budd, HS and Burkett, K and Busetto, G and Byon
             Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell,
             M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou,
             CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca,
             E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin Hennessy and D and Culbertson,
             R and Daniels, T and De Jongh and F and Delchamps, S and Dell Agnello and S and Dell Orso and M and Demina, R and Demortier, L},
   Title = {Measurement of double parton scattering in pp collisons at
             s},
   Journal = {Physical Review Letters},
   Volume = {79},
   Number = {4},
   Pages = {578-583},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.584},
   Abstract = {A strong signal for double parton scattering (DP) is
             observed in a 16 pb−1 sample of pp → γ + 3 jets + X
             data from the CDF experiment at the Fermilab Tevatron. The
             process-independent DP parameter, σ eff, is obtained
             without reference to theoretical calculations by comparing
             observed DP events to events with hard scatterings at
             separate pp collisons. The result, σ eff = (14.5 ± 1.7
             +1.7−2.3)mb, represents a significant improvement over
             previous measurements. For the first time, the Feynman x
             dependence of the σeff parameter is investigated, and no
             dependence is seen. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.79.584},
   Key = {fds309741}
}

@article{fds309744,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
             A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner,
             N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
             R and Daniels, T and De Jongh and F and Delchamps, S and Dell’agnello, S and Dell’orso, M and Demina, R and Demortier, L},
   Title = {The μτ and eτ decays of top quark pairs produced in pp¯
             collisions at √s=1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {79},
   Number = {19},
   Pages = {3585-3590},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.3585},
   Abstract = {We present a search for dilepton events from tt¯ production
             with one electron or muon and one hadronically decaying τ
             lepton from the decay tt¯→(ℓνℓ)(τντ)bbú,
             (ℓ=e,μ), using the Collider Detector at Fermilab. In a
             109pb−1 data sample of pp¯ collisions at √S=1.8TeV we
             expect ∼1 signal event and a total background of ∼2
             events; we observe 4 candidate events (2eτ and 2μτ).
             Three of these events have jets identified as b candidates,
             compared to an estimated background of 0.28±0.02 events. ©
             1997 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.79.3585},
   Key = {fds309744}
}

@article{fds309745,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and De-Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas,
             A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner,
             N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro,
             A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane, D and Cronin-Hennessy, D and Culbertson,
             R and Daniels, T and De Jongh and F and Delchamps, S and Dell’agnello, S and Dell’orso, M and Demina, R and Demortier, L},
   Title = {J/ψ and ψ(2s) Production pp collisions at √ s =
             1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {79},
   Number = {4},
   Pages = {572-577},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.572},
   Abstract = {We present a study of J/ψ and ψ(2S) production in pp
             collisons at √ s = 1.8 TeV with the CDF detector at
             Fermilab. The J/ψ and ψ(2S) mesons are reconstructed using
             their μ+μ− decay modes. We have measured the inclusive
             production cross section for both mesons as a function of
             their transverse momentum in the central region, η < 0.6.
             We also measure the fraction of these events originating
             from b hadrons. We thus extract individual cross sections
             for J/ψ and ψ 2(S) mesons from b-quark decays and prompt
             production. We find a large excess (approximately a factor
             of 50) of direct ψ(2S) production compared with predictions
             from the color singlet model. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.79.572},
   Key = {fds309745}
}

@article{fds309746,
   Author = {Brooks, TC and Convery, ME and Davis, WL and Del Signore and KW and Jenkins, TL and Kangas, E and Knepley, MG and Kowalski, KL and Taylor,
             CC and Oh, SH and Walker, WD and Colestock, PL and Hanna, B and Martens, M and Streets, J and Ball, R and Gustafson, HR and Jones, LW and Longo, MJ and Bjorken, JD and Abashian, A and Morgan, N and Pruneau,
             CA},
   Title = {Analysis of charged-particle–photon correlations in
             hadronic multiparticle production},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {55},
   Number = {9},
   Pages = {5667-5680},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.55.5667},
   Abstract = {In order to analyze data on joint charged-particle–photon
             distributions from an experimental search (T-864, MiniMax)
             for disoriented chiral condensate (DCC) at the Fermilab
             Tevatron collider, we have identified robust observables,
             ratios of normalized bivariate factorial moments, with many
             desirable properties. These include insensitivity to many
             efficiency corrections and the details of the modeling of
             the primary pion production, and sensitivity to the
             production of DCC, as opposed to the generic,
             binomial-distribution partition of pions into charged and
             neutral species. The relevant formalism is developed and
             tested in Monte Carlo simulations of the MiniMax
             experimental conditions. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.55.5667},
   Key = {fds309746}
}

@article{fds309728,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Anway-Wiese, C and Aota, S and Apollinari, G and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Badgett, W and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barzi, E and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Benlloch, J and Bensinger, J and Benton, D and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci,
             S and Bevensee, B and Bhatti, A and Biery, K and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bodek, A and Bokhari, W and Bolognesi, V and Bolla, G and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg,
             C and Bruner, N and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cammerata, J and Campagnari, C and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cen, Y and Cervelli, F and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chiarelli, G and Chikamatsu, T and Chiou, CN and Christofek, L and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Couyoumtzelis, C and Crane,
             D and Cronin-Hennessy, D and Culbertson, R and Daniels, T and DeJongh,
             F and Delchamps, S and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L},
   Title = {Measurement of bb̄ production correlations,
             B00 mixing, and a limit on
             ∈B in pp̄ collisions at √s=1.8
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {55},
   Number = {5},
   Pages = {2547-2558},
   Year = {1997},
   Month = {March},
   Abstract = {We present measurements of correlated bb̄ cross sections,
             μ-μ, correlations, the average B0B̄0 mixing parameter
             χ̄, and a limit on the CP-violating parameter ∈B. For
             these measurements, we use muon pairs from bb double
             semileptonic decays. The data used in this analysis were
             taken with the Collider_Detector at Fermilab and represent
             an integrated luminosity of 17.4±0.6 pb-1. The results
             concerning bb̄ production correlations are compared to
             predictions of next-to-leading order QCD
             computations.},
   Key = {fds309728}
}

@article{fds309726,
   Author = {al, FAE},
   Title = {Search for third generation leptoquarks in (p)over-bar-p
             collisions at root s=1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {78},
   Number = {15},
   Pages = {2906-2911},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.78.2906},
   Abstract = {We present the results of a search for third generation
             leptoquark (LQ) pairs in 110±8pb of p p collisions at
             √s=1.8TeV recorded by the Collider Detector at Fermilab.
             We assume third generation leptoquarks decay to a Τ lepton
             and a bquark with brancing ratio β. We observe one
             candidate event, consistent with standard model background
             expectations. We place upper limits on σ(p p→LQLQ )β as
             a function of the leptoquark mass M . We exclude at 95%
             confidence level scalar leptoquarks with M <99GeV/c , gauge
             vector leptoquarks with MLQ<225GeV/c , and nongauge vector
             leptoquarks with M <170GeV/c for β=1. © 1996 American
             Physical Society. ࢤ1 ¯ ¯ ¯ 2 2 2 2 LQ LQ
             LQ},
   Doi = {10.1103/PhysRevLett.78.2906},
   Key = {fds309726}
}

@article{fds309743,
   Author = {al, FAE},
   Title = {Observation of diffractive W-boson production at the
             Fermilab tevatron},
   Journal = {Phys. Rev. Lett.},
   Volume = {78},
   Number = {14},
   Pages = {2698-2703},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.78.2698},
   Abstract = {We report the first observation of diffractively produced W
             bosons.In a sample of W → eν events produced in pp
             collisions at √s=1.8TeV, we find an excess of events with
             a forward rapidity gap, which is attributed to
             diffraction.The probability that this excess is consistent
             with nondiffractive production is 1.1×10−4 (3.8σ).The
             relatively low fraction of W+ jet events observed within
             this excess implies that mainly quarks from the Pomeron,
             which mediates diffraction, participate in W production.The
             diffractive to nondiffractive W production ratio is found to
             be RW=(1.15±0.55)%.© 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.78.2698},
   Key = {fds309743}
}

@article{fds309733,
   Author = {al, FAE},
   Title = {Search for new particles decaying to dijets at
             CDF},
   Journal = {Phys. Rev. D},
   Volume = {55},
   Number = {9},
   Pages = {R5263-R5268},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.55.R5263},
   Abstract = {We have used 106 pb[Formula presented] of data collected
             with the Collider Detector at Fermilab to search for new
             particles decaying to dijets. We exclude at the 95%
             confidence level models containing the following new
             particles: axigluons and flavor universal colorons with a
             mass between 200 and 980 GeV/[Formula presented], excited
             quarks with a mass between 80 and 570 GeV/[Formula
             presented] and between 580 and 760 GeV/[Formula presented],
             color octet techni-[Formula presented]’s with a mass
             between 260 and 480 GeV/[Formula presented], [Formula
             presented] bosons with a mass between 300 and 420
             GeV/[Formula presented], and [Formula presented] diquarks
             with a mass between 290 and 420 GeV/[Formula presented]. ©
             1997 The American Physical Society.},
   Doi = {10.1103/PhysRevD.55.R5263},
   Key = {fds309733}
}

@article{fds309739,
   Author = {al, FAE},
   Title = {Search for charged Higgs boson decays of the top quark using
             hadronic decays of the tau lepton},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {3},
   Pages = {357-362},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.357},
   Abstract = {This Letter describes a direct search for charged Higgs
             boson production in proton-antiproton collisions at
             sqrt(s)=1.8 TeV recorded by the Collider Detector at
             Fermilab. Two-Higgs-doublet extensions to the standard model
             predict the existence of charged Higgs bosons. In such
             models, the branching fraction for top quarks B(t → H b
             → tau nu b) can be large. This search uses the hadronic
             decays of the tau lepton in this channel to significantly
             extend previous limits on charged Higgs production. © 1997
             The American Physical Society.},
   Doi = {10.1103/PhysRevLett.79.357},
   Key = {fds309739}
}

@article{fds309740,
   Author = {al, FAE},
   Title = {Measurement of double parton scattering in (p)over-bar-p
             collisions at root s=1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {4},
   Pages = {584-589},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.79.584},
   Abstract = {A strong signal for double parton scattering (DP) is
             observed in a 16 pb-1 sample of p̄ p → γ + 3 jets + X
             data from the CDF experiment at the Fermilab Tevatron. The
             process-independent DP parameter, σeff, is obtained without
             reference to theoretical calculations by comparing observed
             DP events to events with hard scatterings at separate p̄ p
             collisions. The result, σeff = (14.5 ± 1.7-2.3+1.7) mb,
             represents a significant improvement over previous
             measurements. For the first time, the Feynman x dependence
             of the σeff parameter is investigated, and no dependence is
             seen.},
   Doi = {10.1103/physrevlett.79.584},
   Key = {fds309740}
}

@article{fds309736,
   Author = {al, FAE},
   Title = {Search for gluinos and squarks at the Fermilab tevatron
             collider},
   Journal = {Phys. Rev. D},
   Volume = {56},
   Number = {3},
   Pages = {R1357-R1362},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.56.R1357},
   Abstract = {We report on a search for supersymmetric squark and gluino
             particles in a data sample of 19 [Formula presented] of
             [Formula presented] collisions at [Formula presented] TeV
             recorded by the Collider Detector at Fermilab. We searched
             for events containing jets plus appreciable missing
             transverse energy [Formula presented] This signature is
             indicative of pair production and subsequent decay of
             squarks and/or gluinos. After all cuts, there are [Formula
             presented] events with [Formula presented] GeV and three
             jets, and [Formula presented] events with [Formula
             presented] GeV and four jets. These numbers of events are
             consistent with estimates of standard model processes plus
             detector-induced background sources. The analysis yields
             lower limits on gluino and squark masses, based on the
             predictions from the mnimal supersymmetric extension of the
             standard model. At the [Formula presented] confidence level,
             we find gluino and squark mass limits up to 216 [Formula
             presented] assuming equal gluino and squark masses, and
             gluino mass limits up to [Formula presented] [Formula
             presented] independent of squark mass. © 1997 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.56.R1357},
   Key = {fds309736}
}

@article{fds309732,
   Author = {al, FAE},
   Title = {Limits on quark-lepton compositeness scales from dileptons
             produced in 1.8 TeV p(p)over-bar collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {12},
   Pages = {2198-2203},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.2198},
   Abstract = {The dilepton mass spectrum in pp-→|+|-+X interactions is
             studied using dielectrons (ee) and dimuons (μμ) in 100 pb-
             of data collected with the Collider Detector at Fermilab.
             The data are consistent with standard model predictions. The
             mass spectrum, being a probe for new physics, is examined
             for new interactions of quarks and leptons from a common
             composite structure. Assuming a contact interaction with the
             conventional coupling g20/4π = 1, limits on chiral
             quark-electron and quark-muon compositeness scales in the
             range of 2.5 to 4.2 TeV are obtained. © 1997 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.79.2198},
   Key = {fds309732}
}

@article{fds309734,
   Author = {al, FAE},
   Title = {Properties of six-jet events with large six-jet mass at the
             Fermilab proton-antiproton collider},
   Journal = {Phys. Rev. D},
   Volume = {56},
   Number = {5},
   Pages = {2532-2543},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.56.2532},
   Abstract = {We describe the properties of six-jet events, with the
             six-jet mass exceeding [Formula presented] produced at the
             Fermilab proton-antiproton collider operating at a
             center-of-mass energy of 1.8 TeV. Observed distributions for
             a set of 20 multijet variables are compared with predictions
             from the HERWIG QCD parton shower Monte Carlo program, the
             NJETS leading order QCD matrix element Monte Carlo program,
             and a phase-space model in which six-jet events are
             distributed uniformly over the kinematically allowed region
             of the six-body phase space. In general the QCD predictions
             provide a good description of the observed six-jet
             distributions. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.56.2532},
   Key = {fds309734}
}

@article{fds309735,
   Author = {al, FAE},
   Title = {First observation of the all-hadronic decay of t(t)over-bar
             pairs},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {11},
   Pages = {1992-1997},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.1992},
   Abstract = {We present the first observation of the all hadronic decay
             of tt― pairs. The analysis is performed using 109 pb−1
             of pp― collisions at s = 1.8 TeV collected with the
             Collider Detector at Fermilab. We observe an excess of
             events with five or more jets, including one or two b jets,
             relative to background expectations. Based on this excess we
             evaluate the production cross section to be in agreement
             with previous results. We measure the top mass to be
             186±10±12 GeV/c2. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.79.1992},
   Key = {fds309735}
}

@article{fds309738,
   Author = {al, FAE},
   Title = {Search for new gauge bosons decaying into dileptons in
             (p)over-bar-p collisions at root s=1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {12},
   Pages = {2192-2197},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.2192},
   Abstract = {We have searched for heavy neutral gauge bosons (Z') in
             dielectron and dimuon decay modes using 110pb-1 of p-p
             collisions at √s = 1.8TeV collected with the Collider
             Detector at Fermilab. We present a limit on the production
             cross section times branching ratio of a Z' mass. For mass
             MZ' > 600 GeV/c2, the upper limit is 40 fb at 95% confidence
             level. We set the lower mass limits of 690, 590, 620, 595,
             565, 630, and 600 GeV/c2 for Z'SM, ZΨ, Zψ, Zχ, ZI, ZLR,
             and ZALRM, respectively. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.79.2192},
   Key = {fds309738}
}

@article{fds309737,
   Author = {al, FAE},
   Title = {Double parton scattering in (p)over-bar-p collisions at root
             s=1.8 TeV},
   Journal = {Phys. Rev. D},
   Volume = {56},
   Number = {7},
   Pages = {3811-3832},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.56.3811},
   Abstract = {A strong signal for double parton (DP) scattering is
             observed in a [Formula presented] sample of [Formula
             presented] data from the CDF experiment at the Fermilab
             Tevatron. In DP events, two separate hard scatterings take
             place in a single [Formula presented] collision. We isolate
             a large sample of data [Formula presented] of which 53% are
             found to be DP. The process-independent parameter of double
             parton scattering, [Formula presented] is obtained without
             reference to theoretical calculations by comparing observed
             DP events to events with hard scatterings in separate
             [Formula presented] collisions. The result [Formula
             presented] represents a significant improvement over
             previous measurements, and is used to constrain simple
             models of parton spatial density. The Feynman [Formula
             presented] dependence of [Formula presented] is investigated
             and none is apparent. Further, no evidence is found for
             kinematic correlations between the two scatterings in DP
             events. © 1997 The American Physical Society.},
   Doi = {10.1103/PhysRevD.56.3811},
   Key = {fds309737}
}

@article{fds309742,
   Author = {al, FAE},
   Title = {Measurement of diffractive dijet production at the Fermilab
             Tevatron},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {14},
   Pages = {2636-2641},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.2636},
   Abstract = {We report the observation and measurement of the rate of
             diffractive dijet production at the Fermilab Tevatron p¯p
             collider at √s=1.8TeV. In events with two jets of
             ET>20GeV, 1.8<|η|<3.5, and η1η2>0, we find that the
             diffractive to nondiffractive production ratio is
             RJJ=[0.75±0.05(stat)±0.09(syst)]%. By comparing this
             result, in combination with our measured rate for
             diffractive W boson production reported previously, with
             predictions based on a hard partonic pomeron structure, we
             determine the pomeron gluon fraction to be fg=0.7±0.2. ©
             1997 American Physical Society.},
   Doi = {10.1103/PhysRevLett.79.2636},
   Key = {fds309742}
}

@article{fds309731,
   Author = {al, FAE},
   Title = {Search for new particles decaying into b(b)over-bar and
             produced in association with W bosons decaying into e nu or
             mu nu at the Fermilab Tevatron},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {20},
   Pages = {3819-3824},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.3819},
   Abstract = {We search for new particles that decay into b¯b and are
             produced with W bosons in p¯p collisions at √s = 1.8TeV.
             The search uses 109 ± 7pb-1 accumulated by the CDF
             experiment at Fermilab. We select events with an eν or
             μν, and two jets, one of them b tagged. The number of
             events and the two-jet mass distribution are consistent with
             expectations. Using W+Higgs production as a model for the
             acceptance, we set an upper limit on the production cross
             section times branching ratio for the new particle ranging
             from 14 to 19 pb (95% C.L.) as the particle mass varies from
             70 to 120GeV/c2. © 1997 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.79.3819},
   Key = {fds309731}
}

@article{fds309725,
   Author = {al, FAE},
   Title = {Search for first generation leptoquark pair production in
             p(p)over-bar collisions at root s=1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {22},
   Pages = {4327-4332},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.79.4327},
   Abstract = {We present the results of a search for first generation
             scalar leptoquarks pairs (S1S®1) in 110 ± 7 pb−1 of data
             collected by the Collider Detector at Fermilab. We assume
             both leptoquarks decay to an electron and a quark. Three
             candidate events, with masses below 140 GeV/c2 and
             consistent with background expectations, are observed. We
             obtain a 95% confidence level upper limit on the production
             cross section as a function of the leptoquark mass. Using a
             next-to-leading order calculation of S1S®1 production, we
             exclude scalar leptoquarks with mass less than 213GeV/c2 at
             95% C.L. for a branching ratio into eq equal to 1. © 1997
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.79.4327},
   Key = {fds309725}
}

@article{fds309730,
   Author = {al, FAE},
   Title = {Properties of jets in W boson events from 1.8 TeV
             (p)over-bar-p collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {79},
   Number = {24},
   Pages = {4760-4765},
   Publisher = {American Physical Society (APS)},
   Year = {1997},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.79.4760},
   Abstract = {We present a study of events with W bosons and hadronic jets
             produced in p̄p collisions at a center of mass energy of
             1.8 TeV. The data consist of 51 400 W± → e± decay
             candidates from 108 pb-1 of integrated luminosity collected
             using the CDF detector at the Fermilab Tevatron Collider.
             Cross sections and jet production properties have been
             measured for W + ≥1 to ≥4 jet events. The data are
             compared to predictions of leading-order QCD matrix element
             calculations with added gluon radiation and simulated parton
             fragmentation.},
   Doi = {10.1103/physrevlett.79.4760},
   Key = {fds309730}
}

@article{fds313339,
   Author = {Collaboration, CDF},
   Title = {Search for the Rare Decay W+,->D+ pp in Collisions at „©
             s= 1.8 TeV},
   Journal = {Phys. Rev.},
   Volume = {D58},
   Number = {9},
   Pages = {5},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.091101},
   Abstract = {We search for the rare decay [Formula Presented] in [Formula
             Presented] of [Formula Presented] collisions recorded with
             the Collider Detector at Fermilab. At the 95% confidence
             level, we find an upper limit on the relative branching
             fraction to be [Formula Presented]. © 1998 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.58.091101},
   Key = {fds313339}
}

@article{fds332117,
   Author = {Collaboration, CDF},
   Title = {Search for the Rare Decay W+ ->ƒà+ + ƒ× in
             Proton-Antiproton Collisions at = 1.8 TeV},
   Journal = {Phys. Rev. Rapid Communications},
   Volume = {D58},
   Number = {3},
   Pages = {031101},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.031101},
   Abstract = {We have searched for the rare decay [Formula Presented] in
             [Formula Presented] of data taken in proton-antiproton
             collisions at [Formula Presented] with the Collider Detector
             at Fermilab. We find three events in the signal region and
             estimate the background to be 5.2±1.5 events. We set a 95%
             confidence level upper limit of [Formula Presented] on the
             ratio of partial widths, [Formula Presented]. © 1998 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.58.031101},
   Key = {fds332117}
}

@article{fds313354,
   Author = {al, FAE},
   Title = {``Observation of $B_{c}$ Mesons in $p\overline p$ Collisions
             at $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review},
   Volume = {D58},
   Number = {11},
   Pages = {112004},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.112004},
   Abstract = {We report the observation of bottom-charmed mesons [Formula
             Presented] in 1.8 TeV [Formula Presented] collisions using
             the CDF detector at the Fermilab Tevatron. The [Formula
             Presented] mesons were found through their semileptonic
             decays, [Formula Presented] A fit to the [Formula Presented]
             mass distribution yielded [Formula Presented] events from
             [Formula Presented] mesons. A test of the null hypothesis,
             i.e., an attempt to fit the data with background alone, was
             rejected at the level of 4.8 standard deviations. By
             studying the quality of the fit as a function of the assumed
             [Formula Presented] mass, we determined [Formula Presented]
             From the distribution of trilepton intersection points in
             the plane transverse to the beam direction we measured the
             [Formula Presented] lifetime to be [Formula Presented] We
             also measured the ratio of production cross section times
             branching fraction for [Formula Presented] relative to that
             for [Formula Presented] to be [Formula Presented] © 1998
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.58.112004},
   Key = {fds313354}
}

@article{fds309696,
   Author = {al, FAE},
   Title = {``Measurement of $B$ Hadron Lifetimes Using J/$\psi$ final
             States at CDF,''},
   Journal = {Physical Review},
   Volume = {D57},
   Number = {9},
   Pages = {5382},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.57.5382},
   Abstract = {The average bottom-hadron and individual (Formula
             presented), (Formula presented), and (Formula presented)
             meson lifetimes have been determined using decays with a
             (Formula presented) in the final state. The data sample
             consists of 110 pb(Formula presented) of (Formula presented)
             collisions at (Formula presented) TeV collected by the CDF
             detector at the Fermilab Tevatron collider during
             1992–1995. For the average lifetime of (Formula presented)
             hadrons decaying into (Formula presented)+X, we obtain
             (Formula presented) For the (Formula presented) and (Formula
             presented) meson lifetimes, we determine (Formula presented)
             (Formula presented) and (Formula presented) For the (Formula
             presented) meson lifetime, we find (Formula presented) ps.
             © 1998 The American Physical Society.},
   Doi = {10.1103/PhysRevD.57.5382},
   Key = {fds309696}
}

@article{fds309698,
   Author = {al, FAE},
   Title = {Search for Higgs Bosons Produced in Association with a
             Vector Boson in pp collisions at $\sqrt{s} = 1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {26},
   Pages = {5748},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.5748},
   Abstract = {We search for Higgs bosons produced in association with a
             massive vector boson in 91±7pb-1 of pp collisions at √s =
             1.8TeV recorded by the Collider Detector at Fermilab. We
             assume the Higgs scalar H0 decays to a bb pair with
             branching ratio β, and we consider the hadronic decays of
             the vector boson V (W or Z). Observations are consistent
             with background expectations. We place 95% confidence level
             upper limits on σ(pp → H0V)β as a function of the scalar
             mass (MH0) over the range 70 < MH0 < 140GeV/c2. When
             combined with an analysis of the case where V is a
             leptonically decaying W, these limits vary from 23 pb at MH0
             = 70GeV/c2 to 17 pb at MH0 = 140GeV/c2. © 1998 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.81.5748},
   Key = {fds309698}
}

@article{fds309699,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla,
             G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
             S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
             B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
             H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
             O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti,
             G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
             R and Handa, T and Handler, R and Happacher, F and Hao, W and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Hohlmann,
             M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
             BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins,
             D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch,
             L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo,
             K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald,
             W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
             JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
             S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin,
             A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
             S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
             KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
             A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
             L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang,
             CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Search for the decays Bs0,
             Bd0 → e±μ
             and Pati-Salam leptoquarks},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {26},
   Pages = {5742-5747},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.5742},
   Abstract = {We have searched for the decays Bs0 → e±μ∓ and Bd0 →
             e±μ∓ using a 102 pb-1 data sample of pp̄ collisions at
             √s = 1.8 TeV collected with the Collider Detector at
             Fermilab. We set upper limits on the branching fractions of
             B(Bs0 → e±μ∓) &lt; 6.1(8.2) × 10-6 and B(Bs0 →
             e±μ∓) &lt; 3.5(4.5) × 10-6 at 90(95)% confidence level.
             Using these limits, we set lower bounds on the corresponding
             Pati-Salam leptoquark masses and find that MLQ(BS0) &gt;
             20.7(19.3) TeV/c2 and MLQ(Bd0) &gt; 21.7(20.4) TeV/c2 at
             90(95)% confidence level.},
   Doi = {10.1103/PhysRevLett.81.5742},
   Key = {fds309699}
}

@article{fds309700,
   Author = {al, FAE},
   Title = {``Events with a Rapidity Gap Between Jets in $p\overline p$
             Collisions at $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {24},
   Pages = {5278},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.5278},
   Abstract = {We report a measurement of the fraction of dijet events with
             a rapidity gap between jets produced by color-singlet
             exchange in p̄p collisions at √S = 630 GeV at the
             Fermilab Tevatron. In events with two jets of transverse
             energy ETjet &gt; 8 GeV, pseudorapidity in the range 1.8
             &lt; |ηjet| &lt; 3.5 and η1η2 &lt; 0, the color-singlet
             exchange fraction is found to be R = [2.7 ± 0.7(stat) ±
             0.6(syst)]%. Comparisons are made with results obtained at
             √s = 1800 GeV and with theoretical expectations.},
   Doi = {10.1103/PhysRevLett.81.5278},
   Key = {fds309700}
}

@article{fds309701,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
             AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch, H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
             DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
             M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handa,
             T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris,
             RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
             U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
             J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Nakano, I and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu,
             YC and Lockyer, N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews,
             JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
             KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
             A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg,
             D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith,
             C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella,
             F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka, M and Tannenbaum,
             B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto,
             Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk,
             W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal,
             R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson,
             R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Search for the rare decay W± →
             Dsplusmnγ in pp̄ collisions at √s
             = 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {9},
   Pages = {911011-911015},
   Year = {1998},
   Key = {fds309701}
}

@article{fds309702,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
             AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
             DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
             M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton, R and Handa,
             T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris,
             RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
             U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
             J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster,
             M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
             N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
             SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
             TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
             A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
             MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
             A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
             K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
             R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
             M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar,
             R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of the B- and B̄0meson
             lifetimes using semileptonic decays},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {9},
   Pages = {920021-9200212},
   Year = {1998},
   Abstract = {The lifetimes of the B- and B̄0 mesons are measured using
             the partially reconstructed semileptonic decays B̄ → Dl-
             v̄X, where D0 is either a D0 or D*+ meson. The data were
             collected by the CDF detector at the Fermilab Tevatron
             collider during 1992-1995 and correspond to about 110 pb-1
             of pp collisions at √s = 1.8 TeV. We measure decay lengths
             and extract the lifetimes to be τ(B-) =
             1.637±0.058-0.043+0.045 ps and τ(B̄0) =
             1.474±0.039-0.051+0.052 ps, and the ratio of the lifetimes
             to be τ(B-)/τ(B̄0) = 1.110±0.056-0.030+0.033, where the
             first uncertainties are statistical and the second are
             systematic.},
   Key = {fds309702}
}

@article{fds309703,
   Author = {al, FAE},
   Title = {Measurement of the Lepton Charge Asymmetry in W-Boson Decays
             Produced in pp Collisions},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {26},
   Pages = {5754},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.5754},
   Abstract = {We describe a measurement of the charge asymmetry of leptons
             from W-boson decays in the rapidity range 0 < |yl| < 2.5
             using W → eν,μν events from 110±7pb-1 of data
             collected by the CDF detector during 1992–1995. The
             asymmetry data constrain the ratio of d and u quark momentum
             distributions in the proton over the x range of 0.006 to
             0.34 at Q2 ≈ M2W. The asymmetry predictions that use
             parton distribution functions obtained from previously
             published CDF data in the central rapidity region (0.0 <
             |yl| < 1.1) do not agree with the new data in the large
             rapidity region (|yl| > 1.1). © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.81.5754},
   Key = {fds309703}
}

@article{fds309704,
   Author = {Collboration, CDF},
   Title = {Measurement of the _(W +> 1 Jet)/_ (W) Cross Section Ratio
             from pp Collisions at „© s = 1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {81},
   Number = {7},
   Pages = {1367},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.1367},
   Abstract = {The ratio of the W + ≥ 1 jet cross section to the
             inclusive W cross section is measured using W±→ e±v
             events from p¯p collisions at √ = 1.8 TeV. The data are
             from 108pb−1 of integrated luminosity collected with the
             Collider Detector at Fermilab. Measurements of the cross
             section ratio for jet transverse energy thresholds(EminT)
             ranging from 15 to 95 GeV are compared to theoretical
             predictions using next-to-leading-order QCD calculations.
             Data and theory agree well for EminT > 25 GeV, where the
             predictions lie within 1 standard deviation of the measured
             values. © 1998 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.81.1367},
   Key = {fds309704}
}

@article{fds309705,
   Author = {al, FAE},
   Title = {``Measurement of the Top Quark Mass,''},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {13},
   Pages = {2767},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.2767},
   Abstract = {We present a measurement of the top quark mass using a
             sample of tt decays into an electron or a muon, a neutrino,
             and four jets. The data were collected in pp collisions at
             √s = 1.8TeV with the Collider Detector at Fermilab and
             correspond to an integrated luminosity of 109pb−1. We
             measure the top quark mass to be 175.9±4.8(stat)
             ±4.9(syst)GeV/c2. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.80.2767},
   Key = {fds309705}
}

@article{fds309706,
   Author = {al, FAE},
   Title = {``Measurement of the Differential Cross Section for Events
             with Large Total Transverse Energy in $p\overline p$
             Collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {16},
   Pages = {3461},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.3461},
   Abstract = {We present a measurement of the differential cross section
             dσ/dΣEjetT for the production of multijet events in pp
             collisions where the sum is over all jets with transverse
             energy EjetT > EminT. The measured cross section for events
             with EjetT > 320 GeV is compared to O(α3s) perturbative QCD
             predictions and QCD parton shower Monte Carlo predictions.
             The agreement between the O(α3s) predicted and observed
             event rates is reasonable for EminT = 100 GeV, but poorer
             for EminT = 20 GeV. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.80.3461},
   Key = {fds309706}
}

@article{fds309707,
   Author = {Collaboration, CDF},
   Title = {Observation of the Bc Meson in pp Collisions at „© s =
             1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {81},
   Number = {12},
   Pages = {2432},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.2432},
   Abstract = {We have observed bottom-charm mesons via the decay mode B±c
             → J/ψl±ν in 1.8 TeV pp¯ collisions using the CDF
             detector at the Fermilab Tevatron. A fit of background and
             signal contributions to the J/ψl mass distribution yielded
             20.4+6.2-5.5 events from Bc mesons. A fit to the same
             distribution with background alone was rejected at the level
             of 4.8 standard deviations. We measured the B+c mass to be
             6.40 ± 0.39(stat) ± 0.13(syst) GeV/c2 and the B+c lifetime
             to be 0.46+0.18-0.16(stat) ± 0.03(syst)ps. Our measured
             yield (production cross section times branching ratio) for
             B±c → J/ψl+ν relative to that for B+ → J/ψK+ is
             0.132+0.041-0.037(stat) ± 0.031(syst)+0.032-0.020(lifetime).
             © 1998 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.81.2432},
   Key = {fds309707}
}

@article{fds309708,
   Author = {al, FAE},
   Title = {``Search for Second Generation Leptoquarks in the Dimuon
             plus Dijet Channel of $p\overline p$ Collisions at $\sqrt{s}
             = 1.8$ TeV,"},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {22},
   Pages = {4806},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.4806},
   Abstract = {We report on a search for second generation leptoquarks(Φ2)
             using a data sample corresponding to an integrated
             luminosity of 110 pb−1 collected at the Collider Detector
             at Fermilab. We present upper limits on the production cross
             section as a function of Φ2 mass, assuming that the
             leptoquarks are produced in pairs and decay into a muon and
             a quark with branching ratio MΦ2 > 202(160)GeV/c2 at 95%
             confidence level for scalar leptoquarks with β = 1(0.5). ©
             1998 American Physical Society.},
   Doi = {10.1103/PhysRevLett.81.4806},
   Key = {fds309708}
}

@article{fds309709,
   Author = {Collaboration, CDF},
   Title = {Search for Chargino-Neutralino Associated Production at the
             Fermilab Tevatron Collider},
   Journal = {Phys. Rev. Lett.},
   Volume = {80},
   Number = {13},
   Pages = {5275},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.5275},
   Abstract = {We have searched in pp collisions at √s=1.8TeV for events
             with three charged leptons and missing transverse energy. In
             the minimal supersymmetric standard model, we expect
             trilepton events from chargino-neutralino (√ √ ) pair
             production, with subsequent decay into leptons. We observe
             no candidate e e e , e e μ , e μ μ , or μ μ μ events
             in 106pb integrated luminosity. We present limits on the sum
             of the branching ratios times cross section for the four
             channels: σ χ B(χ χ →3ℓ+X)<0.34pb, M χ81.5GeV/c ,
             and M >82.2GeV/c for tan >=2, μ=-600GeV/c , and M =M . ©
             1998 The American Physical Society. ± 0 + - ± + - ± ± +
             - + - ± -1 ± 0 ± 0 ± 2 0 2 2 1 2 σ 1 2 1 2 χ 1 χ 2 q
             g},
   Doi = {10.1103/PhysRevLett.80.5275},
   Key = {fds309709}
}

@article{fds309711,
   Author = {Collaboration, CDF},
   Title = {Searches for New Physics in Diphoton Events in pp at „©s
             = 1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {81},
   Number = {9},
   Pages = {1791},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.1791},
   Abstract = {We have searched for anomalous production of missing ET(ET),
             jets, leptons (e, μ, τ), bquarks, or additional photons in
             events containing two isolated, central (|η| < 1.0) photons
             with ET > 12GeV. The results are consistent with standard
             model expectations, with the possible exception of one event
             that has in addition to the two photons a central electron,
             a high-ET electromagnetic cluster, and large ET. We set
             limits using two specific supersymmetry scenarios for
             production of diphoton events with ET. © 1998 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.81.1791},
   Key = {fds309711}
}

@article{fds309712,
   Author = {al, FAE},
   Title = {Measurement of the CP-Violation Parameter sin(2B) in B0d/B0d
             -> J/PsiK0s Decays},
   Journal = {Physical Review Letters},
   Volume = {81},
   Number = {25},
   Pages = {5513},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.81.5513},
   Abstract = {We present a measurement of the time-dependent asymmetry in
             the rate for B̄d0 versus Bd0 decays to J/ψ KS0. A nonzero
             asymmetry would be an indication of CP violation, and within
             the standard model this may be used to measure the
             CP-violation parameter sin(2β). A total of 198 ± 17
             Bd0/B̄d0 decays were observed in pp̄ collisions at √s =
             1.8 TeV by the CDF detector at the Fermilab Tevatron. Bd0
             and B̄d0 are distinguished by a technique based on charge
             correlations from hadronization of the b quark. Our analysis
             results in sin(2β) = 1.8 ± 1.1(stat) ±
             0.3(syst).},
   Doi = {10.1103/PhysRevLett.81.5513},
   Key = {fds309712}
}

@article{fds309713,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
             AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
             C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
             L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
             O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi,
             E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukheņee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
             SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
             TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
             A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
             MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
             A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
             K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
             R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
             M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and Vejcik, S and Velev, G and Vidal, R and Vilar,
             R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Observation of Bc mesons in pp̄ collisions at
             √s = 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {11},
   Pages = {1120041+11200429},
   Year = {1998},
   Abstract = {We report the observation of bottom-charmed mesons Bc ni 1.8
             TeV pp̄ collisions using the CDF detector at the Fermilab
             Tevatron. The Bc mesons were found through their
             semileptonic decays, B±c → J/ψl± X. A fit to the J/ψl
             mass distribution yielded 20.4+6.2-5.5 events from Bc
             mesons. A test of the null hypothesis, i.e., an attempt to
             fit the data with background alone, was rejected at the
             level of 4.8 standard deviations. By studying the quality of
             the fit as a function of the assumed Bc mass, we determined
             M(Bc) = 6.40 ±0.39 (stat.)±0.13 (syst) GeV/c2. From the
             distribution of trilepton intersection points in the plane
             transverse to the beam direction we measure the Bc lifetime
             to be τ(Bc) = 0.46+0.18-0.16 (stat)±0.03 (syst) ps. We
             also measured the ratio of production cross section times
             branching fraction for B+c → J/ψl+ v relative to that for
             B+ → J/ψK+ to be σ(Bc)×B(B c→J/ψlv)/σ(B)×B(B→J/ψK)
             = 0.132+0.041-0.037 (stat)±0.031 (syst)+0.032-0.020(lifetime).},
   Key = {fds309713}
}

@article{fds309714,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
             AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
             C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
             L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Nakano, I and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and Compte, TL and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
             N and Long, O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
             KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
             A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg,
             D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith,
             C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella,
             F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka, M and Tannenbaum,
             B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto,
             Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk,
             W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal,
             R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson,
             R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Observation of B+ → ψ(2S)K+ and
             B0 → ψ(2S)K*(892)0 decays and
             measurements of B-meson branching fractions into J/ ψ and
             ψ(2S) final states},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {58},
   Number = {7},
   Pages = {720011-720012+7200115},
   Year = {1998},
   Abstract = {We report the observations of the decays B+ → ψ(2S)K+ and
             B0 → ψ(2S)K*(892)0 in pp̄ collisions at a center-of-mass
             energy of 1.8 TeV using a 110 pb-1 data sample recorded by
             the Collider Detector at Fermilab. We also reconstruct the
             decays B+ → J/ψK+ and B0 → J/ψK*(892)0 and measure the
             six ratios of branching fractions of these four decays. The
             relative branching-fraction results are shown to be
             consistent with phenomenological factorization calculations
             of hadronic B-meson decays. We use the world-average
             branching fraction ℬ(B+ → J/ψK+) to derive ℬ(B+ →
             ψ(2S)K+) = (0.56±0.08±0.10) × 10-3, ℬ(B0 →
             ψ(2S)K*(892)0) = (0.92±0.20±0.16) × 10-3, and ℬ(B0 →
             J/ψK*(892)0) = (1.78±0.14±0.29) × 10-3, where the first
             and second uncertainties are statistical and systematic,
             respectively.},
   Key = {fds309714}
}

@article{fds309715,
   Author = {al, FAE},
   Title = {``Measurement of the $B^0$-$\overline B^0$ Oscillation
             Frequency Using $\pi$-$B$ Meson Charge-Flavor Correlations
             in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,''},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {10},
   Pages = {2057},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.2057},
   Abstract = {We present a measurement of the B0 ↔ B̄0 oscillalion
             frequency using a flavor tagging method based on
             correlations of B meson flavor with the charge of other
             particles produced in pp̄ collisions at √s = 1.8 TeV.
             Such correlations are expected to arise from b quark
             hudronization and from B** decays. We partially reconstruct
             B mesons using the semileptonic decays B0 → D(*)-X and B+
             rarr; -D̄0X. From the oscillation frequency, we obtain the
             mass difference between the two B0 mass eigenstates. Δmd =
             0.471 -0.068+0.078(stat) ± 0.034(syst)ℏ ps-1, and measure
             the efficiency and purity of this flavor tagging method for
             both charged and neutral B mesons.},
   Doi = {10.1103/PhysRevLett.80.2057},
   Key = {fds309715}
}

@article{fds309716,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal,
             M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli,
             M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and III, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
             C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
             L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Nakano, I and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and Compte, TL and Leone, S and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
             O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martin, A and Matthews, JAJ and Mazzanti, P and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi,
             E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Nakada, H and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pondrom,
             L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
             L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang,
             CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Search for the decays B0d→μ+μ-
             and B0s→μ+μ-
             in pp̄ collisions at √s=1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {57},
   Number = {7},
   Pages = {R3811-R3816},
   Year = {1998},
   Abstract = {We present a search for the flavor-changing neutral current
             decays B0d→μ+μ- and B0s→μ+μ- in pp̄ collisions at
             √s=1.8 TeV, using 98 pb-1 of data collected at the
             Collider Detector at Fermilab. We find one candidate event
             for these decays, which is consistent with the background
             estimates, and set upper limits on the branching fractions
             of ℬ(B0d→μ+μ -)&lt;8.6×10-7 and ℬ(B0s→μ+μ
             -)&lt;2.6×10-6 at 95% confidence level.},
   Key = {fds309716}
}

@article{fds309718,
   Author = {al, FAE},
   Title = {Dijet Production by Color-Singlet Exchange at the Fermilab
             Tevatron},
   Journal = {Phys. Rev. Lett.},
   Volume = {80},
   Number = {6},
   Pages = {1156},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.1156},
   Abstract = {We report a new measurement of dijet production by
             color-singlet exchange in pp® collisions at √s = 1.8 TeV
             at the Fermilab Tevatron. In a sample of events with two
             jets of transverse energy EjetT > 20 GeV, pseudorapidity in
             the range 1.8 < |ηjet| < 3.5, and η1η2 < 0, we find that
             a fraction R = [1.13 ± 0.12(stat) ± 0.11(syst)]% has a
             pseudorapidity gap within |η| < 1 between the jets that can
             be attributed to color-singlet exchnage. The fraction R
             shows no significant dependence on EjetT or on the
             pseudorapidity separation between the jets. © 1998 American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.80.1156},
   Key = {fds309718}
}

@article{fds309719,
   Author = {al, FAE},
   Title = {``Search for Flavor-Changing Neutral Current Decays of the
             Top Quark in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,''},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {12},
   Pages = {2525},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.2525},
   Abstract = {We search for the flavor-changing neutral current decays of
             the top quark t → λ and t → qZ (here represents the c
             and u quarks) in pp collisions at √s = 1.8 TeV. We use a
             dataset (∫ L dt˜ 110pb-1) collected during the 1992-1995
             run of the Collider Detector at Fermilab. We set 95%
             confidence level limits on the branching fractions B(t →
             qλ) < 3.2% and B(t → qZ) < 33%, consistent with the
             standard model. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.80.2525},
   Key = {fds309719}
}

@article{fds309720,
   Author = {al, FAE},
   Title = {``Properties of Photon Plus Two-Jet Events in $\overline pp$
             Collisions at $\sqrt s$ =1.8 TeV,''},
   Journal = {Physical Review},
   Volume = {D57},
   Number = {1},
   Pages = {67},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.57.67},
   Abstract = {We present the first general measurements (invariant-mass,
             transverse-energy, and angular distributions) of the
             process, (Formula presented) (Formula presented) using data
             collected by the CDF at Fermilab. We compare the data with
             predictions from a tree-level QCD calculation and the PYTHIA
             shower Monte Carlo program. Our data sample is particularly
             sensitive to contributions from initial- and final-state
             radiation of photons and jets. Using the PYTHIA Monte Carlo
             program, we contrast the kinematical distributions for
             direct photon production with those for initial- and
             final-state photon radiation (bremsstrahlung). Based on the
             angular distributions, we find that our data favor a mixture
             of bremsstrahlung and direct photon production, as
             predicted, over either process alone. © 1998 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.57.67},
   Key = {fds309720}
}

@article{fds309721,
   Author = {al, FAE},
   Title = {``Jet Pseudorapidity Distribution in Direct Photon Events in
             $\overline pp$ Collisions at $\sqrt s$ =1.8
             TeV,''},
   Journal = {Physical Review},
   Volume = {D57},
   Number = {3},
   Pages = {1359},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.57.1359},
   Abstract = {We present the first measurement of the jet pseudorapidity
             distribution in direct photon events from a sample of
             (Formula presented) collisions at (Formula presented)
             recorded with the Collider Detector at Fermilab. Quantum
             chromodynamics (QCD) predicts that these events are
             primarily from hard quark-gluon Compton scattering, (Formula
             presented) with the final state quark producing the jet of
             hadrons. The jet pseudorapidity distribution in this model
             is sensitive to parton momentum fractions between 0.015 and
             0.15. We find that the shape of the measured pseudorapidity
             distribution agrees well with next-to-leading order QCD
             calculations. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.57.1359},
   Key = {fds309721}
}

@article{fds309724,
   Author = {Oh, SH and Sinkevitch, RM and Baker, JA and Nichols,
             GE},
   Title = {Use of catalytic monoliths for on-road ozone
             destruction},
   Journal = {SAE Technical Papers},
   Year = {1998},
   url = {http://dx.doi.org/10.4271/980677},
   Abstract = {The automotive clean-air catalyst system from Engelhard
             Corporation (PremAir™) consists of a catalyst-coated
             vehicle radiator and air-conditioning condenser designed to
             catalytically remove ground-level ozone and carbon monoxide
             (CO) from ambient air. Although initial on-road testing of
             the PremAir™ system showed reasonably high ozone
             conversion activity and satisfactory catalyst durability
             during the course of relatively low mileage accumulation,
             the long-term durability of the catalyst coating, its
             potential negative impact on cooling efficiency and
             corrosion characteristics, and incompatibility with the
             existing radiator manufacturing process remain among the
             issues of some concern. This paper describes an alternative
             approach to the problem of on-road pollutant destruction,
             which involves placing a thin catalytic monolith brick
             immediately behind the uncoated vehicle radiator. The ozone
             and CO conversion performance of the alternative clean-air
             catalyst system was evaluated on a Delphi-Harrison Thermal
             Systems' dissipator and compared with that of
             catalyst-coated radiator cores. The tests show the superior
             ozone conversion performance of the catalytic monoliths (but
             at the expense of higher pressure drop) compared to the
             catalyzed radiator cores. A simple mathematical analysis of
             the ozone conversion data indicates that the ozone
             conversion reaction over both the catalytic monoliths and
             catalyzed radiators occurs under the influence of
             significant mass transfer limitations, and that the ozone
             destruction performance advantage of the catalytic monoliths
             can be attributed to their higher gas-solid mass transfer
             rate. The CO conversion efficiencies observed with both
             types of catalyst samples were too low (&lt; 10 %) to draw
             definite conclusions about the impact of catalyst system
             configuration on CO conversion performance. Copyright ©
             1998 Society of Automotive Engineers, Inc.},
   Doi = {10.4271/980677},
   Key = {fds309724}
}

@article{fds313343,
   Author = {al, FAE},
   Title = {``Measurement of the $B^-$ and $\overline B^0$ Meson
             Lifetimes using Semileptonic Decays,"},
   Journal = {Physical Review},
   Volume = {D58},
   Number = {3},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.59.032004},
   Abstract = {The lifetime of the [Formula Presented] meson is measured
             using the semileptonic decay [Formula Presented] The data
             sample consists of about [Formula Presented] of [Formula
             Presented] collisions at [Formula Presented] collected by
             the CDF detector at Fermilab. Four different [Formula
             Presented] decay modes are reconstructed resulting in
             approximately 600 [Formula Presented] signal events. The
             [Formula Presented] meson lifetime is determined to be
             [Formula Presented] where the first and second uncertainties
             are statistical and systematic, respectively. The [Formula
             Presented] meson decay length distribution is examined for a
             lifetime difference [Formula Presented] between the two mass
             eigenstates of the [Formula Presented] meson. An upper limit
             of ΔΓ/Γ<0.83 is set at the 95% confidence level. © 1999
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.59.032004},
   Key = {fds313343}
}

@article{fds313365,
   Author = {Collaboration, CDF},
   Title = {Search for the Decays B^0->____ and B^0-> ___ in pp
             Collisions at „©s = 1.8 TeV},
   Journal = {Phys. Rev. Rapid Communications},
   Volume = {D57},
   Number = {7},
   Pages = {R3811},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.57.R3811},
   Abstract = {We present a search for the flavor-changing neutral current
             decays (Formula presented) and (Formula presented) in
             (Formula presented) collisions at (Formula presented) TeV,
             using (Formula presented) of data collected at the Collider
             Detector at Fermilab. We find one candidate event for these
             decays, which is consistent with the background estimates,
             and set upper limits on the branching fractions of (Formula
             presented) and (Formula presented) at 95% confidence level.
             © 1998 The American Physical Society.},
   Doi = {10.1103/PhysRevD.57.R3811},
   Key = {fds313365}
}

@article{fds313353,
   Author = {al, FAE},
   Title = {``Search for Long-Lived Parents of $Z^{0}$ Bosons in
             $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,"},
   Journal = {Physical Review},
   Volume = {D58},
   Number = {5},
   Pages = {051102},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.051102},
   Abstract = {We search for new long-lived particles which decay to
             [Formula Presented] bosons by looking for [Formula
             Presented] decays with displaced vertices. We find no
             evidence for parent particles of the [Formula Presented]
             with long lifetimes in [Formula Presented] of data from the
             CDF experiment at Fermilab. We set a cross section limit as
             a function of the lifetime of the parent particle for both a
             generic [Formula Presented] parent and a fourth-generation,
             charge [Formula Presented] quark that decays into [Formula
             Presented]. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.58.051102},
   Key = {fds313353}
}

@article{fds357485,
   Author = {al, FAE},
   Title = {``Observation of $B^{+}\rightarrow\psi$(2S)$K^{+}$ and
             $B^{0}\rightarrow\psi(2S)K^{*}(892)^{0}$ Decays and
             Measurements of $B$-Meson Branching Fractions into $J/\psi$
             and $\psi$(2S) Final States,"},
   Journal = {Physical Review},
   Volume = {D58},
   Number = {7},
   Pages = {112004},
   Year = {1998},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.072001},
   Doi = {10.1103/PhysRevD.58.072001},
   Key = {fds357485}
}

@article{fds309697,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Baccehtta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and De Barbaro and P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Chigangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and De Jongh and F and Dell’agnello, S and Dell’orso, M and Demina, R and Demortier, L},
   Title = {Measurement of the top quark mass and t¯t production cross
             section from dilepton events at the collider detector at
             fermilab},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {13},
   Pages = {2779-2784},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.2779},
   Abstract = {We present an analysis of dilepton events originating from
             t¯t production in p¯p collisions at √s = 1.8TeV at the
             Fermilab Tevatron Collider. The sample corresponds to an
             integrated luminosity of 109 ± 7pb-1. We observe nine
             candidate events, with an estimated background of 2.4 ± 0.5
             events. We determine the mass of the top quark to be Mtop =
             161 ± 17(stat) ± 10(syst)GeV/c2. In addition, we measure a
             t¯t production cross section of 8.2+4.4-3.4pb (where Mtop =
             175GeV/c2 has been assumed for the acceptance estimate). ©
             1998 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.80.2779},
   Key = {fds309697}
}

@article{fds309710,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and De Barbara and P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
             AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and Dejongh, F and Dell'Agnello, S and Dell'Orso, M},
   Title = {Search for long-lived parents of Z° bosons inpp collisions
             at √s = 1.8 TeV},
   Journal = {Physical Review D},
   Volume = {58},
   Number = {5},
   Pages = {511021-511025},
   Year = {1998},
   Month = {January},
   Abstract = {We search for new long-lived particles which decay to Z0
             bosons by looking for Z0→e+e- decays with displaced
             vertices. We find no evidence for parent particles pf the Z0
             with long lifetimes in 90 pb-1 of data from the CDF
             experiment at Fermilab. We set a cross section limit as a
             function of the lifetime of the parent particle for both a
             generic Z0 parent and a fourth-generation, charge -1/3 quark
             that decays into Z0b. © 1998 The American Physical
             Society.},
   Key = {fds309710}
}

@article{fds309717,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and De Barbaro and P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
             C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti,
             R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers,
             W and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and De Jongh and F and Dell’agnello, S and Dell’orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF},
   Title = {Measurement of the t¯t Production Cross Section in p¯p
             Collisions at √s = 1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {80},
   Number = {13},
   Pages = {2773-2778},
   Publisher = {American Physical Society (APS)},
   Year = {1998},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.80.2773},
   Abstract = {We present a measurement of the t¯t production cross
             section in p¯p collisions at √s = 1.8TeV using an
             integrated luminosity of 109pb-1 collected with the Collider
             Detector at Fermilab. The measurement uses t¯t decays into
             final states which contain one or two high transverse
             momentum leptons and multiple jets, and final states which
             contain only jets. Using acceptances appropriate for a top
             quark mass of 175GeV/c2, we find σt¯t = 7.6+1.8-1.5pb. ©
             1998 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.80.2773},
   Key = {fds309717}
}

@article{fds309722,
   Author = {Akesson, T and Antonov, A and Bondarenko, V and Bytchkov, V and Carling,
             H and Commichau, K and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Dulny, B and Ebenstein, WL and Egede, U and Farthouat,
             P and Fent, J and Froidevaux, D and Gavrilenko, I and Hanson, G and Holder,
             M and Ivochkin, VG and Jagielski, S and Jaroslawski, S and Keener, PT and Kisielewski, B and Konovalov, S and Konstantinov, A and Kramarenko,
             VA and Lichard, P and Lundberg, B and Luehring, F and Lutsch, Y and Malecki, P and Muraviev, S and Nadtochy, A and Nevski, P and Newcomer,
             FM and Norton, P and Nuennerich, R and Ogren, H and Oh, SH and Olszowska,
             J and Pavlenko, S and Peshekhonov, V and Richter, R and Romaniouk, A and Rust, DR and Ryjov, V and Saxon, DH and Schegelsky, V and Schulte, R and Semenov, S and Shmeleva, A and Smirnov, S and Smirnova, LN and Soderberg, M and Sosnovtsev, V and Spiridenkov, E and Stavrianakou,
             M and Thulesius, M and Tikhomirov, V and Van Berg and R and Wang, C and White,
             DJ and Williams, HH},
   Title = {Electron identification with a prototype of the Transition
             Radiation Tracker for the ATLAS experiment},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {412},
   Number = {2-3},
   Pages = {200-215},
   Publisher = {Elsevier BV},
   Year = {1998},
   Month = {August},
   url = {http://dx.doi.org/10.1016/S0168-9002(98)00457-4},
   Abstract = {A prototype of the Transition Radiation Tracker (TRT) for
             the ATLAS detector at the LHC has been built and tested. The
             TRT is an array of straw tubes which integrate tracking and
             electron identification by transition radiation into one
             device. Results of experimental measurements and of
             comparisons with Monte-Carlo simulations are presented for
             the electron identification performance as a function of
             various detector parameters. Under optimal operating
             conditions, a rejection against pions of a factor 100 was
             achieved with 90% electron efficiency. © 1998 Elsevier
             Science B.V. All rights reserved.},
   Doi = {10.1016/S0168-9002(98)00457-4},
   Key = {fds309722}
}

@article{fds309723,
   Author = {Alexopoulos, T and Anderson, EW and Biswas, NN and Bujak, A and Carmony,
             DD and Erwin, AR and Gutay, LJ and Hirsch, AS and Hojvat, C and Kenney, VP and Lindsey, CS and LoSecco, JM and Matinyan, SG and Morgan, N and Oh, SH and Porile, N and Scharenberg, R and Stringfellow, B and Thompson, M and Turkot, F and Walker, WD and Wang, CH},
   Title = {The role of double parton collisions in soft hadron
             interactions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {435},
   Number = {3-4},
   Pages = {453-457},
   Publisher = {Elsevier BV},
   Year = {1998},
   Month = {September},
   url = {http://dx.doi.org/10.1016/S0370-2693(98)00921-6},
   Abstract = {We have examined charged multiplicities arising from p - p
             and p - p̄ collisions over the range of center of mass
             energies, √s, from 30 GeV to 1800 GeV. Results from
             Tevatron experiment E735 support the presence of double
             parton interactions. These processes can be seen to account
             for a large fraction of the increase in the non single
             diffraction inelastic cross section from energies of about
             200 GeV to 1800 GeV. © 1998 Published by Elsevier Science
             B.V. All rights reserved.},
   Doi = {10.1016/S0370-2693(98)00921-6},
   Key = {fds309723}
}

@article{fds313341,
   Author = {al, FAE},
   Title = {``Measurement of the $B_d^0\overline{B_{d}^0}$ Oscillation
             Frequency using Dimuon Data in $p\overline p$ Collisions at
             $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review},
   Volume = {D60},
   Number = {5},
   Pages = {051101},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.051101},
   Abstract = {We present a measurement of the mass difference (Formula
             presented) of the two (Formula presented) mass eigenstates.
             We use a flavor tagging method based on the lepton charge,
             in a sample of events with two muons at low transverse
             momentum. The sample corresponds to an integrated luminosity
             of (Formula presented) collected by the Collider Detector at
             Fermilab. The result obtained is (Formula presented) © 1999
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.60.051101},
   Key = {fds313341}
}

@article{fds340928,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bikhari, W and Bolla,
             G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Burner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
             S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
             B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
             H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
             O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti,
             G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn,
             SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hausser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
             KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
             BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins,
             D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch,
             L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo,
             K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald,
             W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
             JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
             S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
             S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
             C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
             KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
             A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
             L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Volobouev, I and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
             AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
             X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Kinematics of tt̄ events at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {59},
   Number = {9},
   Pages = {1-20},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.59.092001},
   Abstract = {The kinematic properties of tt̄ events are studied in the
             W+ multijet channel using data collected with the CDF
             detector during the 1992-1995 runs at the Fermilab Tevatron
             collider corresponding to an integrated luminosity of 109
             pb-1. Distributions of a variety of kinematic variables
             chosen to be sensitive to different aspects of tt̄
             production are compared with those expected from Monte Carlo
             calculations. A sample of 34 events rich in tt̄ pairs is
             obtained by requiring at least one jet identified by the
             silicon vertex detector (SVX) as having a displaced vertex
             consistent with the decay of a b hadron. The data are found
             to be in good agreement with predictions of the leading
             order tt̄ matrix element with color coherent parton shower
             evolution. ©1999 The American Physical Society.},
   Doi = {10.1103/PhysRevD.59.092001},
   Key = {fds340928}
}

@article{fds313362,
   Author = {al, FAE},
   Title = {``Measurement of the $B_{S}^{0}$ Meson Lifetime using
             Semileptonic Decays,"},
   Journal = {Physical Review},
   Volume = {D59},
   Number = {9},
   Pages = {032004},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.58.092002},
   Abstract = {The lifetimes of the [Formula Presented] and [Formula
             Presented] mesons are measured using the partially
             reconstructed semileptonic decays [Formula Presented] where
             [Formula Presented] is either a [Formula Presented] or
             [Formula Presented] meson. The data were collected by the
             CDF detector at the Fermilab Tevatron collider during
             1992–1995 and correspond to about [Formula Presented] of
             [Formula Presented] collisions at [Formula Presented] We
             measure decay lengths and extract the lifetimes to be
             [Formula Presented] ps and [Formula Presented] and the ratio
             of the lifetimes to be [Formula Presented] where the first
             uncertainties are statistical and the second are systematic.
             © 1998 The American Physical Society.},
   Doi = {10.1103/PhysRevD.58.092002},
   Key = {fds313362}
}

@article{fds313359,
   Author = {al, FAE},
   Title = {``Search for New Physics in Diphoton Events in $p\overline
             p$ Collisions at $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review},
   Volume = {D59},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.59.092002},
   Abstract = {We present a detailed description of a search for anomalous
             production of missing [Formula Presented] [Formula
             Presented] jets, leptons [Formula Presented] b quarks, or
             additional photons in events containing two isolated,
             central [Formula Presented] photons with [Formula Presented]
             The results are consistent with standard model expectations,
             with the possible exception of one event that has, in
             addition to the two photons, a central electron, a
             high-[Formula Presented] electromagnetic cluster, and large
             [Formula Presented] We set limits using two specific SUSY
             scenarios for production of diphoton events with [Formula
             Presented] © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.59.092002},
   Key = {fds313359}
}

@article{fds313360,
   Author = {al, FAE},
   Title = {``Measurement of $B^0$-$\overline{B^0}$ Flavor Oscillations
             using Jet-Charge and Lepton Flavor Tagging in $p\overline p$
             Collisions at $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review},
   Volume = {D60},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.072003},
   Abstract = {We present a measurement of the mass difference (Formula
             presented) for the (Formula presented) meson and the
             statistical power of the b flavor tagging methods used. The
             measurement uses (Formula presented) of data from (Formula
             presented) collisions at (Formula presented) collected with
             the CDF detector. An inclusive lepton trigger is used to
             collect a large sample of B hadron semileptonic decays. The
             mass difference (Formula presented) is determined from the
             proper time dependence of the fraction of B hadrons that
             undergo flavor oscillations. The flavor at decay is inferred
             from the charge of the lepton from semileptonic B decay. The
             initial flavor is inferred by determining the flavor of the
             other B hadron produced in the collision, either from its
             semileptonic decay (soft-lepton tag) or from its jet charge.
             The measurement yields (Formula presented), where the first
             uncertainty is statistical and the second uncertainty is
             systematic. The statistical powers (Formula presented) of
             the soft-lepton and jet-charge flavor taggers are (Formula
             presented) and (Formula presented), respectively. © 1999
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.60.072003},
   Key = {fds313360}
}

@article{fds313349,
   Author = {al, FAE},
   Title = {``Measurement of $Z^{0}$ and Drell-Yan Production Cross
             Sections using Dimuons in $p\overline p$ Collisions at
             $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review},
   Volume = {D59},
   Number = {5},
   Pages = {052002},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.59.052002},
   Abstract = {We present a measurement of [Formula Presented] boson and
             Drell-Yan production cross sections in [Formula Presented]
             collisions at [Formula Presented] using a sample of [Formula
             Presented] accumulated by the Collider Detector at Fermilab.
             The Drell-Yan cross section is measured in the mass range of
             [Formula Presented] We compare the measurements with the
             predictions of quantum chromodynamics in both leading order
             and next-to-leading order, incorporating the recent parton
             distribution functions. The measurements are consistent with
             the standard model expectations. © 1999 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.59.052002},
   Key = {fds313349}
}

@article{fds309527,
   Author = {Collaboration, CDF},
   Title = {Measurement of the Associated ƒ× + ƒÝ„b Production
             Cross Section in pp Collisions at = 1.8 TeV},
   Journal = {Phys. Rev.},
   Volume = {D60},
   Number = {8},
   Pages = {092003},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/physrevlett.97.082004},
   Abstract = {We present a measurement of the top quark pair production
             cross section in pp collisions at square root of s = 1.96
             TeV using 318 pb(-1) of data collected with the Collider
             Detector at Fermilab. We select tt[over ] decays into the
             final states enu+jets and mu nu+ jets, in which at least one
             b quark from the t-quark decays is identified using a
             secondary vertex-finding algorithm. Assuming a top quark
             mass of 178 GeV/c2, we measure a cross section of 8.7 +/-
             0.9(stat)(-0.9)+1.1(syst) pb. We also report the first
             observation of tt[over ] with significance greater than
             5sigma in the subsample in which both b quarks are
             identified, corresponding to a cross section of
             10.1(-1.4)+1.6(stat)(-1.3)+2.0(syst) pb.},
   Doi = {10.1103/physrevlett.97.082004},
   Key = {fds309527}
}

@article{fds313356,
   Author = {al, TAE},
   Title = {``Measurement of the $B^0 \overline{B^0}$ Oscillation
             Frequency using $lÐD^{*+}$ Pairs and Lepton Flavor
             Tags,"},
   Journal = {Physical Review},
   Volume = {D60},
   Number = {11},
   Pages = {112004},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.112004},
   Abstract = {The oscillation frequency (Formula presented) of (Formula
             presented) mixing is measured using the partially
             reconstructed semileptonic decay (Formula presented) The
             data sample was collected with the CDF detector at the
             Fermilab Tevatron collider during 1992–1995 by triggering
             on the existence of two lepton candidates in an event, and
             corresponds to about 110 (Formula presented) of (Formula
             presented) collisions at (Formula presented) TeV. We
             estimate the proper decay time of the (Formula presented)
             meson from the measured decay length and reconstructed
             momentum of the (Formula presented) system. The charge of
             the lepton in the final state identifies the flavor of the
             (Formula presented) meson at its decay. The second lepton in
             the event is used to infer the flavor of the (Formula
             presented) meson at production. We measure the oscillation
             frequency to be (Formula presented) (Formula presented),
             where the first uncertainty is statistical and the second is
             systematic. © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.60.112004},
   Key = {fds313356}
}

@article{fds313346,
   Author = {al, FAE},
   Title = {``Measurement of $b$ Quark Fragmentation Fractions in the
             Production of Strange and Light $B$ Mesons in $p\overline p$
             Collisions at $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review},
   Volume = {D60},
   Number = {9},
   Pages = {092005},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.092005},
   Abstract = {A new technique to measure the ratio of b quark
             fragmentation fractions in (Formula presented) collisions is
             described. Using a (Formula presented) sample of low-mass
             dimuon trigger data recorded with the Collider Detector at
             Fermilab, we identify B mesons by observing the double
             semileptonic decays (Formula presented) with (Formula
             presented) By counting the numbers of (Formula presented)
             (Formula presented) and φ(1020) mesons produced in
             association with these muon pairs, we measure the ratio of
             strange to nonstrange B meson production to be (Formula
             presented) This measurement is the most precise available
             from hadron collisions to date. Limits on the branching
             fractions of semileptonic charm meson decays with (Formula
             presented) (Formula presented) and (Formula presented)
             mesons in the final state are also obtained. © 1999 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.60.092005},
   Key = {fds313346}
}

@article{fds309683,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bikhari, W and Bolla,
             G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Burner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
             S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
             B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
             H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
             O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti,
             G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn,
             SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hausser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
             KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
             BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins,
             D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch,
             L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo,
             K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald,
             W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
             JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
             S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
             S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
             C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
             KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
             A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
             L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Volobouev, I and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
             AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
             X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Searches for new physics in diphoton events in pp̄
             collisions at √s = 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {59},
   Number = {9},
   Pages = {1-29},
   Year = {1999},
   Abstract = {We present a detailed description of a search for anomalous
             production of missing ET (Slashed E signT), jets, leptons
             (e, μ, τ), b quarks, or additional photons in events
             containing two isolated, central (|η|&lt;1.0) photons with
             ET&gt;12 GeV. The results are consistent with standard model
             expectations, with the possible exception of one event that
             has, in addition to the two photons, a central electron, a
             high-ET electromagnetic cluster, and large Slashed E signT.
             We set limits using two specific SUSY scenarios for
             production of diphoton events with Slashed E signT. ©1999
             The American Physical Society.},
   Key = {fds309683}
}

@article{fds309684,
   Author = {Collaboration, CDF},
   Title = {A Search for B - B Oscillations Using the Semileptonic Decay
             B -> o;=Xu},
   Journal = {Phys. Rev. Lett.},
   Volume = {82},
   Number = {18},
   Pages = {3576},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.3576},
   Abstract = {A search for Bs0-B̄s0 oscillations is performed in a sample
             of Bs0 semileptonic decays collected using dilepton triggers
             at the Tevatron Collider during 1992-1995. The Bs0 is
             reconstructed using φ mesonlepton correlations; its initial
             production flavor is determined with the second lepton in
             the event. From a signal of 1068 with a Bs0 purity of 61%,
             we obtain a limit on the Bs0-B̄s0 oscillation frequency of
             Δms &gt; 5.8 ps-1 at 95% confidence level. © 1999 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.82.3576},
   Key = {fds309684}
}

@article{fds309685,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla,
             G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
             S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
             B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch,
             H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel,
             O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti,
             G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
             R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Hohlmann,
             M and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
             BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins,
             D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch,
             L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo,
             K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald,
             W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
             JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
             S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
             S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
             KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
             A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
             L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang,
             CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Measurement of Z0 and Drell-Yan production cross
             sections using dimuons in p̄p collisions at
             √s=1.8TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {59},
   Number = {5},
   Pages = {1-15},
   Year = {1999},
   Abstract = {We present a measurement of Z0 boson and Drell-Yan
             production cross sections in p̄p collisions at √s =1.8TeV
             using a sample of 107 pb-1 accumulated by the Collider
             Detector at Fermilab. The Drell-Yan cross section is
             measured in the mass range of Mμμ&gt;40GeV/c2. We compare
             the measurements with the predictions of quantum
             chromodynamics in both leading order and next-to-leading
             order, incorporating the recent parton distribution
             functions. The measurements are consistent with the standard
             model expectations. ©1999 The American Physical
             Society.},
   Key = {fds309685}
}

@article{fds309686,
   Author = {al, FAE},
   Title = {``Search for Third-Generation Leptoquarks from Technicolor
             Models in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,"},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {16},
   Pages = {3206},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.3206},
   Abstract = {We report the results of a search for technicolor using
             110pb-1 of pp collisions recorded by the Collider Detector
             at Fermilab (CDF). In technicolor models containing a
             technifamily, color-octet technirhos enhance the pair
             production of color-triplet technipions, which behave as
             third-generation leptoquarks. From our previously reported
             search for third-generation leptoquarks, we present
             constraints on the production of color-triplet technipions
             and color-octet technirhos as a function of their masses. ©
             1999 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.82.3206},
   Key = {fds309686}
}

@article{fds309687,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
             AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
             C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
             L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
             O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
             SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
             TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
             A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
             MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
             A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
             K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
             R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
             M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar,
             R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of the BS0 meson lifetime
             using semileptonic decays},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {59},
   Number = {3},
   Pages = {1-14},
   Year = {1999},
   Abstract = {The lifetime of the BS0 meson is measured using the
             semileptonic decay BS0→DS-l+νX. The data sample consists
             of about 110 pb-1 of pp̄ collisions at √s=1.8 TeV
             collected by the CDF detector at Fermilab. Four different
             DS- decay modes are reconstructed resulting in approximately
             600 DS-l+ signal events. The BS0 meson lifetime is
             determined to be τ(BS0)=(1.36±0.09-0.05+0.06) ps, where
             the first and second uncertainties are statistical and
             systematic, respectively. The BS0 meson decay length
             distribution is examined for a lifetime difference ΔΓ/Γ
             between the two mass eigenstates of the BS0 meson. An upper
             limit of ΔΓ/Γ&lt;0.83 is set at the 95% confidence
             level.},
   Key = {fds309687}
}

@article{fds309688,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark,
             AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
             C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Hao, W and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Hollebeek, R and Holloway,
             L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Limon, P and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
             O and Loomis, C and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh,
             SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips,
             TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni,
             A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt,
             MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill,
             A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok,
             K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima,
             R and Takikawa, K and Tanaka, M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko,
             M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar,
             R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of the Bd0-B̄d0
             flavor oscillation frequency and study of same side flavor
             tagging of B mesons in pp̄ collisions},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {59},
   Number = {3},
   Pages = {1-41},
   Year = {1999},
   Abstract = {Bd0-B̄d0 oscillations are observed in "self-tagged" samples
             of partially reconstructed B mesons decaying into a lepton
             and a charmed meson collected in pp̄ collisions at √s=1.8
             TeV. A flavor tagging technique is employed which relies
             upon the correlation between the flavor of B mesons and the
             charge of a nearby particle. We measure the flavor
             oscillation frequency to be Δmd=0.471-0.068+0.078±0.034
             ps-1. The tagging method is also demonstrated in exclusive
             samples of Bu+→J/ψK+ and Bd0→J/ψK*0(892), where
             similar flavor-charge correlations are observed. The tagging
             characteristics of the various samples are compared with
             each other, and with Monte Carlo simulations.},
   Key = {fds309688}
}

@article{fds309689,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
             C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg,
             C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
             M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Dolce, G and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti,
             C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman,
             J and Friedman, J and Frisch, H and Fukui, Y and Gadomski, S and Galeotti,
             S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel,
             AF and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold, M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber,
             C and Hafen, E and Hahn, SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz,
             E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato,
             Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart,
             R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
             J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster,
             M and Lanzoni, M and Latino, G and LeCompte, T and IV, AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
             N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Partos,
             D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara,
             L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi,
             F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw,
             NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith,
             C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella,
             F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka, M and Tannenbaum,
             B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto,
             Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk,
             W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal,
             R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner,
             RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei,
             C and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Measurement of the Bd0d0
             oscillation frequency using dimuon data in pp̄ collisions
             at √s = 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {5},
   Pages = {1-6},
   Year = {1999},
   Abstract = {We present a measurement of the mass difference Δmd of the
             two Bd0 mass eigenstates. We use a flavor tagging method
             based on the lepton charge, in a sample of events with two
             muons at low transverse momentum. The sample corresponds to
             an integrated luminosity of 90 pb-1 collected by the
             Collider Detector at Fermilab. The result obtained is
             Δmd=0.503±0.064(stat)±0.071(syst) ps-1. ©1999 The
             American Physical Society.},
   Key = {fds309689}
}

@article{fds309690,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
             C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg,
             C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
             M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
             B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui,
             Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
             DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
             M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
             R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
             U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi,
             T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
             JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and IV,
             AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin,
             A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
             S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
             C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas,
             J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
             AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
             X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of B0-B̄0 flavor
             oscillations using jet-charge and lepton flavor tagging in
             pp̄ collisions at √s=1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {7},
   Pages = {1-22},
   Year = {1999},
   Abstract = {We present a measurement of the mass difference Δmd for the
             B0 meson and the statistical power of the b flavor tagging
             methods used. The measurement uses 90 pb-1 of data from pp̄
             collisions at √s= 1.8 TeV collected with the CDF detector.
             An inclusive lepton trigger is used to collect a large
             sample of B hadron semileptonic decays. The mass difference
             Δmd is determined from the proper time dependence of the
             fraction of B hadrons that undergo flavor oscillations. The
             flavor at decay is inferred from the charge of the lepton
             from semileptonic B decay. The initial flavor is inferred by
             determining the flavor of the other B hadron produced in the
             collision, either from its semileptonic decay (soft-lepton
             tag) or from its jet charge. The measurement yields
             Δmd=(0.500±0.052±0.043)ℏ ps-1, where the first
             uncertainty is statistical and the second uncertainty is
             systematic. The statistical powers (∈D2) of the
             soft-lepton and jet-charge flavor taggers are (0.91±0.10
             ±0.11)% and (0.78±0.12±0.08)%, respectively. ©1999 The
             American Physical Society.},
   Key = {fds309690}
}

@article{fds309691,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari,
             C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg,
             C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
             M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
             B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui,
             Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
             DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
             M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
             R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
             U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi,
             T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux,
             JI and Lancaster, M and Lanzoni, M and Latino, G and LeCompte, T and Leone,
             S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler,
             S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson,
             C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Portos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Ströhmer, R and Strologas,
             J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Vidai, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
             AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
             X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of b quark fragmentation fractions in the
             production of strange and light B mesons in pp̄ collisions
             at √s=1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {9},
   Pages = {1-14},
   Year = {1999},
   Abstract = {A new technique to measure the ratio of b quark
             fragmentation fractions in pp̄ collisions is described.
             Using a 70-pb-1 sample of low-mass dimuon trigger data
             recorded with the Collider Detector at Fermilab, we identify
             B mesons by observing the double semileptonic decays b→c
             μX with c→s μX. By counting the numbers of K*(892)0,
             K*(892)+, and φ(1020) mesons produced in association with
             these muon pairs, we measure the ratio of strange to
             nonstrange B meson production to be fs/(fu+fd)=[21.0±3.6(stat)
             -3.0+3.8(syst)]%. This measurement is the most precise
             available from hadron collisions to date. Limits on the
             branching fractions of semileptonic charm meson decays with
             K1(1270), K1* (1410), and K2*(1430) mesons in the final
             state are also obtained. ©1999 The American Physical
             Society.},
   Key = {fds309691}
}

@article{fds309692,
   Author = {al, FAE},
   Title = {``Measurement of the Associated $\gamma + \mu^{\pm}$
             Production Cross Section in $p\overline p$ Collisions at
             $\sqrt{s} = 1.8$ TeV,"},
   Journal = {Physical Review},
   Volume = {D60},
   Number = {9},
   Pages = {092003},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.60.092003},
   Abstract = {We present the first measurement of associated direct
             photon(Formula presented)muon production in hadronic
             collisions, from a sample of 1.8 TeV (Formula presented)
             collisions recorded with the Collider Detector at Fermilab.
             Quantum chromodynamics (QCD) predicts that these events are
             primarily from the Compton scattering process (Formula
             presented) with the final state charm quark producing a
             muon. Hence this measurement is sensitive to the charm quark
             content of the proton. The measured cross section of
             (Formula presented) pb is compared to a leading-order QCD
             parton shower model as well as a next-to-leading-order QCD
             calculation. © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.60.092003},
   Key = {fds309692}
}

@article{fds309693,
   Author = {Adamczyk, AA and Hubbard, CP and Ament, F and Oh, SH and Brady, MJ and Yee,
             MC},
   Title = {Experimental and modeling evaluations of a vacuum-insulated
             catalytic converter},
   Journal = {SAE Technical Papers},
   Year = {1999},
   url = {http://dx.doi.org/10.4271/1999-01-3678},
   Abstract = {Vehicle evaluations and model calculations were conducted on
             a vacuum-insulated catalytic converter (VICC). This
             converter uses vacuum and a eutectic PCM (phase-change
             material) to prolong the temperature cool-down time and
             hence, may keep the converter above catalyst light-off
             between starts. Tailpipe emissions from a 1992 Tier 0 5.2L
             van were evaluated after 3hr, 12hr, and 24hr soak periods.
             After a 12hr soak the HC emissions were reduced by about 55%
             over the baseline HC emissions; after a 24hr soak the device
             did not exhibit any benefit in light-off compared to a
             conventional converter. Cool-down characteristics of this
             VICC indicated that the catalyst mid-bed temperature was
             about 180°C after 24hrs. Model calculations of the
             temperature warm-up were conducted on a VICC converter.
             Different warm-up profiles within the converter were
             predicted depending on the initial temperature of the
             device. If the device was at 227°C, the initial exotherm
             occurred downstream of the inlet and eventually spread over
             the entire converter as a result of convective heat
             transfer. If the device was at ambient (27°C), the initial
             exotherm occurred at the inlet and the temperature profile
             decreased monotonically across the catalyst, typical of a
             conventional converter. The model simulations show that
             there is little cold-start benefit unless the converter
             temperature after the soak exceeds 200°C. To be considered
             for widespread automotive usage, either overall VICC design
             must be improved to meet a 36hr catalyst light-off
             temperature retention period as specified in US emissions
             regulations or the cold soak period must be shortened to
             about 16-18hrs to match the characteristics of a VICC-type
             catalyst. In addition, other challenges for a VICC-type
             device include reduced packaging size, improved real world
             durability and reduced amount of driving preparation
             necessary to fully melt its PCM material so as to allow it
             to retain heat for the longer period of time. Copyright ©
             1999 Society of Automotive Engineers, Inc.},
   Doi = {10.4271/1999-01-3678},
   Key = {fds309693}
}

@article{fds309694,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
             T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
             JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
             C and Bloom, K and Blusk, S and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
             A and Brink, SVD and Bromberg, C and Brunner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson,
             J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng,
             MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze,
             G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein,
             J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
             J and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck,
             C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara,
             H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
             A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV,
             AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn,
             S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
             R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos,
             A and Pondrom, L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos,
             F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum,
             B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidai, R and Vilar, R and Vologouev,
             I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts,
             T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu,
             I and Yu, S and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Measurement of the B00 oscillation
             frequency using l-D*+ pairs and lepton
             flavor tags},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {60},
   Number = {11},
   Pages = {1-12},
   Year = {1999},
   Abstract = {The oscillation frequency Δmd of B0B̄0 mixing is measured
             using the partially reconstructed semileptonic decay
             B̄0→l-ν̄D*+X. The data sample was collected with the
             CDF detector at the Fermilab Tevatron collider during
             1992-1995 by triggering on the existence of two lepton
             candidates in an event, and corresponds to about 110 pb-1 of
             p̄p collisions at √s=1.8 TeV. We estimate the proper
             decay time of the B̄0meson from the measured decay length
             and reconstructed momentum of the l-D*+ system. The charge
             of the lepton in the final state identifies the flavor of
             the B̄0 meson at its decay. The second lepton in the event
             is used to infer the flavor of the B̄0 meson at production.
             We measure the oscillation frequency to be Δmd=0.516
             ±0.099-0.035+0.029 ps-1, where the first uncertainty is
             statistical and the second is systematic. ©1999 The
             American Physical Society.},
   Key = {fds309694}
}

@article{fds313344,
   Author = {al, FAE},
   Title = {``Measurement of the $B_{d}^{0}$-$\overline {B_{d}^{0}}$
             Flavor Oscillation Frequency and Study of Same Side Flavor
             Tagging of $B$ Mesons in $p\overline p$ Collisions,"},
   Journal = {Physical Review},
   Volume = {D59},
   Number = {3},
   Pages = {032001},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   url = {http://dx.doi.org/10.1103/PhysRevD.59.032001},
   Abstract = {[Formula Presented] oscillations are observed in
             “self-tagged” samples of partially reconstructed
             [Formula Presented] mesons decaying into a lepton and a
             charmed meson collected in [Formula Presented] collisions at
             [Formula Presented] A flavor tagging technique is employed
             which relies upon the correlation between the flavor of
             [Formula Presented] mesons and the charge of a nearby
             particle. We measure the flavor oscillation frequency to be
             [Formula Presented] The tagging method is also demonstrated
             in exclusive samples of [Formula Presented] and [Formula
             Presented] where similar flavor-charge correlations are
             observed. The tagging characteristics of the various samples
             are compared with each other, and with Monte Carlo
             simulations. © 1998 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.59.032001},
   Key = {fds313344}
}

@article{fds332115,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Bao, J and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers,
             W and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy,
             D and Culbertson, R and Dagenhart, D and Daniels, T and De Jongh and F and Dell’agnello, S},
   Title = {Search for new particles decaying to b¯b in p¯p collisions
             at √s=1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {82},
   Number = {10},
   Pages = {2038-2043},
   Publisher = {American Physical Society (APS)},
   Year = {1999},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevLett.82.2038},
   Abstract = {We have used 87pb−1 of data collected with the collider
             detector at Fermilab to search for new particles decaying to
             b¯b. We present model-independent upper limits on the cross
             section for narrow resonances which exclude the color-octet
             technirho in the mass interval 350<M<440GeV/c2. In addition,
             we exclude top-gluons, predicted in models of
             top-color-assisted technicolor, of width Τ=0.3M in the mass
             range 280<M<670GeV/c2, of width Τ=0.5M in the mass range
             340<M<640GeV/c2, and of width Τ=0.7M in the mass range
             375<M<560GeV/c2. © 1999 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.82.2038},
   Key = {fds332115}
}

@article{fds309695,
   Author = {Oh, SH and Wang, CH and Ebenstein, WL},
   Title = {Super high rate straw drift chamber},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {425},
   Number = {1},
   Pages = {75-83},
   Publisher = {Elsevier BV},
   Year = {1999},
   Month = {April},
   url = {http://dx.doi.org/10.1016/S0168-9002(98)01376-X},
   Abstract = {We have devised a technique to read out a sense wire inside
             a straw tube in many independent sections without bulky
             plates between sections, thus reducing the occupancy
             considerably. Based on this technique, a prototype chamber
             is constructed, which is suitable for extremely high rate
             environments.},
   Doi = {10.1016/S0168-9002(98)01376-X},
   Key = {fds309695}
}

@article{fds309454,
   Author = {al, TAE},
   Title = {``Direct measurement of the $W$ boson width in $p\overline
             p$ Collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {7},
   Pages = {3347},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/physrevlett.100.071801},
   Abstract = {A direct measurement of the total decay width of the W boson
             Gamma(W) is presented using 350 pb(-1) of data from pp[over
             ] collisions at square root s = 1.96 TeV collected with the
             CDF II detector at the Fermilab Tevatron. The width is
             determined by normalizing predicted signal and background
             distributions to 230 185 W candidates decaying to enu and
             micronu in the transverse-mass region 50<M(T)<90 GeV and
             then fitting the predicted shape to 6055 events in the
             high-M(T) region, 90<M(T)<200 GeV. The result is
             Gamma(W)=2032 +/- 45(stat)+/-57(syst) MeV, consistent with
             the standard model expectation.},
   Doi = {10.1103/physrevlett.100.071801},
   Key = {fds309454}
}

@article{fds313351,
   Author = {al, TAE and Collaboration, TCDF},
   Title = {A Measurement of sin 2 from B with the CDF
             Detector},
   Journal = {Phys. Rev.},
   Volume = {D61},
   Number = {7},
   Pages = {072005},
   Year = {2000},
   Abstract = {This paper reports an updated measurement of the standard
             model CP violation parameter sin 2β using the CDF Detector
             at Fermilab. The entire run I data sample of 110 pb -1 of
             proton-antiproton collisions at √s = 1.8 TeV is used to
             identify a signal sample of ∼400 B→J/φK s0 events,
             where J/φ→μ + μ - →μ + μ - . The flavor of the
             neutral B meson is identified at the time of production by
             combining information from three tagging algorithms: a
             same-side tag, a jet-charge tag, and a soft-lepton tag. A
             maximum likelihood fitting method is used to determine sin
             2β=0.79 -0.44+0.41 (stat+syst). This value of sin 2β is
             consistent with the standard model prediction, based upon
             existing measurements, of a large positive CP-violating
             asymmetry in this decay mode. ©2000 The American Physical
             Society.},
   Key = {fds313351}
}

@article{fds332113,
   Author = {al, TAE},
   Title = {``Observation of Diffractive $b$-Quark Production at the
             Fermilab Tevatron,"},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {2},
   Pages = {232},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.232},
   Abstract = {We report a measurement of the fraction of b quarks produced
             diffractively in ⊯pp collisions at √ s = 1.8 TeV.
             Diffraction is identified by the absence of particles in a
             forward pseudorapidity region. From events with an electron
             of transverse momentum 9.5 < peT< 20 GeV/c within the
             pseudorapidity region |η| < 1.1, the ratio of diffractive
             to total b-quark production rates is found to be R⊯bb=
             [0.62 ± 0.19(stat) ± 0.16(syst)]%. This result is
             comparable in magnitude to corresponding ratios for W and
             dijet production but significantly lower than expectations
             based on factorization. © 2000 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.84.232},
   Key = {fds332113}
}

@article{fds313364,
   Author = {al, TAE},
   Title = {``Search for the charged Higgs boson in the decays of top
             quark pairs in the $e \tau$ and $\mu \tau$ channels at
             $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review},
   Volume = {D62},
   Number = {1},
   Pages = {012004},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevD.62.012004},
   Abstract = {Top quark production offers the unique opportunity to search
             for a charged Higgs boson (Formula presented) as the
             contribution from (Formula presented) can be large in
             extensions of the standard model. We use results from a
             search for top quark pair production by the Collider
             Detector at Fermilab (CDF) in the (Formula presented) and
             (Formula presented) signatures to set an upper limit on the
             branching ratio of (Formula presented) in 106 (Formula
             presented) of data. The upper limit is in the range 0.5 to
             0.6 at 95% C.L. for (Formula presented) masses in the range
             60 to 160 GeV, assuming the branching ratio for (Formula
             presented) is 100%. The (Formula presented) lepton is
             detected through its 1-prong and 3-prong hadronic decays. ©
             2000 The American Physical Society.},
   Doi = {10.1103/PhysRevD.62.012004},
   Key = {fds313364}
}

@article{fds309663,
   Author = {al, TAE},
   Title = {``Measurement of $b$-Quark Fragmentation Fractions in
             $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,"},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {8},
   Pages = {1663},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/physrevlett.84.1663},
   Abstract = {We have studied the production of B hadrons in 1.8-TeV
             pp[over ¯] collisions. We present measurements of the
             fragmentation fractions, f_{u}, f_{d}, f_{s}, and
             f_{baryon}, of produced b quarks that yield B^{+}, B^{0},
             B_{s}^{0}, and Λ[over ¯]_{b}^{0} hadrons. Reconstruction
             of five electron-charm final states yields f_{s}/(
             f_{u}+f_{d})=0.213±0.068 and f_{baryon}/(
             f_{u}+f_{d})=0.118±0.042, assuming f_{u}=f_{d}. If all B
             hadrons produced in pp[over ¯] collisions cascade to one of
             these four hadrons, we determine f_{u}=f_{d}=0.375±0.023,
             f_{s}=0.160±0.044, and f_{baryon}=0.090±0.029. If we do
             not assume f_{u}=f_{d}, we find f_{d}/f_{u}=0.84±0.16.},
   Doi = {10.1103/physrevlett.84.1663},
   Key = {fds309663}
}

@article{fds309664,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amadon, A and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Baumann, T and Bedeschi, F and Behrends, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery,
             K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla,
             G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada,
             J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao,
             HY and Chapman, J and Cheng, MT and Chertok, M and Chiarelli, G and Chiou,
             CN and Chlebana, F and Christofek, L and Cropp, R and Chu, ML and Cihangir,
             S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely, R and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher,
             B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui,
             Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
             DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
             M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hamilton,
             R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi,
             U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
             J and Kordas, K and Korytov, A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster,
             M and Lanzoni, M and Latino, G and LeCompte, T and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long,
             O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts,
             KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Reischl, M and Ribon,
             A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
             L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini,
             N and Uchida, T and Ukegawa, F and Valls, J and Brink, SCVD and III, SV and Velev, G and Volobouev, I and Vidal, R and Vilar, R and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and III, WCW and Wicklund,
             AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu,
             X and Wyss, J and Yagil, A and Yao, W and Yasuoka, K and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of bb̄ rapidity correlations in pp̄ collisions
             at √s=1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {61},
   Number = {3},
   Pages = {1-18},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevD.61.032001},
   Abstract = {We report the first direct measurement of bb̄ rapidity
             correlations in pp̄ collisions at √=1.8 TeV. We select
             events with a high transverse momentum muon accompanied by a
             jet, and a second jet associated with a decay vertex
             displaced from the pp̄ interaction vertex. Two independent
             samples are obtained corresponding to events with a forward
             (2.0&lt;|η|&lt;2.6) or central (|η|&lt;0.6) muon. We
             measure the ratio of forward to central bb̄ production to
             be 0.361±0.033(stat)-0.031+0.015(syst), in good agreement
             with the next-to-leading order QCD prediction
             0.338-0.097+0.014. ©2000 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.61.032001},
   Key = {fds309664}
}

@article{fds309665,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonusnkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Brink,
             SVD and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr,
             EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furie, I and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein,
             J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haas, RM and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara,
             K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kirby, M and Kirk, M and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu,
             YC and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi,
             N and Moore, E and Moore, R and Morita, Y and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman,
             J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos, F and Pukhov, O and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson,
             A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Safonov, A and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi,
             L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt,
             MP and Schmitt, M and Scodellaro, E and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo,
             P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka,
             M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi,
             K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Vidal, R and Vilar,
             R and Volobouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
             J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and III,
             WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu,
             Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of J / ψ and ψ (2S) polarization in pp̄
             collisions at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {14},
   Pages = {2886-2891},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/physrevlett.85.2886},
   Abstract = {We have measured the polarization of J/ψ and ψ(2S) mesons
             produced in pp̄ collisions at √s = 1.8 TeV, using data
             collected at the Collider Detector at Fermilab during
             1992-1995. The polarization of promptly produced J/ψ
             [ψ(2S)] mesons is isolated from those produced in B-hadron
             decay, and measured over the kinematic range 4 [5.5] &lt; PT
             &lt; 20 GeV/c and |y| &lt; 0.6. For PT ≳ 12 GeV/c we do
             not observe significant polarization in the prompt
             component. © 2000 The American Physical
             Society.},
   Doi = {10.1103/physrevlett.85.2886},
   Key = {fds309665}
}

@article{fds309666,
   Author = {al, TAE},
   Title = {``Search for Color Singlet Technicolor Particles in
             $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,"},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {6},
   Pages = {1110},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.1110},
   Abstract = {We search for color singlet technirho and technipion
             production in pp¯ Collisions at √s = 1.8TeVrecorded with
             the Collider Detector at Fermilab. These exotic technimesons
             are present in a model of walking technicolor. The
             signatures studied are lepton plus two jets plus ET and
             multijet final states. No excess of events is seen in either
             final state. We set an upper limit on the technirho
             production cross section and exclude a region in the
             technipion mass versus technirho mass plane. © 2000
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.84.1110},
   Key = {fds309666}
}

@article{fds309667,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti,
             A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandi, A and Brink, SVD and Bromberg, C and Brozovic,
             M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
             M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang,
             PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu,
             CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli,
             M and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent,
             PF and Devlin, T and Dittmann, JR and Donau, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori,
             I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer,
             S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold,
             M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos,
             K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Kara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
             T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and Lecompte, T and IV, AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer,
             N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti, P and McFarland,
             KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore,
             E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn, S and Nakada,
             H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
             R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
             L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
             F and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
             A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
             T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton,
             P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Volobouev,
             I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters,
             D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of the differential dijet mass cross section in
             pp̄ collisions at √s=1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {61},
   Number = {9},
   Pages = {1-6},
   Year = {2000},
   Abstract = {We present a measurement of the cross section for production
             of two or more jets as a function of dijet mass, based on an
             integrated luminosity of 86 pb-1 collected with the Collider
             Detector at Fermilab. Our dijet mass spectrum is described
             within errors by next-to-leading order QCD predictions using
             CTEQ4HJ parton distributions, and is in good agreement with
             a similar measurement from the DØ experiment. ©2000 the
             American Physical Society.},
   Key = {fds309667}
}

@article{fds309668,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti,
             A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic,
             M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell,
             M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang,
             PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu,
             CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli,
             M and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent,
             PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori,
             I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch, H and Fukui, Y and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hinrichsen, B and Hoffman, KD and Hohlmann, M and Holck, C and Holloway,
             L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones,
             M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg,
             J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen,
             AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV, AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Loken,
             J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari,
             L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore,
             E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn, S and Nakada,
             H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
             R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
             L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
             F and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
             A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
             T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton,
             P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Volobouev,
             I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters,
             D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Search for the charged Higgs boson in the decays of top
             quark pairs in the eτ and μτ channels at √s=1.8
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {62},
   Number = {1},
   Pages = {1-7},
   Year = {2000},
   Abstract = {Top quark production offers the unique opportunity to search
             for a charged Higgs boson (H±), as the contribution from
             t→H+b→τ+νb can be large in extensions of the standard
             model. We use results from a search for top quark pair
             production by the Collider Detector at Fermilab (CDF) in the
             eτ+Slashed E signT+jets and μτ+Slashed E signT+jets
             signatures to set an upper limit on the branching ratio of
             ℬ(t→H+b) in 106 pb-1 of data. The upper limit is in the
             range 0.5 to 0.6 at 95% C.L. for H+ masses in the range 60
             to 160 GeV, assuming the branching ratio for H+→τν is
             100%. The τ lepton is detected through its 1-prong and
             3-prong hadronic decays. ©2000 The American Physical
             Society.},
   Key = {fds309668}
}

@article{fds309671,
   Author = {al, TAE},
   Title = {``Search for second and third generation leptoquarks
             including production via technicolor interactions in
             $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,''},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {10},
   Pages = {2056},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.2056},
   Abstract = {The collider detector at Fermilab was used to examine second
             and third generation leptoquarks. The potential production
             of color triplet technipions in strongly-coupled color octet
             technirhos decays was examined. Events with heavy flavor
             jets and missing energy may indicate the second-generation
             leptoquark decay to a charm quark and neutrino. Since there
             were no excess of events above standard model predictions,
             95% confidence level limits were determined.},
   Doi = {10.1103/PhysRevLett.85.2056},
   Key = {fds309671}
}

@article{fds309672,
   Author = {al, TAE},
   Title = {``Limits on gravitino production and new processes with
             large missing transverse energy in $p\overline p$ Collisions
             at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {7},
   Pages = {1378},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.1378},
   Abstract = {Events collected by the Collider Detector at Fermilab (CDF)
             with an energetic jet plus large missing transverse energy
             can be used to search for physics beyond the standard model.
             We see no deviations from the expected backgrounds and set
             upper limits on the production of new processes. We consider
             in addition the production of light gravitinos and set a
             limit at 95% F ≥ 217GeV, which excludes gravitino masses
             smaller than 1.1 × 10−5eV/c2. © 2000 American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.85.1378},
   Key = {fds309672}
}

@article{fds309674,
   Author = {al, TAE},
   Title = {``Dijet production by double pomeron exchange at the
             Fermilab Tevatron,''},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {20},
   Pages = {4215},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.4215},
   Abstract = {Dijet production by double Pomeron exchange (DPE) in p̄p
             collisions at √ s = 1800 GeV was performed. Factorization
             was tested by comparing the diffractive structure function
             measured in single diffractive (SD) with that determined
             from DPE. As a result, a class of events with a double
             Pomeron exchange topology were observed.},
   Doi = {10.1103/PhysRevLett.85.4215},
   Key = {fds309674}
}

@article{fds309675,
   Author = {Collaboration, CDF},
   Title = {Search for a Fourth-Generation Quark More Massive than the
             Z0 Boson in pp Collisions at = 1.8 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {84},
   Number = {5},
   Pages = {835},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.835},
   Abstract = {We present the results of a search for pair production of a
             fourth-generation charge -1/3 quark (b′) in √s=1.8 TeV
             pp¯ collisions using 88 pb−1 of data obtained with the
             Collider Detector at Fermilab. We assume that both quarks
             decay via the flavor-changing neutral current process
             b′→bZ0 and that the b′ mass is greater than mZ+mb. We
             studied the decay mode b′b′¯→Z0Z0bb¯ where one Z0
             decays into e+e− or μ+μ− and the other decays
             hadronically, giving a signature of two leptons plus jets.
             An upper limit on the σpp¯→b′b′¯×[B(b′→bZ0)]2
             is established as a function of the b′ mass. We exclude at
             95% confidence level a b′ quark with mass between 100 and
             199 GeV/c2 for B(b′→bZ0)=100%. © 2000 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.84.835},
   Key = {fds309675}
}

@article{fds309676,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
             T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
             JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
             C and Bloom, K and Blumenfeld, B and Blusk, BS and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SVD and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto,
             G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein,
             J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
             J and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck,
             C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara,
             H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
             A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and Lee,
             AM and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman,
             J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
             L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni,
             A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo,
             P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
             A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
             T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk,
             S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
             BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of sin 2β from B→J/φKs0
             with the CDF detector},
   Journal = {Physical Review D},
   Volume = {61},
   Number = {7},
   Pages = {1-16},
   Year = {2000},
   Abstract = {This paper reports an updated measurement of the standard
             model CP violation parameter sin 2β using the CDF Detector
             at Fermilab. The entire run I data sample of 110 pb-1 of
             proton-antiproton collisions at √s = 1.8 TeV is used to
             identify a signal sample of ∼400 B→J/φKs0 events, where
             J/φ→μ+μ- →μ+μ-. The flavor of the neutral B meson
             is identified at the time of production by combining
             information from three tagging algorithms: a same-side tag,
             a jet-charge tag, and a soft-lepton tag. A maximum
             likelihood fitting method is used to determine sin
             2β=0.79-0.44+0.41(stat+syst). This value of sin 2β is
             consistent with the standard model prediction, based upon
             existing measurements, of a large positive CP-violating
             asymmetry in this decay mode. ©2000 The American Physical
             Society.},
   Key = {fds309676}
}

@article{fds309677,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
             T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
             JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
             C and Bloom, K and Blumenfeld, B and Blusk, BS and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SVD and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto,
             G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr,
             EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer, S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold, M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo,
             RS and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Heiss, A and Hinrichsen, B and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara,
             H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
             A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV,
             AML and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman,
             J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Peters, MD and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
             L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni,
             A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo,
             P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco, L and Steele, J and Stefanini,
             A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
             T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk,
             S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Vologouev,
             I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts,
             T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu,
             I and Yu, S and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Measurement of sin2β from B→J/ψKS0
             with the CDF detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {61},
   Number = {7},
   Pages = {1-16},
   Year = {2000},
   Abstract = {This paper reports an updated measurement of the standard
             model CP violation parameter sin 2β using the CDF Detector
             at Fermilab. The entire run I data sample of 110 pb-1 of
             proton-antiproton collisions at √s =1.8 TeV is used to
             identify a signal sample of ∼400 B→J/ψKS0 events, where
             J/ψ→μ+μ- and KS0 →π+π-. The flavor of the neutral B
             meson is identified at the time of production by combining
             information from three tagging algorithms: a same-side tag,
             a jet-charge tag, and a soft-lepton tag. A maximum
             likelihood fitting method is used to determine
             sin2β=0.19-0.44+0.41(stat+syst). This value of sin 2β is
             consistent with the standard model prediction, based upon
             existing measurements, of a large positive CP-violating
             asymmetry in this decay mode. ©2000 The American Physical
             Society.},
   Key = {fds309677}
}

@article{fds309678,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
             T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
             JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
             C and Bloom, K and Blusk, S and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
             A and Brink, SVD and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson,
             J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng,
             MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze,
             G and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Costa, JGD and Costanzo, D and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan,
             Q and Feild, RG and Ferretti, C and Fiori, I and Flaugher, B and Foster,
             GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer,
             S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold,
             M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos,
             K and Grassmann, H and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Guo, RS and Haber, C and Hafen, E and Hahn,
             SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama,
             K and Hauser, J and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
             KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston,
             J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
             A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and Lee,
             AM and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Meschi, E and Mesropian, C and Miao, C and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Moggi, N and Moore, E and Moore, R and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn,
             S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Pagliarone, C and Palmonari, F and Paoletti,
             R and Papadimitriou, V and Pappas, SP and Parri, A and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos,
             A and Pondrom, L and Pope, G and Prokoshin, F and Proudfoot, J and Ptohos,
             F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi, F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Stanco, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Takano, T and Tannenbaum,
             B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Truitt, S and Tseng, J and Turini, N and Ukegawa, F and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
             BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Transverse Momentum and Total Cross Section of
             e+e- Pairs in the Z-Boson Region from
             pp̄ Collisions at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {5},
   Pages = {845-850},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.845},
   Abstract = {The transverse momentum and total cross section of e+e−
             pairs in the Z-boson region of 66<Mee<116GeV/c2 from pp¯
             collisions at √s=1.8TeV are measured using 110 pb−1 of
             collisions taken by the Collider Detector at Fermilab during
             1992-1995. The total cross section is measured to be 248±11
             pb. The differential transverse momentum cross section is
             compared with calculations that match quantum chromodynamics
             perturbation theory at high transverse momentum with the
             gluon resummation formalism at low transverse momentum. ©
             2000 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.84.845},
   Key = {fds309678}
}

@article{fds313345,
   Author = {al, TAE},
   Title = {``A Measurement of the Differential Dijet Mass Cross Section
             in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,''},
   Journal = {Physical Review},
   Volume = {D61},
   Number = {9},
   Pages = {091101},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevD.61.091101},
   Abstract = {We present a measurement of the cross section for production
             of two or more jets as a function of dijet mass, based on an
             integrated luminosity of 86 (Formula presented) collected
             with the Collider Detector at Fermilab. Our dijet mass
             spectrum is described within errors by next-to-leading order
             QCD predictions using CTEQ4HJ parton distributions, and is
             in good agreement with a similar measurement from the DØ
             experiment. © 2000 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.61.091101},
   Key = {fds313345}
}

@article{fds332111,
   Author = {al, TAE},
   Title = {``Production of $\Upsilon(1S)$ Mesons from $\chi_b$ Decays
             in $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,''},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {10},
   Pages = {2094},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.2094},
   Abstract = {We have reconstructed the radiative decays χb(1P)→
             ϒ(1S)ϒ and χb(2p)→ ϒ(1S)ϒ in p¯p collisions at
             v√s=1.8TeV, and measured the fraction of ϒ(1S) mesons
             that originate from these decays. For ϒ(1S) mesons with
             pϒT>8.0GeV/c, the fractions that come from χb(1P) and
             χb(2P) decays are [27.1±6.9(stat)±4.4(syst)]% and
             [10.5±4.4(stat)±1.4(syst)]%, respectively. We have derived
             the fraction of directly produced ?(1S) mesons to be
             [50.9±8.2(stat)±9.0(syst)]%. © 2000 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.84.2094},
   Key = {fds332111}
}

@article{fds332112,
   Author = {al, TAE},
   Title = {``Search for scalar top quark production in $p\overline p$
             Collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {23},
   Pages = {5273},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.5273},
   Abstract = {We have searched for direct production of scalar top quarks
             at the Collider Detector at Fermilab in 88pb-1of p⊯p
             collisions at vs=1.8TeV. We assume the scalar top quark
             decays into either a bottom quark and a chargino or a bottom
             quark, a lepton, and a scalar neutrino. The event signature
             for both decay scenarios is a lepton, missing transverse
             energy, and at least two b-quark jets. For a chargino mass
             of 90GeV/c2and scalar neutrino masses of at least 40GeV/c2,
             we find no evidence for scalar top production and present
             upper limits on the production cross section in both decay
             scenarios. © 2000 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.84.5273},
   Key = {fds332112}
}

@article{fds332110,
   Author = {al, TAE},
   Title = {``Diffractive dijets with a leading antiproton in
             $p\overline p$ Collisions at $\sqrt{s} = 1.8$
             TeV,''},
   Journal = {Physical Review Letters},
   Volume = {84},
   Number = {22},
   Pages = {5043},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   url = {http://dx.doi.org/10.1103/PhysRevLett.84.5043},
   Abstract = {We report results from a study of events with a leading
             antiproton of beam momentum fraction 0.905 < xF< 0.965 and
             4-momentum transfer squared |t| < 3GeV2produced in ⊯pp
             collisions at ⊡ s = 1800GeV at the Fermilab Tevatron
             collider. Approximately 2% of the events contain two jets of
             transverse energy EjetT> 7GeV. Using the dijet events, we
             evaluate the diffractive structure function of the
             antiproton and compare it with expectations based on results
             obtained in diffractive deep inelastic scattering
             experiments at the DESY ep collider HERA. © 2000 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.84.5043},
   Key = {fds332110}
}

@article{fds313340,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Antos, J and Apollinari, G and Arisawa,
             T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge,
             JP and Berryhill, J and Bertolucci, S and Bevensee, B and Bhatti, A and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker,
             C and Bloom, K and Blumenfeld, B and Blusk, BS and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and van den Brink, S and Bromberg, C and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto,
             G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Cobal, M and Cocca, E and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Guimaraes da Costa and J and Costanzo, D and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F},
   Title = {Measurement of [formula presented] from [formula presented]
             with the CDF detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {61},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   ISSN = {0556-2821},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000086065200013&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {This paper reports an updated measurement of the standard
             model (Formula presented) violation parameter (Formula
             presented) using the CDF Detector at Fermilab. The entire
             run I data sample of (Formula presented) of
             proton-antiproton collisions at (Formula presented) is used
             to identify a signal sample of (Formula presented) events,
             where (Formula presented) and (Formula presented) The flavor
             of the neutral B meson is identified at the time of
             production by combining information from three tagging
             algorithms: a same-side tag, a jet-charge tag, and a
             soft-lepton tag. A maximum likelihood fitting method is used
             to determine (Formula presented) This value of (Formula
             presented) is consistent with the standard model prediction,
             based upon existing measurements, of a large positive
             (Formula presented)-violating asymmetry in this decay mode.
             © 2000 The American Physical Society.},
   Doi = {10.1103/PhysRevD.61.072005},
   Key = {fds313340}
}

@article{fds332114,
   Author = {Ukegawa, F and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar,
             R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl,
             J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
             BL},
   Title = {Measurement of the helicity of W bosons in top quark
             decays},
   Journal = {Physical review letters},
   Volume = {84},
   Number = {2},
   Pages = {216-221},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.84.216},
   Abstract = {We use the transverse momentum spectrum of leptons in the
             decay chain t-->bW with W-->lnu to measure the helicity of
             the W bosons in the top quark rest frame. Our measurement
             uses a t&tmacr; sample isolated in 106+/-4 pb(-1) of data
             collected in p&pmacr; collisions at sqrt[s] = 1.8 TeV with
             the CDF detector at the Fermilab Tevatron. Assuming a
             standard V-A weak decay, we find that the fraction of W's
             with zero helicity in the top rest frame is F0 = 0.91+/-0.
             37(stat)+/-0.13(syst), consistent with the standard model
             prediction of F0 = 0.70 for a top mass of 175
             GeV/c(2).},
   Doi = {10.1103/physrevlett.84.216},
   Key = {fds332114}
}

@article{fds309549,
   Author = {collaboration, CDF},
   Title = {Measurement of the Helicity of W Bosons in Top Quark
             Decays},
   Journal = {Phys.Rev.Lett.},
   Volume = {84},
   Number = {11},
   Pages = {216-221},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.111103},
   Abstract = {http://arXiv.org/ps/hep-ex/9909042},
   Doi = {10.1103/PhysRevD.73.111103},
   Key = {fds309549}
}

@article{fds309680,
   Author = {Alexopoulos, T and Anderson, EW and Biswas, NN and Bujak, A and Carmony,
             DD and Erwin, AR and Findeisen, C and Goshaw, AT and Gulbrandsen, K and Gutay, LJ and Hirsch, AS and Hojvat, C and Jennings, JR and Kenney, VP and Lindsey, CS and LoSecco, JM and Morgan, N and Nelson, K and Oh, SH and Porile, N and Preston, L and Scharenberg, R and Stringfellow, B and Thompson, M and Turkot, F and Walker, WD and Wang, CH and Warchol,
             J},
   Title = {Cross sections for deuterium, tritium, and helium production
             in [formula presented] collisions at [formula presented]
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {62},
   Number = {7},
   Pages = {8},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.62.072004},
   Abstract = {We present the results of a search for the production of
             light elements in (Formula presented) collisions at the
             Fermilab Tevatron collider. Momentum, time of flight, and
             (Formula presented) measurements are used to distinguish
             nuclei from elementary particles. A production ratio for
             deuterium to hydrogen is calculated and compared to the
             primordial value of the big bang model. Some evidence for
             tritium is found and none for helium isotopes. © 2000 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.62.072004},
   Key = {fds309680}
}

@article{fds309681,
   Author = {Brooks, TC and Convery, ME and Davis, WL and Del Signore and KW and Jenkins, TL and Kangas, E and Knepley, MG and Kowalski, KL and Taylor,
             CC},
   Title = {Search for disoriented chiral condensate at the Fermilab
             Tevatron},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {61},
   Number = {3},
   Pages = {1-14},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.61.032003},
   Abstract = {We present results from MiniMax (Fermilab T-864), a small
             test/experiment at the Fermilab Tevatron designed to search
             for the production of a disoriented chiral condensate (DCC)
             in p-(Formula presented) collisions at (Formula presented)
             TeV in the forward direction, (Formula presented) Data,
             consisting of (Formula presented) events, are analyzed using
             the robust observables developed in an earlier paper. The
             results are consistent with generic, binomial-distribution
             partition of pions into charged and neutral species. Limits
             on DCC production in various models are presented. © 2000
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.61.032003},
   Key = {fds309681}
}

@article{fds331222,
   Author = {Abe, F and Akimoto, H and Akopian, A and Albrow, MG and Amendolia, SR and Amidei, D and Antos, J and Aota, S and Apollinari, G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azzi-Bacchetta, P and Bacchetta, N and Bagdasarov, S and Bailey, MW and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Behrends, S and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bertolucci, S and Bettelli, S and Bevensee, B and Bhatti, A and Biery, K and Bigongiari, C and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blusk, S and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Breccia, L and Bromberg, C and Bruner, N and Brunetti, R and Buckley-Geer, E and Budd, HS and Burkett, K and Busetto,
             G and Byon-Wagner, A and Byrum, KL and Campbell, M and Caner, A and Carithers, W and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chang, PS and Chang, PT and Chao, HY and Chapman, J and Cheng,
             MT and Chertok, M and Chiarelli, G and Chiou, CN and Chlebana, F and Christofek, L and Chu, ML and Cihangir, S and Clark, AG and Cobal, M and Cocca, E and Contreras, M and Conway, J and Cooper, J and Cordelli, M and Costanzo, D and Couyoumtzelis, C and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Daniels, T and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Dennino, M and Derwent, PF and Devlin, T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Ely,
             R and Engels, E and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Feng, Z and Ferretti, C and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Frisch, H and Fukui, Y and Gadomski, S and Galeotti, S and Gallinaro, M and Ganel, O and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Geer, S and Gerdes,
             DW and Giannetti, P and Giokaris, N and Giromini, P and Giusti, G and Gold,
             M and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Grassmann,
             H and Green, C and Groer, L and Grosso-Pilcher, C and Guillian, G and Guimaraes da Costa and J and Guo, RS and Haber, C and Hafen, E and Hahn,
             SR and Hamilton, R and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hauser, J and Hayashi, E and Heinrich, J and Heiss, A and Hinrichsen, B and Hoffman,
             KD and Holck, C and Hollebeek, R and Holloway, L and Huang, Z and Huffman,
             BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incagli, M and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Joshi, U and Kajfasz, E and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Kestenbaum, D and Khazins, D and Kikuchi, T and Kirk, M and Kim, BJ and Kim, HS and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Knoblauch, D and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korytov,
             A and Kovacs, E and Kowald, W and Kroll, J and Kruse, M and Kuhlmann, SE and Kuns, E and Kurino, K and Kuwabara, T and Laasanen, AT and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Lanzoni, M and Latino,
             G and LeCompte, T and Lee, AM and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Lockyer, N and Long, O and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lys, J and Maeshima, K and Maksimovic, P and Mangano, M and Mariotti, M and Marriner, JP and Martignon, G and Martin, A and Matthews, JA and Mazzanti, P and McFarland, K and McIntyre, P and Melese, P and Menguzzato, M and Menzione, A and Meschi, E and Metzler, S and Miao, C and Miao, T and Michail, G and Miller, R and Minato, H and Miscetti, S and Mishina, M and Miyashita, S and Moggi, N and Moore, E and Morita, Y and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nakada,
             H and Nakaya, T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CY and Niu, H and Nodulman, L and Nomerotski,
             A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okabe, M and Okusawa, T and Olsen, J and Pagliarone, C and Paoletti, R and Papadimitriou, V and Pappas, SP and Parashar, N and Parri, A and Partos,
             D and Patrick, J and Pauletta, G and Paulini, M and Perazzo, A and Pescara,
             L and Peters, MD and Phillips, TJ and Piacentino, G and Pillai, M and Pitts, KT and Plunkett, R and Pompos, A and Pondrom, L and Proudfoot, J and Ptohos, F and Punzi, G and Ragan, K and Reher, D and Ribon, A and Rimondi,
             F and Ristori, L and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Saab, T and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Scott, A and Scribano,
             A and Segler, S and Seidel, S and Seiya, Y and Semeria, F and Shah, T and Shapiro, MD and Shaw, NM and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Sliwa, K and Smith, C and Snider, FD and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Stanco,
             L and Steele, J and Stefanini, A and Ströhmer, R and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, J and Suzuki, T and Takahashi, T and Takano, T and Takashima, R and Takikawa, K and Tanaka,
             M and Tannenbaum, B and Tartarelli, F and Taylor, W and Tecchio, M and Teng, PK and Teramoto, Y and Terashi, K and Tether, S and Theriot, D and Thomas, TL and Thurman-Keup, R and Timko, M and Tipton, P and Titov, A and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and de Troconiz, JF and Truitt, S and Tseng, J and Turini, N and Uchida, T and Ukegawa, F and Valls, J and van Den Brink,
             SC and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Vologouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Warburton, A and Watanabe, T and Watts, T and Webb, R and Wei, C and Wenzel, H and Wester,
             WC and Wicklund, AB and Wicklund, E and Wilkinson, R and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolinski, D and Wolinski, J and Worm, S and Wu, X and Wyss, J and Yagil, S and Yao, W and Yasuoka, K and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Zanetti, A and Zetti, F and Zucchelli, S and C D F Collaboration},
   Title = {Search for a W' boson via the decay mode W'-->munumu in 1.8
             TeV pp collisions.},
   Journal = {Physical review letters},
   Volume = {84},
   Number = {25},
   Pages = {5716-5721},
   Year = {2000},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.84.5716},
   Abstract = {We report the results of a search for a W' boson produced in
             pp collisions at a center-of-mass energy of 1.8 TeV using a
             107 pb-1 data sample recorded by the Collider Detector at
             Fermilab. We consider the decay channel W'-->&munumu and
             search for anomalous production of high transverse mass
             munumu lepton pairs. We observe no excess of events above
             background and set limits on the rate of W' boson production
             and decay relative to standard model W boson production and
             decay using a fit of the transverse mass distribution
             observed. If we assume standard model strength couplings of
             the W' boson to quark and lepton pairs, we exclude a W'
             boson with invariant mass less than 660 GeV/c2 at 95%
             confidence level.},
   Doi = {10.1103/physrevlett.84.5716},
   Key = {fds331222}
}

@article{fds309679,
   Author = {Akesson, T and Antonov, A and Bondarenko, V and Bytchkov, V and Carling,
             H and Dittus, F and Dolgoshein, B and Dressnandt, N and Ebenstein, WL and Egede, U and Farthouat, P and Froidevaux, D and Gavrilenko, I and Grichkevitch, Y and Hajduk, Z and Hanson, G and Ivochkin, VG and Jagielski, S and Keener, PT and Konovalov, S and Kramarenko, VA and Laritchev, A and Lichard, P and Lundberg, B and Luehring, F and Muraviev, S and Nadtochy, A and Nevski, P and Newcomer, FM and Ogren, H and Oh, SH and Peshekhonov, V and Romaniouk, A and Rousseau, D and Rust, DR and Schegelsky, V and Semenov, S and Shmeleva, A and Smirnov, S and Smirnova, LN and Soderberg, M and Sosnovtsev, V and Spiridenkov, E and Stavrianakou, M and Tartarelli, F and Tikhomirov, V and Berg, RV and Wang, C and Williams, HH},
   Title = {Straw tube drift-time properties and electronics parameters
             for the ATLAS TRT detector},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {449},
   Number = {3},
   Pages = {446-460},
   Publisher = {Elsevier BV},
   Year = {2000},
   Month = {July},
   url = {http://dx.doi.org/10.1016/S0168-9002(99)01470-9},
   Abstract = {The basic drift-time measurement properties of the
             proportional tubes (straws) of the ATLAS TRT detector and
             the impact of the parameters of the front-end electronics on
             performance are discussed. The performance of two different
             front-end electronics prototypes has been studied in detail
             at very high counting rate and is reported
             here.},
   Doi = {10.1016/S0168-9002(99)01470-9},
   Key = {fds309679}
}

@article{fds309673,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den
             Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer,
             E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Cihangir, S and Ciobanu, CI and Clark, AG and Connolly,
             A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and de Jongh, F and dell'Agnello, S and dell'Orso, M and Demina,
             R},
   Title = {Search for new particles decaying to tt̄ in pp̄ collisions
             at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {10},
   Pages = {2062-2067},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.2062},
   Abstract = {The search for narrow-width vector particles was undertaken
             using 106 pb-1 data from the collider detector at Fermilab.
             The cross section upper limits for narrow vector resonances
             decaying to tt are presented. The existence of leptophobic Z
             boson was not included in the top-color-assisted technicolor
             model at the 95% confidence level.},
   Doi = {10.1103/PhysRevLett.85.2062},
   Key = {fds309673}
}

@article{fds340927,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and De
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Van Den
             Brink and S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer,
             E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and Dejongh, F and Dell'Agnello, S and Dell'Orso, M and Demina,
             R},
   Title = {Direct measurement of the W Boson width in pp̄ collisions
             at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {16},
   Pages = {3347-3352},
   Year = {2000},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.3347},
   Abstract = {The W boson width, ΓW obtained in studies of the
             transverse-mass spectra of leptonic W decays is measured.
             Through analysis, the W width is determined from a binned
             log-likelihood fit to the transverse-mass distribution in
             the region 100 < MT < 200 GeV. Including previously
             published computational fluid dynamics (CDF) electron result
             with the same common error yields ΓW = 2.05 ± 0.10(stat)
             ± 0.08(syst) GeV.},
   Doi = {10.1103/PhysRevLett.85.3347},
   Key = {fds340927}
}

@article{fds309669,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den
             Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer,
             E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and de Jongh, F and dell'Agnello, S and dell'Orso,
             M},
   Title = {Measurement of the decay amplitudes of B0 →
             J/ψK*0 and Bs0 → J/ψφ
             decays},
   Journal = {Physical Review Letters},
   Volume = {85},
   Number = {22},
   Pages = {4668-4673},
   Publisher = {American Physical Society (APS)},
   Year = {2000},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.85.4668},
   Abstract = {A full angular analysis of both the B0 and Bs0 decay modes
             was carried out. For this analysis, the B0 → J/ψK*0 and
             Bs0 → J/ψφ decays were reconstructed. The obtained data
             were analyzed in detail.},
   Doi = {10.1103/PhysRevLett.85.4668},
   Key = {fds309669}
}

@article{fds337972,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbara, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
             R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
             T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
             J and Frisch, HJ and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov,
             I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian,
             G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa,
             T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
             T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis, JD and Lindgren,
             M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos, A and Pondrom,
             L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
             F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez,
             C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott,
             A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini,
             A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki,
             T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup,
             A and Tonelli, D and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng,
             J and Turini, N and Ukegawa, F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and III,
             WCW and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Search for narrow diphoton resonances and for γγ+W/Z
             signatures in pp̄ collisions at √s = 1.8
             TeV},
   Journal = {Physical Review D},
   Volume = {64},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/PhysRevD.64.092002},
   Abstract = {We present results of searches for diphoton resonances
             produced both inclusively and also in association with a
             vector boson (W or Z) using 100 pb-1 of pp̄ collisions
             using the CDF detector. We set upper limits on the product
             of cross section times branching ratio for both
             pp̄→γγ+X and pp̄→γγ+ W/Z. Comparing the inclusive
             production to the expectations from heavy sgoldstinos we
             derive limits on the supersymmetry-breaking scale √F in
             the TeV range, depending on the sgoldstino mass and the
             choice of other parameters. Also, using a NLO prediction for
             the associated production of a Higgs boson with a W or Z
             boson, we set an upper limit on the branching ratio for H
             → γγ. Finally, we set a lower limit on the mass of a
             "bosophilic" Higgs boson (e.g., one which couples only to
             γ, W, and Z bosons with standard model couplings) of 82
             GeV/c2 at 95% confidence level. ©2001 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.64.092002},
   Key = {fds337972}
}

@article{fds332108,
   Author = {al, TAE},
   Title = {``Observation of orbitally excited $B$ mesons in \ppb
             collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review},
   Volume = {D64},
   Number = {7},
   Pages = {072002},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/PhysRevD.64.072002},
   Abstract = {We measure the relative rate of production of orbitally
             excited [Formula Presented] states of B mesons [Formula
             Presented] by observing their decays into [Formula
             Presented] We reconstruct B mesons through semileptonic
             decay channels using data collected in [Formula Presented]
             collisions at [Formula Presented] The fraction of light B
             mesons that are produced as [Formula Presented] states is
             measured to be [Formula Presented] We also measure the
             collective mass of the [Formula Presented] states, and
             quantify the result by quoting the (model-dependent) mass of
             the lowest [Formula Presented] state to be [Formula
             Presented] © 2001 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.64.072002},
   Key = {fds332108}
}

@article{fds309365,
   Author = {al, TAE},
   Title = {``Search for the supersymmetric partner of the top quark in
             \pbp collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review},
   Volume = {D63},
   Number = {9},
   Pages = {091101},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/PhysRevD.63.091101},
   Abstract = {We report on a search for the supersymmetric partner of the
             top quark (top squark) produced in [Formula Presented]
             events using [Formula Presented] of [Formula Presented]
             collisions at [Formula Presented] recorded with the Collider
             Detector at Fermilab. In the case of a light top squark, the
             decay of the top quark into a top squark plus the lightest
             supersymmetric particle (LSP) could have a significant
             branching ratio. The observed events are consistent with
             standard model [Formula Presented] production and decay.
             Hence, we set limits on the branching ratio of the top quark
             decaying into a top squark plus LSP, excluding branching
             ratios above 45% for a LSP mass up to [Formula Presented] ©
             2001 The American Physical Society.},
   Doi = {10.1103/PhysRevD.63.091101},
   Key = {fds309365}
}

@article{fds313342,
   Author = {al, TAE},
   Title = {``Tests of enhanced leading order QCD in $W$ boson plus jets
             events from 1.8 TeV \pbp collisions,''},
   Journal = {Physical Review},
   Volume = {D63},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/PhysRevD.63.072003},
   Abstract = {We present a study of events with W bosons and hadronic jets
             produced in [Formula Presented] collisions at a center of
             mass energy of 1.8 TeV. The data consist of 51400 [Formula
             Presented] decay candidates from 108 [Formula Presented] of
             integrated luminosity collected using the CDF detector at
             the Fermilab Tevatron collider. Cross sections and jet
             production properties have been measured for [Formula
             Presented] to [Formula Presented] jet events. The data
             compare well to predictions of leading-order QCD matrix
             element calculations with added gluon radiation and
             simulated parton fragmentation. © 2001 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.63.072003},
   Key = {fds313342}
}

@article{fds309646,
   Author = {al, TAE},
   Title = {``Double Diffraction Dissociation at the Fermilab Tevatron
             Collider,''},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {14},
   Pages = {141802},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/physrevlett.87.141802},
   Abstract = {We present results from a measurement of double diffraction
             dissociation in pp collisions at the Fermilab Tevatron
             collider. The production cross section for events with a
             central pseudorapidity gap of width Deltaeta(0)>3
             (overlapping eta = 0) is found to be 4.43+/-0.02(stat)+/-1.18(syst)
             mb [ 3.42+/-0.01(stat)+/-1.09(syst) mb] at square root of
             (s) = 1800[630] GeV. Our results are compared with previous
             measurements and with predictions based on Regge theory and
             factorization.},
   Doi = {10.1103/physrevlett.87.141802},
   Key = {fds309646}
}

@article{fds309647,
   Author = {al, TAE},
   Title = {``Measurement of the Top Quark $p_T$ Distribution,''},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {10},
   Pages = {102001},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/physrevlett.87.102001},
   Abstract = {We have measured the p(T) distribution of top quarks that
             are pair produced in pp collisions at sqrt[s] = 1.8 TeV
             using a sample of tt decays in which we observe a single
             high- p(T) charged lepton, a neutrino, and four or more
             jets. We use a likelihood technique that corrects for the
             experimental bias introduced due to event reconstruction and
             detector resolution effects. The observed distribution is
             consistent with the standard model prediction. We use these
             data to place limits on the production of high- p(T) top
             quarks suggested in some models of anomalous top quark pair
             production.},
   Doi = {10.1103/physrevlett.87.102001},
   Key = {fds309647}
}

@article{fds309648,
   Author = {al, TAE},
   Title = {``Search for Neutral Supersymmetric Higgs Bosons in \ppb
             Collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review Letters},
   Volume = {86},
   Number = {20},
   Pages = {4472},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/physrevlett.86.4472},
   Abstract = {We present the results of a search for neutral Higgs bosons
             produced in association with b quarks in pp-->bb(phi)-->bbb
             final states with 91+/-7 pb(-1) of pp collisions at sqrt[s]
             = 1.8 TeV recorded by the Collider Detector at Fermilab. We
             find no evidence of such a signal and the data are
             interpreted in the context of the neutral Higgs sector of
             the minimal supersymmetric extension of the standard model.
             With basic parameter choices for the supersymmetric scale
             and the stop-quark mixing, we derive 95% C.L. lower mass
             limits for neutral Higgs bosons for tan(beta) values in
             excess of 35.},
   Doi = {10.1103/physrevlett.86.4472},
   Key = {fds309648}
}

@article{fds309649,
   Author = {al, TAE},
   Title = {``First Measurement of the Ratio $B(t \ra Wb)/B(t\ra Wq)$
             and Associated Limit on the Cabibbo-Kobayashi-Maskawa
             Element $|V_{tb}|$,''},
   Journal = {Physical Review Letters},
   Volume = {86},
   Number = {15},
   Pages = {3233},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/physrevlett.86.3233},
   Abstract = {We present the first measurement of the ratio of branching
             fractions R identical withB(t-->Wb)/B(t-->Wq) from p_p
             collisions at sqrt[s] = 1.8 TeV. The data set corresponds to
             109 pb(-1) of data recorded by the Collider Detector at
             Fermilab during the 1992-95 Tevatron run. We measure R =
             0.94(+0.31)(-0.24)(stat+syst) or R>0.61 (0.56) at 90% (95)%
             C.L., in agreement with the standard model predictions. This
             measurement yields a limit on the Cabibbo-Kobayashi-Maskawa
             quark mixing matrix element /V(tb)/ under the assumption of
             three generations and unitarity.},
   Doi = {10.1103/physrevlett.86.3233},
   Key = {fds309649}
}

@article{fds326141,
   Author = {al, TAE},
   Title = {``Measurement of the two-jet differential cross section in
             \ppb collisions at $\sqrt{s} = 1800$ GeV,''},
   Journal = {Physical Review},
   Volume = {D64},
   Number = {1},
   Pages = {012001},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/PhysRevD.64.012001},
   Abstract = {A measurement is presented of the two-jet differential cross
             section [Formula Presented] at center of mass energy
             [Formula Presented] GeV in [Formula Presented] collisions.
             The results are based on an integrated luminosity of 86
             [Formula Presented] collected during 1994 to 1995 by the CDF
             Collaboration at the Fermilab Tevatron collider. The
             differential cross section is measured as a function of the
             transverse energy [Formula Presented] of a jet in the
             pseudorapidity region [Formula Presented] for four different
             pseudorapidity bins of a second jet restricted to [Formula
             Presented] The results are compared with next-to-leading
             order QCD calculations determined using the CTEQ4 and MRST
             sets of parton distribution functions. None of the sets
             examined in this analysis provides a good description of the
             data. © 2001 The American Physical Society.},
   Doi = {10.1103/PhysRevD.64.012001},
   Key = {fds326141}
}

@article{fds309655,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Bruner,
             N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang,
             PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
             T and Dittmann, JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Errede, D and Errede, S and Fan, Q and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Gorelov, I and Giromini, P and Glagolev,
             V and Gold, M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Gris, P and Groer, L and Grosso-Pilcher,
             C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haas, RM and Haber, C and Hafen, E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss,
             A and Herndon, M and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
             T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn,
             P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn,
             A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte,
             T and Lee, AM and Lee, K and Leone, S and Lewis, JD and Lindgren, M and Liss,
             TM and Liu, JB and Liu, YC and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak,
             R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer,
             J and Mazzanti, P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nahn, S and Nakada, H and Nakaya, T and Nakano, I and Nelson, C and Nelson, T and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari,
             F and Paoletti, R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos, A and Pondrom,
             L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
             F and Pukhov, O and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
             M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
             S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Tollefson, K and Tollestrup, A and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
             F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Vidal, R and Vilar, R and Volobouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang,
             MJ and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Williams, HH and Wilson,
             P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu,
             Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Tests of enhanced leading order QCD in W boson plus jets
             events from 1.8 TeV p̄p collisions},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {63},
   Number = {7},
   Pages = {720031-7200329},
   Year = {2001},
   Abstract = {We present a study of events with W bosons and hadronic jets
             produced in p̄p collisions at a center of mass energy of
             1.8 TeV. The data consist of 51400 W → e ν decay
             candidates from 108 pb-1 of integrated luminosity collected
             using the CDF detector at the Fermilab Tevatron collider.
             Cross sections and jet production properties have been
             measured for W + ≥ 1 to ≥ 4 jet events. The data compare
             well to predictions of leading-order QCD matrix element
             calculations with added gluon radiation and simulated parton
             fragmentation.},
   Key = {fds309655}
}

@article{fds309657,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Borras, K and Bortoletto,
             D and Boudreau, J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro,
             A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Convery, ME and Conway, J and Cordelli, M and Cranshaw,
             J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Dominguez,
             A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov,
             I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian,
             G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa,
             T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
             T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis, JD and Lindgren,
             M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
             A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
             J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Roy,
             A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg,
             D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
             A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
             AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
             J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
             L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
             F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi,
             G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
             D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Observation of diffractive J/ψ production at the Fermilab
             Tevatron},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {24},
   Pages = {2418021-2418026},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/physrevlett.87.241802},
   Abstract = {The first observation of diffractive J/ψ(→μ+μ-)
             production in p̄p collisions at s√=1.8 TeV was presented.
             Events were selected with a pair of muon candidates using a
             three-level dimuon trigger system. The dimuon mass
             distribution was fitted with a sum of a Gaussian and a
             linear function to evaluate the fraction of background
             events in the signal region. A value of 0.59±0.15 for the
             gluon fraction of the diffractive structure function of the
             proton was extracted.},
   Doi = {10.1103/physrevlett.87.241802},
   Key = {fds309657}
}

@article{fds309658,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SV and Bromberg, C and Brozovic, M and Brubaker,
             E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera,
             S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
             AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
             YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
             T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Engels, E and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
             RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
             J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
             AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
             T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis, JD and Lindgren,
             M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos,
             A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
             J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Roy,
             A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg,
             D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
             A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
             AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
             J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
             L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
             F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi,
             G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
             D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Charged-particle multiplicity p p̄ collisions at √s = 1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {21},
   Pages = {2118041-2118046},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/physrevlett.87.211804},
   Abstract = {The mean charged-particle multiplicity of jets in dijet
             events with dijet masses were analyzed using collider
             detectors. The jet energy and direction were measured in the
             central lead-scintillator electromagnetic (CEM) and
             iron-scintillator hadronic (CHA) calorimeters. It is shown
             that the fraction of gluon jets decreases to 23%-26% at 630
             GeV/c2 from 61%-63% of all jets at 80 GeV/c2.},
   Doi = {10.1103/physrevlett.87.211804},
   Key = {fds309658}
}

@article{fds309659,
   Author = {al, TAE},
   Title = {``Search for Quark-Lepton Compositeness and a Heavy
             $W^\prime$ Boson Using the $e \nu$ Channel in \ppb
             Collisions at $\sqrt{s} = 1.8$ TeV,''},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {23},
   Pages = {231803},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/physrevlett.87.231803},
   Abstract = {A study on searches for quark-lepton compositeness and a
             heavy boson at high electron-neutrino transverse mass was
             presented. The data collected in pp̄ collisions at √s=1.8
             TeV was used for the analysis. The data obtained is found to
             be consistent with the standard model (SM)
             predictions.},
   Doi = {10.1103/physrevlett.87.231803},
   Key = {fds309659}
}

@article{fds309662,
   Author = {Schmieg, SJ and Cho, BK and Oh, SH},
   Title = {Hydrocarbon reactivity in a plasma-catalyst system: Thermal
             versus plasma-assisted lean NOx reduction},
   Journal = {SAE Technical Papers},
   Year = {2001},
   url = {http://dx.doi.org/10.4271/2001-01-3565},
   Abstract = {The steady-state reduction of NOx at temperatures between
             150-300°C has been investigated under simulated lean-burn
             conditions using a two-stage transient flow reactor system
             consisting of non-thermal plasma in combination with a
             sodium Y zeolite catalyst. Reactivity comparisons were made
             with and without plasma operation in order to identify the
             plasma-generated hydrocarbon species necessary for the
             selective catalytic reduction (SCR) of NOx. With propene as
             the hydrocarbon in the feed, NO is completely oxidized to
             NO2 in the plasma and the formation of oxidized
             carbon-containing species include formaldehyde,
             acetaldehyde, carbon monoxide, carbon dioxide, and methanol.
             Fourier transform infrared (FTIR) measurements indicate a
             close carbon balance between plasma inlet and outlet gas
             feed concentrations, signifying the major species have been
             identified. Plasma-assisted NOx conversion over the sodium Y
             zeolite catalyst is improved with supplemental acetaldehyde
             injection, primarily through the removal of NO from the feed
             stream. In addition, the thermal (no plasma) reduction of NO
             is much greater with acetaldehyde as the reductant compared
             to propene, demonstrating that the NOx reduction reaction is
             controlled by the acetaldehyde present in the gas feed. The
             thermal catalytic NOx conversion with acetaldehyde in a
             NO-containing feed is much higher than that in a
             NO2-containing feed, indicating that plasma conversion of NO
             to NO2 is not required for NOx reduction. The higher
             activity of NO is due to the increased formation of HCN, a
             partial reduction product that can be removed using a
             downstream Pt/Al2O3 catalyst. Octane, which is more
             representative of hydrocarbons found in diesel fuel/exhaust,
             forms acetaldehyde over the catalyst and yields comparable
             NO x reduction activity. At similar acetaldehyde
             concentration levels entering the catalyst, thermal NOx
             conversion with the feed containing NO and acetaldehyde is
             comparable to the plasma-assisted NO x conversion efficiency
             with the feed containing propene and NO, suggesting that an
             appropriate hydrocarbon can reduce NO without the use of
             non-thermal plasma. Copyright © 2001 Society of Automotive
             Engineers, Inc.},
   Doi = {10.4271/2001-01-3565},
   Key = {fds309662}
}

@article{fds332107,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandi, A and Brink,
             SVD and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demina, R and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann,
             JR and Donati, S and Done, J and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erdmann, W and Errede, D and Errede, S and Fan, Q and Feild, RG and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Geer,
             S and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Gold,
             M and Goldstein, J and Gordon, A and Goshaw, AT and Gotra, Y and Goulianos,
             K and Green, C and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Guo, RS and Haas, RM and Haber, C and Hafen,
             E and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Herndon, M and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jensen, H and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kirby, M and Kirk, M and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Koehn, P and Köngeter, A and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lamoureux, JI and Lancaster, M and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis, JD and Lindgren, M and Liss, TM and Liu, JB and Liu,
             YC and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Musy, M and Nachtman, J and Nahn, S and Nakada, H and Nakaya,
             T and Nakano, I and Nelson, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nicolaidi, P and Niu, H and Nodulman, L and Nomerotski, A and Oh, SH and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen,
             J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pappas, SP and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Plunkett, R and Pompos, A and Pondrom,
             L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot, J and Ptohos,
             F and Pukhov, O and Punzi, G and Ragan, K and Rakitine, A and Reher, D and Reichold, A and Riegler, W and Ribon, A and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Safonov, A and Sakumoto,
             WK and Saltzberg, D and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Siegrist, J and Signorelli, G and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu,
             M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Taylor, W and Tecchio, M and Teng, PK and Terashi, K and Tether, S and Theriot, D and Thurman-Keup, R and Tipton, P and Tkaczyk,
             S and Tollefson, K and Tollestrup, A and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa, F and Vaiciulis,
             T and Valls, J and III, SV and Velev, G and Vidal, R and Vilar, R and Volobouev, I and Vucinic, D and Wagner, RG and Wagner, RL and Wahl, J and Wallace, NB and Walsh, AM and Wang, C and Wang, CH and Wang, MJ and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and III,
             WCW and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yagil, A and Yao, W and Yeh,
             GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu,
             Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Measurement of the W boson mass with the collider detector
             at Fermilab},
   Journal = {Physical Review D},
   Volume = {64},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2001},
   url = {http://dx.doi.org/10.1103/PhysRevD.64.032001},
   Abstract = {We present a measurement of the W boson mass using data
             collected with the CDF detector during the 1994-1995
             collider run at the Fermilab Tevatron. A fit to the
             transverse mass spectrum of a sample of 30115 W → ev
             events recorded in an integrated luminosity of 84 pb-1 gives
             a mass MW=80.473±0.065(stat) ±0.092(syst) GeV/c2. A fit to
             the transverse mass spectrum of a sample of 14740 W → μν
             events from 80 pb-1 gives a mass MW=80.465±0.100(stat)±0.103(syst)
             GeV/c2. The dominant contributions to the systematic
             uncertainties are the uncertainties in the electron energy
             scale and the muon momentum scale, 0.075 GeV/c2 and 0.085
             GeV/c2, respectively. The combined value for the electron
             and muon channel is MW=80.470±0.089 GeV/c2. When combined
             with previously published CDF measurements, we obtain
             MW=80.433±0.079GeV/c2. ©2001 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.64.032001},
   Key = {fds332107}
}

@article{fds309651,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den
             Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer,
             E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Cassada, J and Castro,
             A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, M and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cooper, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and DeJongh, F and Dell’Agnello, S and Dell’Orso,
             M},
   Title = {Measurement of [Formula Presented] for high mass Drell-Yan
             [Formula Presented] pairs from [Formula Presented]
             collisions at [Formula Presented] TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {63},
   Number = {1},
   Pages = {111011-111016},
   Year = {2001},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.63.011101},
   Abstract = {We report on the first measurement of the rapidity
             distribution [Formula Presented] over nearly the entire
             kinematic region of rapidity for [Formula Presented] pairs
             in both the Z-boson region of [Formula Presented] and in the
             high mass region of [Formula Presented] The data sample
             consists of 108 [Formula Presented] of [Formula Presented]
             collisions at [Formula Presented] TeV taken by the Collider
             Detector at Fermilab during 1992–1995. The total cross
             section in the Z-boson region is measured to be [Formula
             Presented] pb. The measured total cross section and [Formula
             Presented] are compared with quantum chromodynamics
             calculations in leading and higher orders. © 2000 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.63.011101},
   Key = {fds309651}
}

@article{fds309654,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
             J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
             S},
   Title = {Production of χc1 and χc2 in pp̄
             collisions at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {86},
   Number = {18},
   Pages = {3963-3968},
   Year = {2001},
   Month = {April},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.86.3963},
   Abstract = {The charmonium system was studied by measuring the relative
             cross sections of the Xc1 and Xc2 produced in pp collisions
             at √ s = 1.8 TeV. As a result, the ratio of production
             cross sections was established.},
   Doi = {10.1103/PhysRevLett.86.3963},
   Key = {fds309654}
}

@article{fds309653,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
             J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D},
   Title = {Search for the supersymmetric partner of the top quark in
             pp̄ collisions at √s=1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {63},
   Number = {9},
   Pages = {911011-911016},
   Year = {2001},
   Month = {August},
   Abstract = {We report on a search for the supersymmetric partner of the
             top quark (top squark) produced in tt̄ events using 110
             pb-1 of pp̄ collisions at √s = 1.8 TeV recorded with the
             Collider Detector at Fermilab. In the case of a light top
             squark, the decay of the top quark into a top squark plus
             the lightest supersymmetric particle (LSP) could have a
             significant branching ratio. The observed events are
             consistent with standard model tt̄ production and decay.
             Hence, we set limits on the branching ratio of the top quark
             decaying into a top squark plus LSP, excluding branching
             ratios above 45% for a LSP mass up to 40
             GeV/c2.},
   Key = {fds309653}
}

@article{fds309660,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and De
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Van Den Brink and S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
             R and Dagenhart, D and D'Auria, S and DeJongh, F},
   Title = {Measurement of dσ/dM and forward-backward charge asymmetry
             for high-mass Drell-Yan e+e- pairs
             from pp̄ collisions at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {87},
   Number = {13},
   Pages = {131802/1-131802/6},
   Year = {2001},
   Month = {September},
   Abstract = {An overview is given on the measurements of dσ/dM and
             improvement of the existing measurements of AFB. All the
             measurements have been taken by the Collider Detector at
             Fermilab (CDF). The measurements of e+e- pairs with
             invariant masses between 40 and 500 eV/c2 complement
             measurements in e+e- machines, that currently extend to 200
             GeV/c2.},
   Key = {fds309660}
}

@article{fds309661,
   Author = {Akesson, T and Arik, E and Assamagan, K and Baker, K and Barberio, E and Barberis, D and Bertelsen, H and Bytchkov, V and Callahan, J and Catinaccio, A and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Ebenstein, WL and Eerola, P and Farthouat, P and Froidevaux, D and Grichkevitch, Y and Hajduk, Z and Hansen, JR and Keener, PT and Kekelidze, G and Konovalov, S and Kowalski, T and Kramarenko, VA and Krivchitch, A and Laritchev, A and Lichard, P and Lucotte, A and Lundberg, B and Luehring, F and Mailov, A and Manara, A and McFarlane, K and Mitsou, VA and Morozov, S and Muraviev, S and Nadtochy,
             A and Newcomer, FM and Olszowska, J and Ogren, H and Oh, SH and Peshekhonov, V and Rembser, C and Romaniouk, A and Rousseau, D and Rust,
             DR and Schegelsky, V and Sapinski, M and Shmeleva, A and Smirnov, S and Smirnova, LN and Sosnovtsev, V and Soutchkov, S and Spiridenkov, E and Tikhomirov, V and Van Berg and R and Vassilakopoulos, V and Wang, C and Williams, HH},
   Title = {Particle identification using the time-over-threshold method
             in the ATLAS transition radiation tracker},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {474},
   Number = {2},
   Pages = {172-187},
   Publisher = {Elsevier BV},
   Year = {2001},
   Month = {December},
   url = {http://dx.doi.org/10.1016/S0168-9002(01)00878-6},
   Abstract = {Test-beam studies of the ATLAS Transition Radiation Tracker
             (TRT) straw tube performance in terms of electron-pion
             separation using a time-over-threshold method are described.
             The test-beam data are compared with Monte Carlo simulations
             of charged particles passing through the straw tubes of the
             TRT. For energies below 10 GeV, the time-over-threshold
             method combined with the standard transition-radiation
             cluster-counting technique significantly improves the
             electron-pion separation in the TRT. The use of the
             time-over-threshold information also provides some kaon-pion
             separation, thereby significantly enhancing the B-physics
             capabilities of the ATLAS detector. © 2001 Elsevier Science
             B.V. All rights reserved.},
   Doi = {10.1016/S0168-9002(01)00878-6},
   Key = {fds309661}
}

@article{fds332106,
   Author = {al, TAE},
   Title = {Cross section and heavy quark composition of gamma+ mu
             events produced in pp collisions},
   Journal = {Physical Review},
   Volume = {D65},
   Number = {1},
   Pages = {012003},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.012003},
   Abstract = {We present a measurement of the cross section and the first
             measurement of the heavy flavor content of associated direct
             photon 1 muon events produced in hadronic collisions. These
             measurements come from a sample of 1.8 TeV pp̅ collisions
             recorded with the Collider Detector at Fermilab. Quantum
             chromodynamics (QCD) predicts that these events are
             primarily due to the Compton scattering process cg→ γ+μ,
             with the final-state charm quark producing a muon. The cross
             section for events with a photon transverse momentum between
             12 and 40 GeV/c is measured to be 46.8±6.3±7.5 pb, which
             is two standard deviations below the most recent theoretical
             calculation. A significant fraction of the events in the
             sample contain a final-state bottom quark. The ratio of
             charm to bottom production is measured to be 2.4±1.2, in
             good agreement with QCD models.},
   Doi = {10.1103/PhysRevD.65.012003},
   Key = {fds332106}
}

@article{fds331217,
   Author = {al, DAE},
   Title = {Upsilon Production and Polarization in pp Collisions at
             $\sqrt{s} = 1.8TeV},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {16},
   Pages = {161802},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/physrevlett.88.161802},
   Abstract = {We report on measurements of the Upsilon(1S), Upsilon(2S),
             and Upsilon(3S) differential cross sections
             (d(2)sigma/dp(T)dy)(/y/<0.4), as well as on the Upsilon(1S)
             polarization in p p macro collisions at square root of s =
             1.8 TeV using a sample of 77+/-3 pb(-1) collected by the
             collider detector at Fermilab. The three resonances were
             reconstructed through the decay Upsilon-->mu(+)mu(-). The
             measured angular distribution of the muons in the
             Upsilon(1S) rest frame is consistent with unpolarized meson
             production.},
   Doi = {10.1103/physrevlett.88.161802},
   Key = {fds331217}
}

@article{fds331218,
   Author = {al, TAE},
   Title = {Searches for new physics in events with a photon and b-quark
             jet at CDF},
   Journal = {Physical Review},
   Volume = {D65},
   Number = {5},
   Pages = {052006},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.052006},
   Abstract = {We have searched for evidence of physics beyond the standard
             model in events that include an energetic photon and an
             energetic b-quark jet, produced in 85 pb-1 of (image found)
             collisions at 1.8 TeV at the Tevatron Collider at Fermilab.
             This signature, containing at least one gauge boson and a
             third-generation quark, could arise in the production and
             decay of a pair of new particles, such as those predicted by
             supersymmetry, leading to a production rate exceeding
             standard model predictions. We also search these events for
             anomalous production of missing transverse energy,
             additional jets and leptons (e, µ and τ), and additional b
             quarks. We find no evidence for any anomalous production of
             γb or γb+X events. We present limits on two supersymmetric
             models: a model where the photon is produced in the decay
             (equation found), and a model where the photon is produced
             in the neutralino decay into the gravitino LSP, (equation
             found). We also present our limits in a model-independent
             form and test methods of applying model-independent
             limits.},
   Doi = {10.1103/PhysRevD.65.052006},
   Key = {fds331218}
}

@article{fds331219,
   Author = {al, DAE},
   Title = {Study of the heavy flavor content of jets produced in
             association with W bosons in pp collisions at $\sqrt{s} =
             1.8 TeV},
   Journal = {Physical Review},
   Volume = {D65},
   Number = {5},
   Pages = {052006},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.052007},
   Abstract = {We present a detailed examination of the heavy flavor
             content of the W+jet data sample collected with the Collider
             Detector at Fermilab during the 1992-1995 collider run at
             the Fermilab Tevatron. Jets containing heavy flavor quarks
             are selected via the identification of secondary vertices or
             semileptonic decays of b and c quarks. There is generally
             good agreement between the rates of secondary vertices and
             soft leptons in the data and in the standard model
             simulation including single and pair production of top
             quarks. An exception is the number of events in which a
             single jet has both a soft lepton and a secondary vertex
             tag. In W+2,3 jet data, we find 13 such events where we
             expected 4.4± 0.6 events. The kinematic properties of this
             small sample of events are statistically difficult to
             reconcile with the simulation of standard model
             processes.},
   Doi = {10.1103/PhysRevD.65.052007},
   Key = {fds331219}
}

@article{fds331220,
   Author = {al, TAE},
   Title = {Measurement of the Strong Coupling Constant from Inclusive
             Jet Production at the Tevatron pb Collider},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {4},
   Pages = {042001},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/physrevlett.88.042001},
   Abstract = {We report a measurement of the strong coupling constant,
             alpha(s)(MZ), extracted from inclusive jet production in pp
             collisions at square root[s] = 1800 GeV. The QCD prediction
             for the evolution of alpha(s) with jet transverse energy ET
             is tested over the range 40<ET<450 GeV using ET for the
             renormalization scale. The data show good agreement with QCD
             in the region below 250 GeV. The value of alpha(s) at the
             mass of the Z0 boson averaged over the range 40<ET<250 GeV
             is found to be alpha(s)(MZ) = 0.1178+/-0.0001(stat)+0.0081(-0.0095)(expt.
             syst). The associated theoretical uncertainties are mainly
             due to the choice of renormalization scale ((+6%)(-4%)) and
             input parton distribution functions (5%).},
   Doi = {10.1103/physrevlett.88.042001},
   Key = {fds331220}
}

@article{fds331221,
   Author = {al, TAE},
   Title = {Search for Gluinos and Scalar Quarks in pp Collisionsat
             $\sqrt{s} = 1.8 TeV Using the Missing Energy plus Multijets
             Signature},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {4},
   Pages = {041801},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/physrevlett.88.041801},
   Abstract = {We have performed a search for gluinos (g) and scalar quarks
             (q) in a data sample of 84 pb(-1) of pp collisions at square
             root[s] = 1.8 TeV, recorded by the Collider Detector at
             Fermilab. We investigate the final state of large missing
             transverse energy and three or more jets, a characteristic
             signature in R-parity-conserving supersymmetric models. The
             analysis has been performed "blind," in that the inspection
             of the signal region is made only after the predictions from
             standard model backgrounds have been calculated. Comparing
             the data with predictions of constrained supersymmetric
             models, we exclude gluino masses below 195 GeV/c2 (95%
             C.L.), independent of the squark mass. For the case m(q)
             approximately m(g), gluino masses below 300 GeV/c2 are
             excluded.},
   Doi = {10.1103/physrevlett.88.041801},
   Key = {fds331221}
}

@article{fds309631,
   Author = {al, DAE},
   Title = {Search for New Physics in Photon-Lepton Events in pp
             Collisions at $\sqrt{s} = 1.8TeV,},
   Journal = {Physical Review Letters},
   Volume = {89},
   Number = {4},
   Pages = {041802},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/physrevlett.89.041802},
   Abstract = {We present the results of a search in pp collisions at
             sqrt[s] = 1.8 TeV for anomalous production of events
             containing a photon and a lepton (e or mu), both with large
             transverse energy, using 86 pb(-1) of data collected with
             the Collider Detector at Fermilab during the 1994-1995
             collider run at the Fermilab Tevatron. The presence of large
             missing transverse energy (E(T)), additional photons, or
             additional leptons in these events is also analyzed. The
             results are consistent with standard model expectations,
             with the possible exception of photon-lepton events with
             large E(T), for which the observed total is 16 events and
             the expected mean total is 7.6+/-0.7 events.},
   Doi = {10.1103/physrevlett.89.041802},
   Key = {fds309631}
}

@article{fds309633,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Dominguez,
             A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan, Q and Fang, HC and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes,
             DW and Giannetti, P and Giordani, MP and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
             AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Heiss, A and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Ivanov, A and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Karr, K and Kartal, S and Kasha,
             H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
             MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Lee, AM and Lee, K and Leone, S and Lewis,
             JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
             K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Miyazaki, Y and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
             A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
             J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Renton, P and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi,
             L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt,
             MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima,
             M and Shochet, M and Sidoti, A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter, AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding, J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka,
             M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi,
             K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli,
             D and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Vaiciulis, T and Valls, J and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar,
             R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner,
             RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters, D and Watts, T and Webb, R and Wenzel, H and Wester, WC and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss,
             J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Search for the decay Bs→μ+μ-φ
             in pp̄ collisions at √s = 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {11},
   Pages = {1111011-1111016},
   Year = {2002},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.111101},
   Abstract = {We present a search for the flavor-changing neutral current
             decay Bs→μ+μ-φ in pp̄ collisions at √s = 1.8 TeV,
             using 91 pb-1 of data collected at the Collider Detector at
             Fermilab (CDF). We find two candidate events for this decay,
             which are consistent with the background estimate of one
             event, and set an upper limit on the branching fraction of
             B(Bs→ μ+μ-φ)&lt;6.7×10-5 at a 95% confidence level.
             This is the first limit on the branching fraction of this
             decay.},
   Doi = {10.1103/PhysRevD.65.111101},
   Key = {fds309633}
}

@article{fds309635,
   Author = {al, DAE},
   Title = {Diffractive Dijet Production at $\sqrt{s} = 630 and 1800 GeV
             at the Fermilab Tevatron},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {15},
   Pages = {151802},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/physrevlett.88.151802},
   Abstract = {The diffractive dijet production at √s = 630 and 1800 GeV
             at the Fermilab Tevatron was presented. The β and ξ
             dependence of the diffractive structure function at √s =
             1800 GeV and it was found that it obeyed β-ξ factorization
             for β&lt;0.5. Results showed that the ξ-0.9±0.1
             dependence indicated that Pomeron-like behavior extended to
             moderately high ξ values in diffractive dijet
             production.},
   Doi = {10.1103/physrevlett.88.151802},
   Key = {fds309635}
}

@article{fds309641,
   Author = {al, TAE},
   Title = {Search for New Heavy Particles in the W Z0 Final State in pp
             Collisions at $\sqrt{s} = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {7},
   Pages = {071806},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/physrevlett.88.071806},
   Abstract = {The general search for new heavy particles, X, was
             presented. The data collected by the Collider Detector at
             Fermilab showed no evidence for production of X in 110 pb-1.
             As a function of mass and width of new particle, the general
             cross section limits were set at 95% C.L. An analysis of
             results as mass limits on the production of new heavy
             charged vector bosons was presented.},
   Doi = {10.1103/physrevlett.88.071806},
   Key = {fds309641}
}

@article{fds309642,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin, T and Dittmann, JR and Dominguez, A and Donati,
             S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan,
             Q and Fang, HC and Feild, RG and Fernandez, JP and Ferretti, C and Field,
             RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman,
             J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov,
             I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian,
             G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa,
             T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Huffman, BT and Hughes, R and Huston,
             J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon,
             T and Kaneko, T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim,
             MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis,
             JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
             K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
             P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
             A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
             J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto,
             WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
             M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
             S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
             A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
             AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
             J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
             L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
             H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
             F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
             D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
   Title = {Study of B0 → J/ψK(*)0π+π-
             decays with the collider detector at Fermilab},
   Journal = {Physical Review Letters},
   Volume = {88},
   Number = {7},
   Pages = {718011-718016},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/physrevlett.88.071801},
   Abstract = {The study of the decays B0 → J/ψK(*)0 π+π-, was
             reported. The study involved the creation of a uū or dd̄
             quark pair in addition to a b̄ → c̄(cs̄) decay.
             Three-level dimuon trigger was used in the analysis. Events
             with two separate sets of atleast three linked hits in the
             muon chambers. The second level required drift chamber
             tracks with pT &gt; 2.0 GeV/c. J/ψ → μ+μ- candidates,
             were accepted in the third level, with a reconstructed
             invariant mass between 2.8 and 3.8 GeV/c2.},
   Doi = {10.1103/physrevlett.88.071801},
   Key = {fds309642}
}

@article{fds332105,
   Author = {al, DAE},
   Title = {Measurement of the B+ total cross section and B+
             differential cross section do/dpT in pp collisions at
             $\sqrt{s} = 1.8 TeV},
   Journal = {Physical Review},
   Volume = {D65},
   Number = {5},
   Pages = {052005},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.052005},
   Abstract = {We present measurements of the [Formula Presented] meson
             total cross section and differential cross section [Formula
             Presented] The measurements use a [Formula Presented]
             [Formula Presented] sample of [Formula Presented] collisions
             at [Formula Presented] collected by the CDF detector.
             Charged B meson candidates are reconstructed through the
             decay [Formula Presented] with [Formula Presented] The total
             cross section, measured in the central rapidity region
             [Formula Presented] for [Formula Presented] is [Formula
             Presented] The measured differential cross section is
             substantially larger than typical QCD predictions calculated
             to next-to-leading order. © 2002 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.65.052005},
   Key = {fds332105}
}

@article{fds332101,
   Author = {al, DAE},
   Title = {``Cross section for forward J/$ production in pp collisions
             at $\sqrt{s} = 1.8 TeV,''},
   Journal = {Physical Review},
   Volume = {D66},
   Number = {9},
   Pages = {092001},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.092001},
   Abstract = {The inclusive cross section for [Formula Presented]
             production times the branching ratio [Formula Presented] has
             been measured in the forward pseudorapidity region: [Formula
             Presented] The results are based on [Formula Presented] of
             data collected by the CDF Collaboration at the Fermilab
             Tevatron Collider. The measurements extend earlier
             measurements of the D0 Collaboration to higher [Formula
             Presented] In the kinematic range where the experiments
             partially overlap, these data are in good agreement with
             previous measurements. © 2002 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.66.092001},
   Key = {fds332101}
}

@article{fds332102,
   Author = {al, DAE},
   Title = {``Branching ratio measurements of exclusive B+ decays to
             charmonium with the Collider Detector at
             Fermilab},
   Journal = {Physical Review},
   Volume = {D66},
   Number = {66},
   Pages = {052005},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.052005},
   Abstract = {We report on measurements of the branching ratios of the
             decays B+ →(Formula presented)(1P)K+ and
             B+→J/ψK+π+π-, where (Formula presented) (1P)→J/ψγ
             and J/ψ→μ+μ- in pp collisions at (Formula presented)1.8
             TeV. Using a data sample from an integrated luminosity of
             110 pb-1 collected by the Collider Detector at Fermilab we
             measure the branching ratios to be BR(B+→(Formula
             presented) (1P)K+)=15.5±5.4(stat)±1.5(syst)±1.3(br)×10-4
             and BR(B+→J/ψK+π+π-)=6.9±1.8(stat)±1.1(syst)±0.4(br)×10-4
             where (br) is due to the finite precision on
             BR(B+→J/ψK+), BR(Formula presented)(1P)→J/ψγ) is used
             to normalize the signal yield, and (syst) encompasses all
             other systematic uncertainties.},
   Doi = {10.1103/PhysRevD.66.052005},
   Key = {fds332102}
}

@article{fds332103,
   Author = {al, DAE},
   Title = {Measurement of the ratio of b quark production cross
             sections in pp collisions at $\sqrt{s}=630$ GeV and
             $\sqrt{s} = 1800 GeV},
   Journal = {Physical Review},
   Volume = {66},
   Number = {D66},
   Pages = {032002},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.032002},
   Abstract = {We report a measurement of the ratio of the bottom quark
             production cross section in antiproton-proton collisions at
             [Formula Presented] to 1800 GeV using bottom quarks with
             transverse momenta greater than 10.75 GeV identified through
             their semileptonic decays and long lifetimes. The measured
             ratio [Formula Presented] is in good agreement with
             next-to-leading order quantum chromodynamics. © 2002 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.66.032002},
   Key = {fds332103}
}

@article{fds331216,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera,
             S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
             AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R},
   Title = {Comparison of the isolated direct photon cross sections in
             [Formula Presented] collisions at [Formula Presented] and
             [Formula Presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {11},
   Pages = {10},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.112003},
   Abstract = {We have measured the cross sections (Formula presented) for
             production of isolated direct photons in (Formula presented)
             collisions at two different center-of-mass energies, 1.8 TeV
             and 0.63 TeV, using the Collider Detector at Fermilab. The
             normalization of both data sets agrees with the predictions
             of quantum chromodynamics for a photon transverse momentum
             (Formula presented) of 25 GeV/c, but the shapes versus
             photon (Formula presented) do not. These shape differences
             lead to a significant disagreement in the ratio of cross
             sections in the scaling variable (Formula presented) This
             disagreement in the (Formula presented) ratio is difficult
             to explain with conventional theoretical uncertainties such
             as scale dependence and parton distribution
             parametrizations. © 2002 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.65.112003},
   Key = {fds331216}
}

@article{fds309634,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, M and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D},
   Title = {Search for new physics in photon-lepton events in [Formula
             Presented] collisions at [Formula Presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {66},
   Number = {1},
   Pages = {120041-1200427},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.012004},
   Abstract = {We present the results of a search in [Formula Presented]
             collisions at [Formula Presented] for anomalous production
             of events containing a photon with large transverse energy
             and a lepton [Formula Presented] or [Formula Presented] with
             large transverse energy, using [Formula Presented] of data
             collected with the Collider Detector at Fermilab during the
             1994–1995 collider run at the Fermilab Tevatron. The
             presence of large missing transverse energy [Formula
             Presented] additional photons, or additional leptons in
             these events is also analyzed. The results are consistent
             with standard model expectations, with the possible
             exception of photon-lepton events with large [Formula
             Presented] for which the observed total is 16 events and the
             expected mean total is [Formula Presented] events. © 2002
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.66.012004},
   Key = {fds309634}
}

@article{fds309636,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Amaral, P and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
             A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett,
             K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
             AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
             JY and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly,
             A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D},
   Title = {Search for single-top-quark production in [Formula
             Presented] collisions at [Formula Presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {9},
   Pages = {6},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.091102},
   Abstract = {We search for standard model single-top-quark production in
             the W-gluon fusion and (Formula presented) channels using
             (Formula presented) of data from (Formula presented)
             collisions at (Formula presented) collected with the
             Collider Detector at Fermilab. We set an upper limit at
             (Formula presented) confidence level (C.L.) on the combined
             W-gluon fusion and (Formula presented) single-top cross
             section of 14 pb, roughly six times larger than the standard
             model prediction. Separate (Formula presented) C.L. upper
             limits in the W-gluon fusion and (Formula presented)
             channels are also determined and are found to be 13 and 18
             pb, respectively. © 2002 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.65.091102},
   Key = {fds309636}
}

@article{fds309637,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Amaral, P and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl,
             A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett,
             K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
             AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
             JY and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly,
             A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D},
   Title = {Soft and hard interactions in [Formula Presented] collisions
             at [Formula Presented] and 630 GeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {7},
   Pages = {12},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.072005},
   Abstract = {We present a study of (Formula presented) collisions at
             (Formula presented) and 630 GeV collected using a minimum
             bias trigger by the CDF experiment in which the data set is
             divided into two classes corresponding to “soft” and
             “hard” interactions. For each subsample, the analysis
             includes measurements of the multiplicity, transverse
             momentum (Formula presented) spectrum, and the average
             (Formula presented) and event-by-event (Formula presented)
             dispersion as a function of multiplicity. A comparison of
             results shows distinct differences in the behavior of the
             two samples as a function of the center of mass (c.m.)
             energy. We find evidence that the properties of the soft
             sample are invariant as a function of c.m. energy. © 2002
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.65.072005},
   Key = {fds309637}
}

@article{fds309638,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera,
             S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan,
             AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R},
   Title = {Measurement of [Formula Presented]-meson lifetimes using
             fully reconstructed [Formula Presented] decays produced in
             [Formula Presented] collisions at [Formula
             Presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {9},
   Pages = {7},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.092009},
   Abstract = {We present an improved measurement of b-meson lifetimes
             using fully reconstructed B-decays produced in (Formula
             presented) collisions at (Formula presented) using (Formula
             presented) of data collected at the Collider Detector at
             Fermilab. We obtain (Formula presented) (Formula presented)
             and for the lifetime ratio (Formula presented). © 2002 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.65.092009},
   Key = {fds309638}
}

@article{fds309643,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
             R and Dagenhart, D and D’Auria, S and DeJongh, F},
   Title = {Charged jet evolution and the underlying event in
             proton-antiproton collisions at 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {9},
   Pages = {920021-9200222},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.092002},
   Abstract = {The growth and development of “charged particle jets”
             produced in proton-antiproton collisions at [Formula
             Presented] are studied over a transverse momentum range from
             [Formula Presented] [Formula Presented] to [Formula
             Presented] [Formula Presented] A variety of leading (highest
             transverse momentum) charged jet observables are compared
             with the QCD Monte Carlo models HERWIG, ISAJET, and PYTHIA.
             The models describe fairly well the multiplicity
             distribution of charged particles within the leading charged
             jet, the size of the leading charged jet, the radial
             distribution of charged particles and transverse momentum
             around the leading charged jet direction, and the momentum
             distribution of charged particles within the leading charged
             jet. The direction of the leading “charged particle jet”
             in each event is used to define three regions of [Formula
             Presented] space. The “toward” region contains the
             leading “charged particle jet”, while the “away”
             region, on the average, contains the away-side jet. The
             “transverse” region is perpendicular to the plane of the
             hard [Formula Presented]-to-[Formula Presented] scattering
             and is very sensitive to the “underlying event”
             component of the QCD Monte Carlo models. HERWIG, ISAJET, and
             PYTHIA with their default parameters do not describe
             correctly all the properties of the “transverse” region.
             © 2002 The American Physical Society.},
   Doi = {10.1103/PhysRevD.65.092002},
   Key = {fds309643}
}

@article{fds332100,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker, E and Bruner,
             N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, M and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, JY and Chung, W and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D and D’Auria, S},
   Title = {Search for radiative [Formula Presented]-hadron decays in
             [Formula Presented] collisions at [Formula
             Presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {66},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.66.112002},
   Abstract = {We have performed a search for radiative b-hadron decays
             using events produced in [Formula Presented] collisions at
             [Formula Presented] and collected by the Collider Detector
             at Fermilab. The decays we considered were [Formula
             Presented] [Formula Presented] [Formula Presented] and their
             charge conjugates. Two independent methods to identify
             photons from such decays were employed. In the first method,
             the photon was detected in the electromagnetic calorimeter.
             In the second method, the photon was identified by an
             electron-positron pair produced through the external photon
             conversion before the tracking detector volume. By combining
             the two methods we obtain upper limits on the branching
             fractions for the [Formula Presented] [Formula Presented]
             and [Formula Presented] radiative decays which, at the 95%
             confidence level, are found to be [Formula Presented]
             [Formula Presented] and [Formula Presented] © 2002 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.66.112002},
   Key = {fds332100}
}

@article{fds332104,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
             A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
             J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
             C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Colijn, AP and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson, R and Dagenhart, D},
   Title = {Search for the decay [Formula Presented] in [Formula
             Presented] collisions at [Formula Presented]
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2002},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.65.111101},
   Abstract = {We present a search for the flavor-changing neutral current
             decay [Formula Presented] in [Formula Presented] collisions
             at [Formula Presented] using [Formula Presented] of data
             collected at the Collider Detector at Fermilab (CDF). We
             find two candidate events for this decay, which are
             consistent with the background estimate of one event, and
             set an upper limit on the branching fraction of [Formula
             Presented] at a 95% confidence level. This is the first
             limit on the branching fraction of this decay. © 2002 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.65.111101},
   Key = {fds332104}
}

@article{fds309639,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
             J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
             S},
   Title = {Erratum: Measurement of the inclusive jet cross section in
             pp collisions at √s= 1.8 Tev (Physical Review D-
             Particles, Fields, Gravitation and Cosmology (2001) 64
             (032001)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {3},
   Pages = {399031},
   Year = {2002},
   Month = {February},
   Key = {fds309639}
}

@article{fds309640,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
             J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
             S},
   Title = {Erratum: Measurement of the two-jet differential cross
             section in pp collisions at √s=1800 GeV (Physical Review
             D- Particles, Fields, Gravitation and Cosmology (2001) 64
             (012001)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {65},
   Number = {3},
   Pages = {399021},
   Year = {2002},
   Month = {February},
   Key = {fds309640}
}

@article{fds309645,
   Author = {Alexopoulos, T and Anderson, EW and Bujak, AT and Carmony, DD and Erwin,
             AR and Gutay, LJ and Hirsch, AS and Nelson, KS and Porile, NT and Oh, SH and Scharenberg, RP and Srivastava, BK and Stringfellow, BC and Turkot,
             F and Warchol, J and Walker, WD},
   Title = {Evidence for hadronic deconfinement in p̄-p collisions at
             1.8 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {528},
   Number = {1-2},
   Pages = {43-48},
   Publisher = {Elsevier BV},
   Year = {2002},
   Month = {February},
   url = {http://dx.doi.org/10.1016/S0370-2693(02)01213-3},
   Abstract = {We have measured deconfined hadronic volumes, 4.4 < V < 13.0
             fm3, produced by a one-dimensional (1D) expansion. These
             volumes are directly proportional to the charged particle
             pseudorapidity densities 6.75 < dNc/dη < 20.2. The
             hadronization temperature is T = 179.5±5(syst) MeV. Using
             Bjorken's 1D model, the hadronization energy density is εF
             = 1.10±0.26(stat) GeV/fm3 corresponding to an excitation of
             24.8±6.2(stat) quark-gluon degrees of freedom. © 2002
             Elsevier Science B.V. All rights reserved.},
   Doi = {10.1016/S0370-2693(02)01213-3},
   Key = {fds309645}
}

@article{fds309644,
   Author = {Akesson, T and Baker, K and Bondarenko, V and Bytchkov, V and Carling,
             H and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Ebenstein, WL and Eerola, P and Egede, U and Farthouat, P and Froidevaux, D and Gavrilenko, I and Grichkevitch, Y and Hajduk, Z and Hanson, G and Ivochkin, VG and Jagielski, S and Keener, PT and Konovalov, S and Kekelidze, G and Kramarenko, VA and Laritchev, A and Lichard, P and Lundberg, B and Luehring, F and McFarlane, K and Muraviev, S and Nadtochy, A and Nevski, P and Newcomer, FM and Ogren, H and Oh, SH and Peshekhonov, V and Romaniouk, A and Rust, DR and Schegelsky,
             V and Semenov, S and Shmeleva, A and Smirnov, S and Smirnova, LN and Sosnovtsev, V and Spiridenkov, E and Stavrianakou, M and Thulesius,
             M and Tikhomirov, V and Van Berg and R and Wang, C and Williams,
             HH},
   Title = {Tracking performance of the transition radiation tracker
             prototype for the ATLAS experiment},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {485},
   Number = {3},
   Pages = {298-310},
   Publisher = {Elsevier BV},
   Year = {2002},
   Month = {June},
   url = {http://dx.doi.org/10.1016/S0168-9002(01)02030-7},
   Abstract = {A prototype of the Transition Radiation Tracker (TRT) for
             the ATLAS experiment at the CERN LHC has been built and
             tested at the CERN SPS. Detailed studies of the drift-time
             measurements, alignment technique, hit registration
             efficiency, track and momentum accuracy were performed. A
             coordinate measurement accuracy of 150 μm for a single TRT
             drift tube and momentum resolution of 0.8% for 20 GeV pions
             in a 1.56 T magnetic field were achieved. The results
             obtained are in agreement with the expected tracking
             performance of the ATLAS TRT. © 2001 Published by Elsevier
             Science B.V.},
   Doi = {10.1016/S0168-9002(01)02030-7},
   Key = {fds309644}
}

@article{fds309630,
   Author = {al, DAE},
   Title = {Limits on Extra Dimensions and New Particle Production in
             the Exclusive Photon and Missing Energy Signature in pp-bar
             Collisions at sqrt[s]=1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {89},
   Number = {28 Pt 1},
   Pages = {281801},
   Year = {2002},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.89.281801},
   Abstract = {The exclusive gamma E̸T signal has a small standard
             model cross section and is thus a channel sensitive to new
             physics. This signature is predicted by models with a
             superlight gravitino or with large extra spatial dimensions.
             We search for such signals at the Collider Detector at
             Fermilab, using 87 pb-1 of data at sqrt[s]=1.8 TeV, and
             extract 95% C.L. limits on these processes. A limit of
             221 GeV is set on the scale |F|1/2 in supersymmetric
             models. For 4, 6, and 8 extra dimensions, model- dependent
             limits on the fundamental mass scale MD of 0.55, 0.58, and
             0.60 TeV, respectively, are found. We also specify a
             "pseudo-model- independent" method of comparing the results
             to theoretical predictions.},
   Doi = {10.1103/physrevlett.89.281801},
   Key = {fds309630}
}

@article{fds309626,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker,
             E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers,
             W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D and D'Auria, S and Cecco, SD and Jongh, FD and dell'Agnello, S and dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo,
             T and Eddy, N and Einsweiler, K and Jr, EE and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fan, Q and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher,
             B and Flores-Castillo, LR and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Gresele, A and Grim, G and Grosso-Pilcher,
             C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Halkiadakis, E and Hall, C and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss, A and Hennecke,
             M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hollebeek,
             R and Holloway, L and Hou, S and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Issever, C and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iwai, J and Iwata, Y and Iyutin, B and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Kang,
             J and Unel, MK and Karr, K and Kartal, S and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, TH and Kim, YK and Kirby,
             M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kotelnikov, K and Kovacs,
             E and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kurino,
             K and Kuwabara, T and Kuznetsova, N and Laasanen, AT and Lai, N and Lami,
             S and Lammel, S and Lancaster, J and Lannon, K and Lancaster, M and Lander,
             R and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren,
             M and Liss, TM and Liu, JB and Liu, T and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, NS and Loginov, A and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak,
             R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Manca, G and Mariotti, M and Martignon, G and Martin, M and Martin, A and Martin, V and Martínez, M and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Miyazaki, Y and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Napora, R and Niell, F and Nelson,
             C and Nelson, T and Neu, C and Neubauer, MS and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Nigmanov, T and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Pescara, L and Phillips, TJ and Piacentino,
             G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Pukhov, O and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov, F and Ray, H and Reher, D and Reichold, A and Renton, P and Rescigno, M and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson,
             WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi,
             L and Sarkar, S and Sato, H and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
             A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
             AJ and Sliwa, K and Snider, FD and Snihur, R and Solodsky, A and Speer, T and Spezziga, M and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
             L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sukhanov, A and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, RJ and Teng, PK and Terashi,
             K and Tether, S and Thom, J and Thompson, AS and Thomson, E and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tonnesmann, M and Toyoda, H and Trischuk, W and Troconiz, JFD and Tseng, J and Tsybychev, D and Turini,
             N and Ukegawa, F and Unverhau, T and Vaiciulis, T and Valls, J and Varganov, A and Vataga, E and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D},
   Title = {Search for Lepton Flavor Violating Decays of a Heavy Neutral
             Particle in p p̄ Collisions at √s = 1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {91},
   Number = {17},
   Pages = {1716021-1716026},
   Year = {2003},
   url = {http://link.aps.org/doi/10.1103/PhysRevLett.91.171602},
   Abstract = {Lepton flavor violating decays of a heavy neutral particle
             in pp̄ collisions at √s = 1.8 TeV were studied. The
             position of PP̄ collisions along the beam line was measured
             in the vertex time projection chamber (VTX). The results
             show no evidence for new particles with lepton flavor
             violating decays. The limits on the cross section for
             production and decay of single sneutrino with R-parity
             violating interactions were also set.},
   Doi = {10.1103/physrevlett.91.171602},
   Key = {fds309626}
}

@article{fds309623,
   Author = {Collaboration, DAEACDF},
   Title = {Search for a W' Boson Decaying to a Top and Bottom Quark
             Pair in 1.8 TeV pp-bar Collisions},
   Journal = {Physical Review Letters},
   Volume = {90},
   Number = {8},
   Pages = {081802},
   Year = {2003},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.90.081802},
   Abstract = {We report the results of a search for a W' boson produced in
             pp -bar collisions at a center-of-mass energy of 1.8 TeV
             using a 106 pb-1 data sample recorded by the Collider
             Detector at Fermilab. We observe no significant excess of
             events above background for a W' boson decaying to a top and
             bottom quark pair. In a model where this boson would mediate
             interactions involving a massive right-handed neutrino ( nu
             R) and have standard model strength couplings, we use these
             data to exclude a W' boson with mass between 225 and 536
             GeV/c2 at 95% confidence level for MW' >> M nu R and between
             225 and 566 GeV/c2 at 95% confidence level for
             MW'},
   Doi = {10.1103/physrevlett.90.081802},
   Key = {fds309623}
}

@article{fds309622,
   Author = {Collaboration, DAEACDF},
   Title = {Search for Long-Lived Charged Massive Particles in pp-bar
             Collisions at sqrt[s]=1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {90},
   Number = {13},
   Pages = {131801},
   Year = {2003},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.90.131801},
   Abstract = {We report a search for the production of long-lived charged
             massive particles in a data sample of 90 pb-1 of sqrt[s]=1.8
             TeV pp-bar collisions recorded by the Collider Detector at
             Fermilab. The search uses the muonlike penetration and
             anomalously high ionization energy loss signature expected
             for such a particle to discriminate it from backgrounds. The
             data are found to agree with background expectations, and
             cross section limits of O(1) pb are derived using two
             reference models, a stable quark and a stable scalar
             lepton.},
   Doi = {10.1103/physrevlett.90.131801},
   Key = {fds309622}
}

@article{fds309624,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker,
             E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers,
             W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson,
             R},
   Title = {Search for associated production of Y and vector boson in
             pp̄ Collisions at √s = 1.8 TeV},
   Journal = {Physical Review Letters},
   Volume = {90},
   Number = {22},
   Pages = {2218031-2218037},
   Year = {2003},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.90.221803},
   Abstract = {Associated production of υ and vector boson in pp̄
             collisions at √s = 1.8 TeV were investigated. The CDF
             detector was used in the analysis. The analysis showed that
             υ(1S) mesons in association with W± or Z0 bosons were not
             observed by the CDF detector.},
   Doi = {10.1103/physrevlett.90.221803},
   Key = {fds309624}
}

@article{fds309625,
   Author = {Collaboration, DAEACDF},
   Title = {Search for the Supersymmetric Partner of the Top Quark in
             Dilepton Events from pp-bar Collisions at sqrt[s]=1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {90},
   Number = {25 I},
   Pages = {251801},
   Year = {2003},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.90.251801},
   Abstract = {We have searched for pair production of the supersymmetric
             partner of the top quark (stop) in 107 pb-1 of pp-bar
             collisions at sqrt[s]=1.8 TeV collected by the Collider
             Detector at Fermilab (CDF). Each stop is assumed to decay
             into a lepton, bottom quark, and supersymmetric neutrino.
             Such a scenario would give rise to events with two leptons,
             two hadronic jets, and a substantial imbalance of transverse
             energy. No evidence of such a stop signal has been found. We
             exclude stop masses in the region (80},
   Doi = {10.1103/physrevlett.90.251801},
   Key = {fds309625}
}

@article{fds309627,
   Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari,
             G and Arisawa, T and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bailey, MW and Bailey, S and de
             Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bevensee, B and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and van den Brink, S and Bromberg, C and Brozovic, M and Bruner, N and Buckley-Geer, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byon-Wagner,
             A and Byrum, KL and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Cassada, J and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman,
             J and Chen, C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
             L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cronin-Hennessy, D and Cropp, R and Culbertson, R and Dagenhart, D and D'Auria,
             S},
   Title = {Erratum: Measurement of the tt̄ production cross in pp̄
             collisions at √s= 1.8 Tev (Physical Review D (2001) 64
             (32002))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {67},
   Number = {11},
   Pages = {1199011-1199012},
   Year = {2003},
   Month = {June},
   Key = {fds309627}
}

@article{fds309621,
   Author = {Collaboration, DAEACDF},
   Title = {Central Pseudorapidity Gaps in Events with a Leading
             Antiproton at the Fermilab Tevatron p-barp
             Collider},
   Journal = {Physical Review Letters},
   Volume = {91},
   Number = {1},
   Pages = {011802},
   Year = {2003},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.91.011802},
   Abstract = {We report a measurement of the fraction of events with a
             large pseudorapidity gap Delta eta within the pseudorapidity
             region available to the proton dissociation products X in
             p-bar+p-->p-bar+X. For a final state p-bar of fractional
             momentum loss xi p-bar and 4-momentum transfer squared
             tp-bar within 0.063 is found to be 0.246±0.001
             (stat)±0.042 (syst) [0.184±0.001 (stat)±0.043 (syst)].
             Our results are compared with gap fractions measured in
             minimum bias p-barp collisions and with theoretical
             expectations.},
   Doi = {10.1103/physrevlett.91.011802},
   Key = {fds309621}
}

@article{fds332099,
   Author = {Collaboration, DAEACDF},
   Title = {Momentum distribution of charged particles in jets in dijet
             events in pp-bar collisions at sqrt[s]=1.8 TeV and
             comparisons to perturbative QCD predictions},
   Journal = {Physical Review},
   Volume = {D68},
   Number = {1},
   Pages = {012003},
   Publisher = {American Physical Society (APS)},
   Year = {2003},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.68.012003},
   Abstract = {Inclusive momentum distributions of charged particles in
             restricted cones around jet axes were measured in dijet
             events with invariant dijet masses in the range 80 to
             600 GeV/c2. Events were produced at the Fermilab Tevatron
             in pp-bar collisions with a center of mass energy of 1.8 TeV
             and recorded by the Collider Detector at Fermilab. The
             results were compared to perturbative QCD calculations
             carried out in the framework of the modified leading log
             approximation (MLLA) and assuming local parton-hadron
             duality. It was shown that the data follow theoretical
             predictions quite well over the whole range of the jet
             energies included in this analysis. We extracted the MLLA
             cutoff scale Qeff and found a value of 230±40 MeV. The
             theoretical prediction of Ejetsin  theta c scaling, where
             theta c is the cone opening angle, was experimentally
             observed for the first time. From the MLLA fits to the data,
             two more parameters were extracted: the ratio of parton
             multiplicities in gluon and quark jets, r=Ng-jetpartons/Nq-jetpartons=1.9±0.5,
             and the ratio of the number of charged hadrons to the number
             of predicted partons in a jet, KchargedLPHD=Nchargedhadrons/Npartons=0.56±0.10.},
   Doi = {10.1103/PhysRevD.68.012003},
   Key = {fds332099}
}

@article{fds309628,
   Author = {Akesson, T and Arik, E and Assamagan, K and Baker, K and Benjamin, D and Bertelsen, H and Bytchkov, V and Callahan, J and Capeans-Garrido, M and Catinaccio, A and Cetin, A and Cwetanski, P and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Ebenstein, WL and Eerola, P and Farthouat, P and Froidevaux, D and Grichkevitch, Y and Hajduk, Z and Hansen, JR and Keener, PK and Kekelidze, G and Konovalov,
             S and Kowalski, T and Kramarenko, VA and Kruger, K and Lundberg, B and Luehring, F and Manara, A and McFarlane, K and Mitsou, VA and Morozov,
             S and Muraviev, S and Nadtochy, A and Newcomer, FM and Olszowska, J and Ogren, H and Oh, SH and Peshekhonov, V and Price, M and Rembser, C and Romaniouk, A and Rust, DR and Schegelsky, V and Sapinski, M and Shmeleva, A and Smirnov, S and Smirnova, LN and Sosnovtsev, V and Soutchkov, S and Spiridenkov, E and Tikhomirov, V and VanBerg, R and Vassilakopoulos, V and Wang, C and Williams, HH},
   Title = {An X-ray scanner for wire chambers},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {507},
   Number = {3},
   Pages = {622-635},
   Publisher = {Elsevier BV},
   Year = {2003},
   Month = {July},
   url = {http://dx.doi.org/10.1016/S0168-9002(03)01389-5},
   Abstract = {A study was performed on an x-ray scanner for wire chambers.
             The techniques to measure the position of sense wires and
             field wires, the gas gain and the gas flow rate inside the
             wire chambers using a collimated and filtered x-ray beam
             were also reported. The gain measurement provided important
             information on the uniformity of the electric field
             configuration.},
   Doi = {10.1016/S0168-9002(03)01389-5},
   Key = {fds309628}
}

@article{fds332098,
   Author = {Collaboration, DAEACDF},
   Title = {Measurement of the mass difference m(D+s)-m(D+) at CDF
             II},
   Journal = {Physical Review},
   Volume = {D68},
   Number = {7},
   Pages = {072004},
   Publisher = {American Physical Society (APS)},
   Year = {2003},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.68.072004},
   Abstract = {We present a measurement of the mass difference
             m(D+s)-m(D+), where both the D+s and D+ are reconstructed in
             the phi pi + decay channel. This measurement uses 11.6 pb-1
             of data collected by CDF II using the new displaced-track
             trigger. The mass difference is found to bem(D+s)-
             m(D+)=99.41±0.38(stat)±0.21(syst) MeV/c2.},
   Doi = {10.1103/PhysRevD.68.072004},
   Key = {fds332098}
}

@article{fds309441,
   Author = {Collaboration, DAEACDF},
   Title = {Search for the flavor-changing neutral current decay
             D0-->µ+µ- in pp-bar collisions at sqrt[s]=1.96 TeV},
   Journal = {Physical Review},
   Volume = {D68},
   Number = {19},
   Pages = {091101},
   Year = {2003},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.101.192002},
   Abstract = {We report on a search for the flavor-changing neutral
             current decay D0-->µ+µ- in pp-bar collisions at
             sqrt[s]=1.96 TeV using 65 pb-1 of data collected by the
             CDF II experiment at the Fermilab Tevatron Collider. A
             displaced-track trigger selects long-lived D0 candidates in
             the D0-->µ+µ- search channel, the kinematically similar
             D0--> pi + pi - channel used for normalization, the
             Cabibbo-favored D0-->K- pi + channel used to optimize the
             selection criteria in an unbiased manner, and their charge
             conjugates. Finding no signal events in the D0-->µ+µ-
             search window, we set an upper limit on the branching
             fractionB(D0-- >µ+µ-)},
   Doi = {10.1103/physrevlett.101.192002},
   Key = {fds309441}
}

@article{fds309620,
   Author = {Collaboration, DAEACDFII},
   Title = {Measurement of Prompt Charm Meson Production Cross Sections
             in pp-bar Collisions at sqrt[s]=1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {91},
   Number = {24},
   Pages = {241804},
   Year = {2003},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.91.241804},
   Abstract = {We report on measurements of differential cross sections d
             sigma /dpT for prompt charm meson production in pp-bar
             collisions at sqrt[s]=1.96 TeV using 5.8±0.3 pb-1 of data
             from the CDF II detector at the Fermilab Tevatron. The data
             are collected with a new trigger that is sensitive to the
             long lifetime of hadrons containing heavy flavor. The charm
             meson cross sections are measured in the central rapidity
             region |y| K- pi +, D*+-->D0 pi +, D+-->K- pi + pi +, D+s-->
             phi pi +, and their charge conjugates. The measured cross
             sections are compared to theoretical calculations.},
   Doi = {10.1103/physrevlett.91.241804},
   Key = {fds309620}
}

@article{fds309629,
   Author = {Akesson, T and Barberio, E and Bondarenko, V and Capeans, M and Catinaccio, A and Cwetanski, P and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Ebenstein, WL and Eerola, P and Farthouat, P and Fedin, O and Froidevaux, D and Gavrilenko, I and Grichkevitch, Y and Gagnon, P and Hajduk, Z and Keener, PT and Kekelidze, G and Konovalov, S and Kowalski, T and Kramarenko, VA and Laritchev, A and Lichard, P and Lundberg, B and Luehring, F and Markina,
             I and Manara, A and Mcfarlane, K and Mitsou, V and Muraviev, S and Newcomer, FM and Ogren, H and Oh, SH and Olszowska, J and Peshekhonov,
             V and Rembser, C and Romaniouk, A and Rhone, O and Rust, DR and Schegelsky,
             V and Shmeleva, A and Smirnov, S and Smirnova, LN and Sosnovtsev, V and Sutchkov, S and Tartarelli, F and Tikhomirov, V and Van Berg and R and Vassilieva, L and Wang, C and Williams, HH},
   Title = {Aging studies for the ATLAS Transition Radiation Tracker
             (TRT)},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {515},
   Number = {1-2},
   Pages = {166-179},
   Publisher = {Elsevier BV},
   Year = {2003},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.nima.2003.08.145},
   Abstract = {A summary of the aging and material validation studies
             carried out for the ATLAS Transition Radiation Tracker (TRT)
             is presented. Particular emphasis is put on the different
             phenomena observed in straw tubes operating with the chosen
             Xe/CF4/CO2 mixture. The most serious effects observed are
             silicon deposition on the anode wire and damage of the anode
             wire gold plating. Etching phenomena and active radical
             effects are also discussed. With a careful choice of all
             materials and components, and with good control of the water
             contamination in the active gas, the ATLAS TRT will operate
             reliably for 10 years at the LHC design luminosity. To
             demonstrate this fully, more work is still needed on the gas
             system purification elements, in particular to understand
             their interplay with the active species containing fluorine
             created in the avalanche process under irradiation. © 2003
             Elsevier B.V. All rights reserved.},
   Doi = {10.1016/j.nima.2003.08.145},
   Key = {fds309629}
}

@article{fds309608,
   Author = {Acosta, D and Affolder, T and Ahn, MH and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro-Galtieri, A and Barker, G and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini,
             G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov,
             S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett,
             K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura,
             P and Campanelli, M and Campbell, M and Canepa, A and Carlsmith, D and Carron, S and Carosi, R and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
             C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chu, ML and Chung, JY and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, MN and Connolly, A and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and DaRonco, S and D'Auria, S and Barbaro, PD and Cecco,
             SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers,
             S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Doksus, P and Dominguez, A and Donati,
             S and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gaijar, A and Gallas, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, DW and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hall, C and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke,
             M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman,
             KD and Holloway, A and Hou, S and Houlden, MA and Huang, Y and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jones, M and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim,
             TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov,
             K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer,
             A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis,
             JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loken, J and Loreti,
             M and Loverre, P and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Meyer, A and Miao, T and Miladinovic,
             N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mishina, M and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Oishi, R and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari,
             F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
             H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi,
             F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni,
             A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
             A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shon, Y and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie, H and Stelzer, B and Stelzer-Chilton, O and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
             K},
   Title = {Observation of the narrow state X(3872) →
             J/ψπ+π- in p̄p collisions at √s
             = 1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {7},
   Pages = {072001-1-072001-6},
   Year = {2004},
   url = {http://dx.doi.org/10.1103/PhysRevLett.93.072001},
   Abstract = {The observation of a state consistent with X(3872) decaying
             into J/ψπ+π- was reported. The X(3872) mass was measured
             to be 3871.3±0.7(stat)±0.4(syst)MeV/c2 from a sample of
             730±90 candidates. The observed width was consistent with
             the detector resolution. The results were found to be
             converging well with the measurements by the Belle
             Collaboration using b± decays.},
   Doi = {10.1103/PhysRevLett.93.072001},
   Key = {fds309608}
}

@article{fds309619,
   Author = {Oh, SH and al, TAE},
   Title = {Design and construction of the TRT for the ATLAS experiment
             at the LHC},
   Journal = {Nucear Instrucments and methods},
   Publisher = {IEEE},
   Year = {2004},
   Key = {fds309619}
}

@article{fds30281,
   Author = {D. Acosta et al},
   Title = {Measurement of the tt-bar production Cross Section in ppbar
             at 1,96TeV Using Dilepton Events},
   Journal = {PRL, 93,142001},
   Year = {2004},
   Key = {fds30281}
}

@article{fds30283,
   Author = {D. Acosta et al},
   Title = {Double-Pomeron Exchange at the Fermilab Tevatron
             Collider},
   Journal = {PRL, 93, 142601},
   Year = {2004},
   Key = {fds30283}
}

@article{fds30285,
   Author = {D. Acosta et al},
   Title = {Underlying event in hard interactions at the fermilab
             tevatron collider},
   Journal = {PRD, D70,072002},
   Year = {2004},
   Key = {fds30285}
}

@article{fds30286,
   Author = {D. Acosta et al},
   Title = {Inclusive Search for Anomalous Production of High pt
             Like-Sign Lepton pairs in ppbar collisions at 1.8
             TeV},
   Journal = {PRL, 93, 061802},
   Year = {2004},
   Key = {fds30286}
}

@article{fds309607,
   Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
             V and Acharya, BS and Acosta, D and Adams, DL and Adams, M and Affolder, T and Ahmed, SN and Akimoto, H and Akopian, A and Albrow, MG and Alexeev, GD and Alton, A and Alves, GA and Amaral, P and Ambrose, D and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arnoud, Y and Arisawa, T and Artikov, A and Asakawa, T and Avila, C and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Babintsev, VV and Babukhadia, L and Bacchetta, N and Bachacou, H and Bacon, TC and Baden,
             A and Badgett, W and Baffioni, S and Bailey, MW and Bailey, S and Baldin,
             B and Balm, PW and Banerjee, S and Barbaro, P and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Baroiant,
             S and Barone, M and Barreto, J and Bartlett, JF and Bassler, U and Bauer,
             D and Bauer, G and Bean, A and Beaudette, F and Bedeschi, F and Behari, S and Begel, M and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Belyaev, A and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Beri, SB and Bernardi, G and Bertram, I and Berryhill, J and Besson, A and Beuselinck, R and Bevensee, B and Bezzubov, VA and Bhat,
             PC and Bhatnagar, V and Bhattacharjee, M and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blazey, G and Blekman, F and Blessing, S and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Boehnlein, A and Bojko,
             NI},
   Title = {Combination of CDF and D0 results on the [Formula Presented]
             boson mass and width},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {70},
   Number = {9},
   Pages = {092008-1-092008-17},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.70.092008},
   Abstract = {The results based on 1992–95 data (Run 1) from the CDF and
             D0 experiments on the measurements of the [Formula
             Presented] boson mass and width are presented, along with
             the combined results. We report a Tevatron collider average
             [Formula Presented]. We also report the Tevatron collider
             average of the directly measured [Formula Presented] boson
             width [Formula Presented]. We describe a new joint analysis
             of the direct [Formula Presented] mass and width
             measurements. Assuming the validity of the standard model,
             we combine the directly measured [Formula Presented] boson
             width with the width extracted from the ratio of [Formula
             Presented] and [Formula Presented] boson leptonic partial
             cross sections. This combined result for the Tevatron is
             [Formula Presented]. Finally, we use the measurements of the
             direct total [Formula Presented] width and the leptonic
             branching ratio to extract the leptonic partial width
             [Formula Presented]. © 2004 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.70.092008},
   Key = {fds309607}
}

@article{fds309611,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
             JY and Chung, W and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
             J and Culbertson, R and Dagenhart, D and D’Auria, S and Barbaro, P and Cecco, S and Dell’Agnello, S and Dell’Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, D and Derwent, PF and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D’Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
             S},
   Title = {Measurement of the polar-angle distribution of leptons from
             W boson decay as a function of the W transverse momentum in
             [Formula Presented] collisions at [Formula
             Presented]},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {70},
   Number = {3},
   Pages = {032004-1-032004-21},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.70.032004},
   Abstract = {We present a measurement of the polar-angle distribution of
             leptons from W boson decay, as a function of the W
             transverse momentum. The measurement uses an [Formula
             Presented] sample of [Formula Presented] collisions at
             [Formula Presented] collected by the CDF detector and
             includes data from both the [Formula Presented] and [Formula
             Presented] decay channels. We fit the W boson transverse
             mass distribution to a set of templates from a Monte Carlo
             event generator and detector simulation in several ranges of
             the W transverse momentum. The measurement agrees with the
             standard model expectation, whereby the ratio of
             longitudinally to transversely polarized W bosons, in the
             Collins-Soper W rest frame, increases with the W transverse
             momentum at a rate of approximately 15% per [Formula
             Presented]. © 2004 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.70.032004},
   Key = {fds309611}
}

@article{fds332097,
   Author = {Acosta, D and al, E},
   Title = {Measurement of the average time-integrated mixing
             probability of b-flavored hadrons produced at the
             Tevatron},
   Journal = {Phys. Rev.},
   Volume = {D69},
   Number = {1},
   Pages = {012002},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.69.012002},
   Abstract = {We have measured the number of like-sign (LS) and
             opposite-sign (OS) lepton pairs arising from double
             semileptonic decays of b and b-bar hadrons, pair produced at
             the Fermilab Tevatron collider. The data samples were
             collected with the Collider Detector at Fermilab during the
             1992Ð1995 collider run by triggering on the existence of
             µµ or eµ candidates in an event. The observed ratio of LS
             to OS dileptons leads to a measurement of the average
             time-integrated mixing probability of all produced
             b-flavored hadrons which decay weakly, chi
             -bar=0.152±0.007Ê(stat)±0.011Ê(syst), that is
             significantly larger than the world average chi
             -bar=0.118±0.005.},
   Doi = {10.1103/PhysRevD.69.012002},
   Key = {fds332097}
}

@article{fds309609,
   Author = {Acosta, D and Affolder, T and Akimoto, H and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and de Barbaro, P and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Bensinger, J and Beretvas, A and Berryhill, J and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bonushkin, Y and Bortoletto, D and Boudreau, J and Brandl, A and Bromberg, C and Brozovic, M and Brubaker,
             E and Bruner, N and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers,
             W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen, C and Chen, YC and Cheng, M-T and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek, L and Chu, ML and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Colijn, AP and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson,
             R and Dagenhart, D and D'Auria, S and De Cecco and S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo,
             T and Eddy, N and Einsweiler, K and Engels, E and Erbacher, R and Errede,
             D and Errede, S and Eusebi, R and Fan, Q and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher,
             B and Flores-Castillo, LR and Foster, GW and Franklin, M and Freeman, J and Friedman, J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Green, C and Gresele, A and Grim, G and Grosso-Pilcher,
             C and Guenther, M and Guillian, G and Guimaraes da Costa and J and Haas,
             RM and Haber, C and Hahn, SR and Halkiadakis, E and Hall, C and Handa, T and Handler, R and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich, J and Heiss,
             A and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hollebeek, R and Holloway, L and Hou, S and Huffman, BT and Hughes, R and Huston, J and Huth, J and Ikeda, H and Issever, C and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iwai, J and Iwata, Y and Iyutin,
             B and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko, T and Kang, J and Karagoz Unel and M and Karr, K and Kartal, S and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster,
             B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kotelnikov, K and Kovacs, E and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kurino, K and Kuwabara, T and Kuznetsova, N and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lannon, K and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Liu, JB and Liu, T and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, NS and Loginov, A and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Manca, G and Mariotti, M and Martignon, G and Martin, M and Martin, A and Martin, V and Martínez, M and Matthews, JAJ and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Miyazaki, Y and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Napora, R and Niell, F and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Neuberger, D and Newman-Holmes, C and Ngan, C-YP and Nigmanov, T and Niu, H and Nodulman,
             L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Pescara, L and Phillips, TJ and Piacentino,
             G and Piedra, J and Pitts, KT and Pompos, A and Pondrom, L and Pope, G and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Pukhov, O and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov, F and Ray, H and Reher, D and Reichold, A and Renton, P and Rescigno, M and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson,
             WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and St Denis and R and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi,
             L and Sarkar, S and Sato, H and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, A and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
             A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
             AJ and Sliwa, K and Snider, FD and Snihur, R and Solodsky, A and Spalding,
             J and Speer, T and Spezziga, M and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel, L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sukhanov, A and Sumorok,
             K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, RJ and Teng, PK and Terashi, K and Tether, S and Thom, J and Thompson, AS and Thomson, E and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tonnesmann,
             M and Toyoda, H and Trischuk, W and De Troconiz and JF and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Unverhau, T and Vaiciulis,
             T and Valls, J and Varganov, A and Vataga, E and Vejcik, S and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev,
             I},
   Title = {Search for pair production of scalar top quarks in R-parity
             violating decay modes in pp collisions at square root of
             s=1.8 TeV.},
   Journal = {Physical review letters},
   Volume = {92},
   Number = {5},
   Pages = {051803},
   Year = {2004},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.92.051803},
   Abstract = {We present the results of a search for pair production of
             scalar top quarks (t(1)) in an R-parity violating
             supersymmetry scenario in 106 pb(-1) of pp collisions at
             square root of s=1.8 TeV collected by the Collider Detector
             at Fermilab. In this mode each t(1) decays into a tau lepton
             and a b quark. We search for events with two tau's, one
             decaying leptonically (e or mu) and one decaying
             hadronically, and two jets. No candidate events pass our
             final selection criteria. We set a 95% confidence level
             lower limit on the t(1) mass at 122 GeV/c(2) for
             Br(t(1)-->tau b)=1.},
   Doi = {10.1103/physrevlett.92.051803},
   Key = {fds309609}
}

@article{fds309606,
   Author = {Collaboration, DAEACDFII},
   Title = {Search for Kaluza-Klein Graviton Emission in pp-bar
             Collisions at sqrt[s]=1.8 TeV Using the Missing Energy
             Signature},
   Journal = {Physical Review Letters},
   Volume = {92},
   Number = {12},
   Pages = {121802},
   Year = {2004},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.92.121802},
   Abstract = {We report on a search for direct Kaluza-Klein graviton
             production in a data sample of 84 pb-1 of pp-bar collisions
             at sqrt[s]=1.8 TeV, recorded by the Collider Detector at
             Fermilab. We investigate the final state of large missing
             transverse energy and one or two high energy jets. We
             compare the data with the predictions from a
             (3+1+n)-dimensional Kaluza-Klein scenario in which gravity
             becomes strong at the TeV scale. At 95% confidence level
             (C.L.) for n=2, 4, and 6 we exclude an effective Planck
             scale below 1.0, 0.77, and 0.71 TeV, respectively.},
   Doi = {10.1103/physrevlett.92.121802},
   Key = {fds309606}
}

@article{fds332096,
   Author = {al, DAE},
   Title = {Optimized search for single top quark production at the
             Fermilab Tevatron},
   Journal = {Phys. Rev.},
   Volume = {D69},
   Number = {5},
   Pages = {052003},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.69.052003},
   Abstract = {We use a neural-network technique to search for standard
             model single-top-quark production in the 106Êpb-1 dataset
             accumulated by the Collider Detector at Fermilab detector
             during the 1992Ð1995 collider run (``run I''). Using a
             sample of 64 W+1, 2, 3 jets events, we set a 95\% confidence
             level upper limit of 24 pb on the W-gluon and W* combined
             single-top cross section.},
   Doi = {10.1103/PhysRevD.69.052003},
   Key = {fds332096}
}

@article{fds309613,
   Author = {Acosta, D and al, E},
   Title = {Heavy flavor properties of jets produced in p anti-p
             interactions at s**(1/2) = 1.8-TeV},
   Journal = {Phys. Rev.},
   Volume = {D69},
   Number = {7},
   Pages = {072004},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.69.072004},
   Abstract = {We present a detailed examination of the heavy flavor
             properties of jets produced at the Fermilab Tevatron
             collider. The data set, collected with the Collider Detector
             at Fermilab, consists of events with two or more jets with
             transverse energy ET >= 15ÊGeV and pseudorapidity | eta | =
             2ÊGeV/c) in the data to that in the tuned simulation. We
             find that this rate is larger than what is expected for the
             conventional production and semileptonic decay of pairs of
             hadrons with heavy flavor.},
   Doi = {10.1103/PhysRevD.69.072004},
   Key = {fds309613}
}

@article{fds309615,
   Author = {Akesson, T and Anghinolfi, F and Arik, E and Baker, OK and Baron, S and Benjamin, D and Bertelsen, H and Bondarenko, V and Bytchkov, V and Callahan, J and Capeáns, M and Cardiel-Sas, L and Catinaccio, A and Cetin, SA and Cwetanski, P and Dam, M and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Driouichi, C and Ebenstein, WL and Eerola, P and Farthouat, P and Fedin, O and Froidevaux, D and Gagnon, P and Grichkevitch, Y and Grigalashvili, N and Hajduk, Z and Hansen, P and Kayumov, F and Keener, PT and Kekelidze, G and Khristatchev, A and Konovalov, S and Koudine, L and Kovalenko, S and Kowalski, T and Kramarenko, VA and Krüger, K and Laritchev, A and Lichard, P and Luehring, F and Lundberg, B and Maleev, V and Markina, I and McFarlane,
             KW and Mialkovski, V and Mindur, B and Mitsou, VA and Morozov, S and Munar,
             A and Muraviev, S and Nadtochy, A and Newcomer, FM and Ogren, H and Oh, SH and Oleshko, S and Olszowska, J and Passmore, S and Patritchev, S and Peshekhonov, V and Petti, R and Price, M and Rembser, C and Rohne, O and Romaniouk, A and Rust, DR and Ryabov, Y and Ryjov, V and Schegelsky, V and Seliverstov, D and Shin, T and Shmeleva, A and Smirnov, S and Sosnovtsev, V and Soutchkov, V and Spiridenkov, E and Szczygiel, R and Tikhomirov, V and Van Berg and R and Vassilakopoulos, VI and Vassilieva,
             L and Wang, C and Williams, HH and Zalite, A},
   Title = {Status of design and construction of the Transition
             Radiation Tracker (TRT) for the ATLAS experiment at the
             LHC},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {522},
   Number = {1-2},
   Pages = {131-145},
   Publisher = {Elsevier BV},
   Year = {2004},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.nima.2004.01.033},
   Abstract = {The ATLAS Inner Detector consists of three sub-systems, the
             Pixel Detector at the innermost radius, the Semi-Conductor
             Tracker at intermediate radii, and the Transition Radiation
             Tracker (TRT) at the outermost radius in front of the
             electromagnetic calorimeter. The TRT provides a combination
             of continuous tracking with many projective measurements
             based on individual drift-tubes (or straws) and of electron
             identification based on radiator fibres or foils interleaved
             between the straws themselves. This paper describes the
             current status of design and construction of the various
             components of the TRT: the assembly of the barrel modules
             has recently been completed, that of the end-cap wheels is
             well underway, and the on-detector front-end electronics is
             in production. The detector modules and front-end
             electronics boards will be integrated together over the next
             year, the barrel and end-cap TRT parts will be assembled and
             tested with their SCT counterparts during 2005 and
             installation and commissioning in the ATLAS pit will take
             place at the end of 2005 and the beginning of 2006. © 2004
             Elsevier B.V. All rights reserved.},
   Doi = {10.1016/j.nima.2004.01.033},
   Key = {fds309615}
}

@article{fds309616,
   Author = {Akesson, T and Arik, E and Baker, K and Baron, S and Benjamin, D and Bertelsen, H and Bondarenko, V and Bytchkov, V and Callahan, J and Capeans, M and Cardiel-Sas, L and Catinaccio, A and Cetin, SA and Cwetanski, P and Dam, M and Danielsson, H and Dittus, F and Dolgoshein,
             B and Dressnandt, N and Driouichi, C and Ebenstein, WL and Eerola, P and Farthouat, P and Fedin, O and Froidevaux, D and Gagnon, P and Grichkevitch, Y and Grigalashvili, N and Hajduk, Z and Hansen, P and Kayumov, F and Keener, PT and Kekelidze, G and Khristatchev, A and Konovalov, S and Koudine, L and Kovalenko, S and Kowalski, T and Kramarenko, VA and Kruger, K and Laritchev, A and Lichard, P and Luehring, F and Lundberg, B and Maleev, V and Markina, I and McFarlane,
             K and Mialkovski, V and Mitsou, VA and Mindur, B and Morozov, S and Munar,
             A and Muraviev, S and Nadtochy, A and Newcomer, FM and Ogren, H and Oh, SH and Oleshko, S and Olszowska, J and Passmore, S and Patritchev, S and Peshekhonov, V and Petti, R and Price, M and Rembser, C and Rohne, O and Romaniouk, A and Rust, DR and Ryabov, Y and Schegelsky, V and Seliverstov, D and Shin, T and Shmeleva, A and Smirnov, S and Sosnovtsev, V and Soutchkov, V and Spiridenkov, E and Tikhomirov, V and Van Berg and R and Vassilakopoulos, V and Vassilieva, L and Wang, C and Williams, HH and Zalite, A},
   Title = {ATLAS Transition Radiation Tracker test-beam
             results},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {522},
   Number = {1-2},
   Pages = {50-55},
   Publisher = {Elsevier BV},
   Year = {2004},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.nima.2004.01.017},
   Abstract = {Several prototypes of the Transition Radiation Tracker for
             the ATLAS experiment at the LHC have been built and tested
             at the CERN SPS accelerator. Results from detailed studies
             of the straw-tube hit registration efficiency and drift-time
             measurements and of the pion and electron spectra without
             and with radiators are presented. © 2004 Elsevier B.V. All
             rights reserved.},
   Doi = {10.1016/j.nima.2004.01.017},
   Key = {fds309616}
}

@article{fds309617,
   Author = {Akesson, T and Arik, E and Baker, K and Baron, S and Benjamin, D and Bertelsen, H and Bondarenko, V and Bytchkov, V and Callahan, J and Capeans, M and Cardiel-Sas, L and Catinaccio, A and Cetin, SA and Cwetanski, P and Dam, M and Danielsson, H and Dittus, F and Dolgoshein,
             B and Dressnandt, N and Driouichi, C and Ebenstein, WL and Eerola, P and Farthouat, P and Fedin, O and Froidevaux, D and Gagnon, P and Grichkevitch, Y and Grigalashvili, N and Hajduk, Z and Hansen, P and Kayumov, F and Keener, PT and Kekelidze, G and Khristatchev, A and Konovalov, S and Koudine, L and Kovalenko, S and Kowalski, T and Kramarenko, VA and Kruger, K and Laritchev, A and Lichard, P and Luehring, F and Lundberg, B and Maleev, V and McFarlane, K and Mialkovski, V and Mindur, B and Mitsou, VA and Morozov, S and Munar, A and Muraviev, S and Nadtochy, A and Newcomer, FM and Ogren, H and Oh, SH and Oleshko, S and Olszowska, J and Passmore, S and Patritchev, S and Peshekhonov, V and Petti, R and Price, M and Rembser, C and Rohne, O and Romaniouk, A and Rust, DR and Ryabov, Y and Schegelsky, V and Seliverstov, D and Shin, T and Shmeleva, A and Smirnov, S and Sosnovtsev, V and Soutchkov, V and Spiridenkov, E and Tikhomirov, V and Van Berg and R and Vassilakopoulos, V and Vassilieva, L and Wang, C and Williams, HH and Zalite, A},
   Title = {Operation of the ATLAS Transition Radiation Tracker under
             very high irradiation at the CERN LHC},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {522},
   Number = {1-2},
   Pages = {25-32},
   Publisher = {Elsevier BV},
   Year = {2004},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.nima.2004.01.013},
   Abstract = {The ATLAS Transition Radiation Tracker (TRT) performance
             depends critically on the choice of the active gas and on
             its properties. The most important operational aspects,
             which have led to the final choice of the active gas for the
             operation of the TRT at the LHC design luminosity, are
             presented. The TRT performance expected at these conditions
             is reviewed, including pile-up effects at high luminosity.
             © 2004 Elsevier B.V. All rights reserved.},
   Doi = {10.1016/j.nima.2004.01.013},
   Key = {fds309617}
}

@article{fds309618,
   Author = {Capeans, M and Åkesson, T and Anghinolfi, F and Arik, E and Baker, OK and Baron, S and Benjamin, D and Bertelsen, H and Bondarenko, V and Bytchkov, V and Callahan, J and Cardiel-Sas, L and Catinaccio, A and Cetin, S and Cwetanski, P and Dam, M and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Driouichi, C and Ebenstein, WL and Eerola, P and Farthouat, P and Fedin, O and Froidevaux, D and Gagnon, P and Grichkevitch, Y and Grigalashvili, N and Hajduk, Z and Hansen, P and Kayumov, F and Keener, PT and Kekelidze, G and Khristatchev, A and Konovalov, S and Koudine, L and Kovalenko, S and Kowalski, T and Kramarenko, VA and Krüger, K and Laritchev, A and Lichard, P and Luehring, F and Lundberg, B and Maleev, V and Markina, I and McFarlane,
             KW and Mialkovski, V and Mindur, B and Mitsou, VA and Morozov, S and Munar,
             A and Muraviev, S and Nadtochy, A and Newcomer, FM and Ogren, H and Oh, SH and Olszowska, J and Passmore, S and Patritchev, S and Peshekhonov, V and Petti, R and Price, M and Rembser, C and Røhne, O and Romaniouk, A and Rust, DR and Ryabov, Y and Ryjov, V and Schegelsky, V and Seliverstov,
             D and Shin, T and Shmeleva, A and Smirnov, S and Sosnovtsev, V and Soutchkov, V and Spiridenkov, E and Szczygiel, R and Tikhomirov, V and Van Berg and R and Vassilakopoulos, VI and Vassilieva, L and Wang, C and Williams, HH and Zalite, A},
   Title = {Recent aging studies for the ATLAS transition radiation
             tracker},
   Journal = {IEEE Transactions on Nuclear Science},
   Volume = {51},
   Number = {3 III},
   Pages = {960-967},
   Publisher = {Institute of Electrical and Electronics Engineers
             (IEEE)},
   Year = {2004},
   Month = {June},
   url = {http://dx.doi.org/10.1109/TNS.2004.829496},
   Abstract = {The transition radiation tracker (TRT) is one of the three
             subsystems of the inner detector of the ATLAS experiment. It
             is designed to operate for 10 yr at the LHC, with integrated
             charges of ∼ 10 C/cm of wire and radiation doses of about
             10 Mrad and 2 × 1014 neutrons/cm2. These doses translate
             into unprecedented ionization currents and integrated
             charges for a large-scale gaseous detector. This paper
             describes studies leading to the adoption of a new
             ionization gas regime for the ATLAS TRT. In this new regime,
             the primary gas mixture is 70%Xe-27%CO2-3%O2. It is planned
             to occasionally flush and operate the TRT detector with an
             Ar-based ternary mixture, containing a small percentage of
             CF4, to remove, if needed, silicon pollution from the anode
             wires. This procedure has been validated in realistic
             conditions and would require a few days of dedicated
             operation. This paper covers both performance and aging
             studies with the new TRT gas mixture.},
   Doi = {10.1109/TNS.2004.829496},
   Key = {fds309618}
}

@article{fds309590,
   Author = {al, DAE},
   Title = {Search for B0s-->µ+µ- and B0d-->µ+µ- Decays in pp-bar
             Collisions at sqrt[s]=1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {5},
   Pages = {032001},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.051104},
   Abstract = {We report on a search for B0s-->µ+µ- and B0d-->µ+µ-
             decays in pp-bar collisions at sqrt[s]=1.96 TeV using 171
             pb-1 of data collected by the CDF II experiment at the
             Fermilab Tevatron Collider. The decay rates of these rare
             processes are sensitive to contributions from physics beyond
             the standard model. One event survives all our selection
             requirements, consistent with the background expectation. We
             derive branching ratio limits of B(B0s--
             >µ+µ-)µ+µ-)},
   Doi = {10.1103/PhysRevD.72.051104},
   Key = {fds309590}
}

@article{fds309614,
   Author = {Acousta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat,
             C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de
             Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Dininno, M and De Pedis,
             D and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Doksus,
             P and Dominguez, A and Donati, S and Donega, M and D'Onnofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan,
             G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester,
             S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Gondcharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra,
             Y and Goulianos, K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Guimaraes da Costa and J and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
             D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Kongisberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin,
             CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martiínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Okusawa,
             T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, KT and Plager, C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
             S and Ratnikov, F and Ray, H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
             WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Sfiligoi, I and Shears,
             T and Scribano, A and Scuri, F and Sefov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Shapiro, MD and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie,
             H},
   Title = {Search for B0s-->micro+micro- and B0d-->micro+micro- decays
             in pp collisions at square root s = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {93},
   Number = {3},
   Pages = {032001},
   Year = {2004},
   Month = {July},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.93.032001},
   Abstract = {We report on a search for B(0)(s)-->micro(+)micro(-) and
             B(0)(d)-->micro(+)micro(-) decays in pp collisions at square
             root of s=1.96 TeV using 171 pb(-1) of data collected by the
             CDF II experiment at the Fermilab Tevatron Collider. The
             decay rates of these rare processes are sensitive to
             contributions from physics beyond the standard model. One
             event survives all our selection requirements, consistent
             with the background expectation. We derive branching ratio
             limits of B(B(0)(s)-->micro(+)micro(-))<5.8x10(-7) and
             B(B(0)(d)-->micro(+)micro(-))<1.5x10(-7) at 90% confidence
             level.},
   Doi = {10.1103/physrevlett.93.032001},
   Key = {fds309614}
}

@article{fds309605,
   Author = {al, DAE},
   Title = {Inclusive Search for Anomalous Production of High-pT
             Like-Sign Lepton Pairs in pp-bar Collisions at sqrt[s]=1.8
             TeV},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {6},
   Pages = {061802},
   Year = {2004},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.93.061802},
   Abstract = {We report on a search for anomalous production of events
             with at least two charged, isolated, like-sign leptons, each
             with pT>11 GeV/c using a 107 pb-1 sample of 1.8 TeV pp-bar
             collisions collected by the CDF detector. We define a signal
             region containing low background from standard model
             processes. To avoid bias, we fix the final cuts before
             examining the event yield in the signal region using control
             regions to test the Monte Carlo predictions. We observe no
             events in the signal region, consistent with an expectation
             of 0.63+0.84-0.07 events. We present 95% confidence level
             limits on new physics processes in both a signature-based
             context as well as within a representative minimal
             supergravity (tan( beta =3) model.},
   Doi = {10.1103/physrevlett.93.061802},
   Key = {fds309605}
}

@article{fds309604,
   Author = {al, DAE},
   Title = {Inclusive Double-Pomeron Exchange at the Fermilab Tevatron
             p-barp Collide},
   Journal = {Physical Review Letters},
   Volume = {93},
   Number = {14},
   Pages = {141601},
   Year = {2004},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.93.141601},
   Abstract = {We report results from a study of events with a double-
             Pomeron exchange topology produced in p-barp collisions at
             sqrt[s]=1800 GeV. The events are characterized by a leading
             antiproton and a large rapidity gap on the outgoing proton
             side. We find that the differential production cross section
             agrees in shape with predictions based on Regge theory and
             factorization, and that the ratio of double-Pomeron exchange
             to single diffractive production rates is relatively
             unsuppressed as compared to the O(10) suppression factor
             previously measured in single diffractive
             production.},
   Doi = {10.1103/physrevlett.93.141601},
   Key = {fds309604}
}

@article{fds309610,
   Author = {al, DAE},
   Title = {Direct photon cross section with conversions at
             CDF},
   Journal = {Physical Review},
   Volume = {D70},
   Number = {7},
   Pages = {074008},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.70.074008},
   Abstract = {0.9 using data collected between 1994 and 1995 by the
             Collider Detector at Fermilab (CDF). The measurement is
             based on events where the photon converts into an
             electron-positron pair in the material of the inner
             detector, resulting in a two track event signature. To
             remove pi 0--> gamma gamma and eta --> gamma gamma events
             from the data we use a new background subtraction technique
             which takes advantage of the tracking information available
             in a photon conversion event. We find that the shape of the
             cross section as a function of photon pT is poorly described
             by next-to- leading-order QCD predictions, but agrees with
             previous CDF measurements.},
   Doi = {10.1103/PhysRevD.70.074008},
   Key = {fds309610}
}

@article{fds309612,
   Author = {al, DAE},
   Title = {The Underlying event in hard interactions at the Fermilab
             Tevatron p-barp collider},
   Journal = {Physical Review},
   Volume = {D70},
   Number = {7},
   Pages = {072002},
   Publisher = {American Physical Society (APS)},
   Year = {2004},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.70.072002},
   Abstract = {For comparison of inclusive jet cross sections measured at
             hadron-hadron colliders to next-to-leading order (NLO)
             parton-level calculations, the energy deposited in the jet
             cone by spectator parton interactions must first be
             subtracted. The assumption made at the Tevatron is that the
             spectator parton interaction energy is similar to the
             ambient level measured in minimum bias events. In this
             paper, we test this assumption by measuring the ambient
             charged track momentum in events containing large transverse
             energy jets at sqrt[s]=1800 GeV and sqrt[s]=630 GeV and
             comparing this ambient momentum with that observed both in
             minimum bias events and with that predicted by two Monte
             Carlo models. Two cones in eta - phi space are defined, at
             the same pseudorapidity, eta , as the jet with the highest
             transverse energy (E(1)T), and at ±90o in the azimuthal
             direction, phi . The total charged track momentum inside
             each of the two cones is measured. The minimum momentum in
             the two cones is almost independent of E(1)T and is similar
             to the momentum observed in minimum bias events, whereas the
             maximum momentum increases roughly linearly with the jet
             E(1)T over most of the measured range. This study was
             carried out using data from the CDF detector taken during
             Run 1 (1994-1995). The study will help improve the precision
             of comparisons of jet cross section data and NLO
             perturbative QCD predictions. The distribution of the sum of
             the track momenta in the two cones is also examined for five
             different E(1)T bins. The HERWIG and PYTHIA Monte Carlo
             generators are reasonably successful in describing the data,
             but neither can describe completely all of the event
             properties.},
   Doi = {10.1103/PhysRevD.70.072002},
   Key = {fds309612}
}

@article{fds340924,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             L and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and DrollingerV, and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, V and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
             F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and HaywardH, and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and HoffmanK, D and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
             D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
             N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
             R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
             D},
   Title = {Measurement of the J/ψ meson and b-hadron production cross
             sections in pp̄ collisions at √s = 1960
             GeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {3},
   Pages = {032001-1-032001-26},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.032001},
   Abstract = {We present a new measurement of the inclusive and
             differential production cross sections of J/ψ mesons and b
             hadrons in proton-antiproton collisions at √s = 1960 GeV.
             The data correspond to an integrated luminosity of 39.7 pb-1
             collected by the CDF run II detector. We find the integrated
             cross section for inclusive J/ψ production for all
             transverse momenta from 0 to 20 GeV/c in the rapidity range
             |y| &lt; 0.6 to be 4.08 ± 0.02(Stat)-0.33+0.36(syst) μb.
             We separate the fraction of J/ψ events from the decay of
             the long-lived b hadrons using the lifetime distribution in
             all events with pT(J/ψ) &gt; 1.25 GeV/c. We find the total
             cross section for b hadrons, including both hadrons and
             antihadrons, decaying to J/ψ with transverse momenta
             greater than 1.25 GeV/c in the rapidity range |y(J/ψ)| &lt;
             0.6 is 0.330 ± 0.005(stat) -0.033+0.036(syst) μb. Using a
             Monte Carlo simulation of the decay kinematics of b hadrons
             to all final states containing a J/ψ, we extract the first
             measurement of the total single b-hadron cross section down
             to zero transverse momentum at √s = 1960 GeV. We find the
             total single b-hadron cross section integrated over all
             transverse momenta for b hadrons in the rapidity range |y|
             &lt; 0.6 to be 17.6 ± 0.4(stat) -2.3+2.5(syst) μb. © 2005
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.032001},
   Key = {fds340924}
}

@article{fds313363,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
             F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
             D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
             N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
             R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy,
             L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard,
             PF},
   Title = {Measurement of the forward-backward charge asymmetry from
             W→ev production in pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {5},
   Pages = {1-9},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://link.aps.org/abstract/PRD/v71/e051104},
   Abstract = {We report a measurement of the forward-backward charge
             asymmetry of electrons from W boson decays in pp̄
             collisions at √s=1.96 TeV using a data sample of 170 pb-1
             collected by the Collider Detector at Fermilab. The
             asymmetry is measured as a function of electron rapidity and
             transverse energy and provides new input on the momentum
             fraction dependence of the u and d quark parton distribution
             functions within the proton. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.71.051104},
   Key = {fds313363}
}

@article{fds317045,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
             J and Culbertson, R and Dagenhart, D and D'Auria, S and Barbaro, PD and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
             C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Flores-Castillo, LR and Foster, GW and Franklin, M and Friedman, J and Furic, I and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, SR and Halkiadakis, E and Handler, R and Happacher,
             F and Hara, K and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
             J and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hou, S and Huffman, BT and Hughes, R and Huston, J and Issever, C and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jones, M and Kamon, T and Kang, J and Unel, MK and Kartal, S and Kasha, H and Kato, Y and Kennedy, RD and Kephart, R and Kilminster, B and Kim, DH and Kim, HS and Kim, MJ and Kim,
             SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lami, S and Lammel, S and Lancaster,
             J and Lannon, K and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Liu, T and Litvintsev, DO and Lockyer, NS and Loginov, A and Loreti, M and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Mangano, M and Manca, G and Mariotti, M and Martin, M and Martin, A and Martin, V and Martínez, M and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer,
             A and Miao, T and Miller, R and Miller, JS and Miscetti, S and Mitselmakher, G and Moggi, N and Moore, R and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napora, R and Niell, F and Nelson, C and Nelson,
             T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nigmanov, T and Nodulman, L and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompo, A and Pondrom, L and Pope, G and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Poukhov, O and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov,
             F and Ray, H and Reichold, A and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez,
             C and Sansoni, A and Santi, L and Sarkar, S and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Sill, A and Sinervo, P and Slaughter, AJ and Sliwa, K and Snider, FD and Snihur, R and Spezziga, M and Spinella, F and Spiropulu, M and Spiegel, L and Stefanini, A and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
             K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Tecchio,
             M and Tesarek, RJ and Teng, PK and Terashi, K and Tether, S and Thom, J and Thompson, AS and Thomson, E and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tönnesmann, M and Toyoda, H and Trischuk, W and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Unverhau, T and Vaiciulis, T and Varganov, A and Vataga, E and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Wagner, RG and Wagner, RL and Wagner, W and Wan, Z and Wang, C and Wang, MJ and Wang, SM and Ward, B and Waschke, S and Waters, D and Watts, T and Weber, M and III, WCW and Whitehouse, B and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
             BL and Wolbers, S and Wolter, M and Worm, S and Wu, X and Würthwein, F and Yang, UK and Yao, W and Yeh, GP and Yi, K and Yoh, J and Yoshida, T and Yu, I and Yu, S and Yun, JC and Zanello, L and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Measurements of bottom-antibottom azimuthal production
             correlations in proton-antiproton collisions at
             s=1.8TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {9},
   Pages = {1-39},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://link.aps.org/abstract/PRD/v71/e092001},
   Abstract = {We have measured the azimuthal angular correlation of bb̄
             production, using 86.5pb-1 of data collected by Collider
             Detector at Fermilab (CDF) in pp̄ collisions at s=1.8TeV
             during 1994-1995. In high-energy pp̄ collisions, such as at
             the Tevatron, bb̄ production can be schematically
             categorized into three mechanisms. The leading-order (LO)
             process is "flavor creation," where both b and b̄ quarks
             substantially participate in the hard scattering and result
             in a distinct back-to-back signal in final state. The
             "flavor excitation" and the "gluon splitting" processes,
             which appear at next-leading-order (NLO), are known to make
             a comparable contribution to total bb̄ cross section, while
             providing very different opening angle distributions from
             the LO process. An azimuthal opening angle between bottom
             and antibottom, Δ, has been used for the correlation
             measurement to probe the interaction creating bb̄ pairs.
             The Δ distribution has been obtained from two different
             methods. One method measures the Δ between bottom hadrons
             using events with two reconstructed secondary vertex tags.
             The other method uses bb̄→(J/ ψX)(X′) events, where
             the charged lepton () is an electron (e) or a muon (μ), to
             measure Δ between bottom quarks. The bb̄ purity is
             determined as a function of Δ by fitting the decay length
             of the J/ψ and the impact parameter of the. Both methods
             quantify the contribution from higher-order production
             mechanisms by the fraction of the bb̄ pairs produced in the
             same azimuthal hemisphere, ftoward. The measured ftoward
             values are consistent with both parton shower Monte Carlo
             and NLO QCD predictions. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.71.092001},
   Key = {fds317045}
}

@article{fds309553,
   Author = {Acosta, and D, and others},
   Title = {Search for first-generation scalar leptoquarks in pp-bar
             collisions at sqrt[s]=1.96 TeV},
   Journal = {Phys. Rev.},
   Volume = {D72},
   Number = {5},
   Pages = {051107},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.051102},
   Abstract = {Results on a search for pair production of second-generation
             scalar leptoquark in pp̄ collisions at s=1.96TeV are
             reported. The data analyzed were collected by the CDF
             detector during the 2002-2003 Tevatron Run II and correspond
             to an integrated luminosity of 198pb-1. Leptoquarks (LQ) are
             sought through their decay into (charged) leptons and
             quarks, with final state signatures represented by two muons
             and jets and one muon, large transverse missing energy and
             jets. We observe no evidence for LQ production and derive
             95% C.L. upper limits on the LQ production cross sections as
             well as lower limits on their mass as a function of β,
             where β is the branching fraction for LQ→μq. © 2006 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.73.051102},
   Key = {fds309553}
}

@article{fds313450,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
             F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer,
             S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao,
             T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel,
             R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
             T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman,
             MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert,
             B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
             K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu,
             V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri,
             F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF},
   Title = {Measurement of the moments of the hadronic invariant mass
             distribution in semileptonic B decays},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {5},
   Pages = {1-9},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://link.aps.org/abstract/PRL/v95/e031801},
   Abstract = {Using 180 pb -1 of data collected with the CDF II detector
             at the Tevatron, we measure the first two moments of the
             hadronic invariant mass-squared distribution in charmed
             semileptonic B decays. From these we determine the
             nonperturbative Heavy Quark Effective Theory parameters Λ
             and λ 1 used to relate the B meson semileptonic branching
             ratio to the CKM matrix element |V cb|. For a minimum lepton
             momentum of 0.7 GeV/c in the B rest frame we measure the
             first two moments of the D** → D (*)π component to be
             〈m D**2〉 = (5.83 ± 0.16 stat ± 0.08 syst) GeV 2/c 4
             and 〈(m D**2 - 〈m D**2〉) 2〉 = (1.30 ± 0.69 stat ±
             0.22 syst) GeV 4/c 8. Combining these with the discrete mass
             terms from the D and D* mesons, we find the total moments to
             be 〈M Ξc2〉 - m̄ D2 = (0.467 ± 0.038 stat ± 0.068
             syst GeV 2/c 4 and 〈(M Ξc2 - 〈M Ξc2〉) 2〉 = (1.05
             ± 0.26 stat ± 0.13 syst) GeV 4/c 8, where m̄ D is the
             spin-averaged D mass. The systematic error is dominated by
             the uncertainties in the world-average branching ratios used
             to combine the D, D*, and D** contributions. The analysis
             makes no assumptions about the shape or resonant structure
             of the D** → D (*)π invariant mass distribution. © 2005
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.051103},
   Key = {fds313450}
}

@article{fds309558,
   Author = {Acosta, and D, and others},
   Title = {Measurement of the t anti-t production cross section in p
             anti-p collisions at sqrt[s]=1.96 TeV using lepton + jets
             events with secondary vertex b-tagging},
   Journal = {Phys. Rev.},
   Volume = {D71},
   Number = {7},
   Pages = {052003},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.072006},
   Abstract = {http://arxiv.org/abs/hep-ex/0410041},
   Doi = {10.1103/PhysRevD.74.072006},
   Key = {fds309558}
}

@article{fds358018,
   Author = {Acosta, and D, and others},
   Title = {Study of jet shapes in inclusive jet production in p anti-p
             collisions at s**(1/2) = 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D71},
   Pages = {112002},
   Year = {2005},
   Abstract = {http://arxiv.org/abs/hep-ex/0505013},
   Key = {fds358018}
}

@article{fds309571,
   Author = {Acosta, and D, and others},
   Title = {Measurement of the cross section for prompt diphoton
             production in p anti-p collisions at sqrt[s]=1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {95},
   Number = {2},
   Pages = {022003},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.95.022003},
   Abstract = {http://arxiv.org/abs/hep-ex/0412050},
   Doi = {10.1103/physrevlett.95.022003},
   Key = {fds309571}
}

@article{fds309574,
   Author = {Acosta, and D, and others},
   Title = {First measurements of inclusive W and Z cross sections from
             Run II of the Tevatron collider},
   Journal = {Phys. Rev. Lett.},
   Volume = {94},
   Number = {9},
   Pages = {091803},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/physrevlett.94.091803},
   Abstract = {http://arxiv.org/abs/hep-ex/0406078},
   Doi = {10.1103/physrevlett.94.091803},
   Key = {fds309574}
}

@article{fds309582,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
             P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr,
             RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays,
             C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
             D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato,
             Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
             T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons,
             L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
             JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine,
             A and Rappoccio, S and Ratnikov, F and Ray, H and Reichold, A and Reisert,
             B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
             K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
             S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz,
             A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan,
             A},
   Title = {Search for electroweak single-top-quark production in pp̄
             collisions at √s = 1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {1},
   Pages = {012005-1-012005-7},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.012005},
   Abstract = {We report on a search for standard model t-channel and
             s-channel single-top quark production in pp̄ collisions at
             a center of mass energy of 1.96 TeV. We use a data sample
             corresponding to 162 pb-1 recorded by the upgraded collider
             detector at Fermilab. We find no significant evidence for
             electroweak top quark production and set upper limits at the
             95% confidence level on the production cross section,
             consistent with the standard model: 10.1 pb for the
             t-channel, 13.6 pb for the s-channel and 17.8 pb for the
             combined cross section of t- and s-channel. © 2005 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.71.012005},
   Key = {fds309582}
}

@article{fds309585,
   Author = {Acosta, and D, and others},
   Title = {Search for anomalous production of diphoton events with
             missing transverse energy at CDF and limits on gauge-
             mediated supersymmetry-breaking models},
   Journal = {Phys. Rev.},
   Volume = {D71},
   Number = {3},
   Pages = {031104},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.031104},
   Abstract = {http://arxiv.org/abs/hep-ex/0410053},
   Doi = {10.1103/PhysRevD.71.031104},
   Key = {fds309585}
}

@article{fds309589,
   Author = {Acosta, and D, and others},
   Title = {Measurement of the cross section for t anti-t production in
             p anti-p collisions using the kinematics of lepton + jets
             events},
   Journal = {Phys. Rev.},
   Volume = {D72},
   Number = {5},
   Pages = {052003},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.052003},
   Abstract = {http://arxiv.org/abs/hep-ex/0504053},
   Doi = {10.1103/PhysRevD.72.052003},
   Key = {fds309589}
}

@article{fds309592,
   Author = {Acosta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
             A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
             P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
             D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
             KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
             PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
             BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
             T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic,
             P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin,
             A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
             T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patricck, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
             S and Ratnikov, F and Ray, H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna,
             G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
             S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smirnov, D and Smith, JR and Snider,
             FD},
   Title = {Measurement of partial widths and search for direct CP
             violation in D 0 meson decays to
             K-K+ and π -π+},
   Journal = {Physical Review Letters},
   Volume = {94},
   Number = {12},
   Pages = {122001},
   Year = {2005},
   url = {http://link.aps.org/abstract/PRL/v94/e122001},
   Abstract = {We present a measurement of relative partial widths and
             decay rate CP asymmetries in K- K+ and π-π+ decays of D0
             mesons produced in pp̄ collisions at,√s = 1.96 TeV. We
             use a sample of 2 × 105 D*+ →D0π+ (and charge conjugate)
             decays with the D0 decaying to K-π+, K-K +, and π-π+,
             corresponding to 123 pb -1 of data collected by the Collider
             Detector at Fermilab II experiment at the Fermilab Tevatron
             collider. No significant direct CP violation is observed. We
             measure γ(D0→ K- K +)/γ(D0-→K-π+) = 0.0992 ±0.0992
             ±0.0012, γ(D0→K -π+)/γ(D0→K -π+) = 0.03594 ±
             0.00054 ±0.00040, A CP(K- K+) = (2.0 ±1.2 ±0.6)%, and
             ACP(π-π+) = (1.0 ±1.3 ±0.6)%, where, in all cases, the
             first uncertainty is statistical and the second is
             systematic. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.94.122001},
   Key = {fds309592}
}

@article{fds313357,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canelli, F and Canepa, A and Casarsa, M and Carlsmith, D and Carosi,
             R and Carron, S and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Cruz, A and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers,
             S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Dituro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, RD and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii,
             Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
             DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
             N and Miles, J and Miller, L and Miller, R and Miller, JS and Mills, C and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi,
             N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Muelmenstaedt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Nelson, T and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Ohsugi,
             T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Osterberg,
             K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
             V and Paramonov, AA and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo,
             T and Rolli, S and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis,
             RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sill, A and Sinervo, P and Sisakyan, A and Sjolin, J and Skiba, A and Slaughter, AJ and Sliwa,
             K},
   Title = {Measurement of the tt̄ production cross section in pp̄
             collisions at s=1.96 TeV using lepton plus jets events with
             semileptonic B decays to muons},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {72},
   Number = {3},
   Pages = {1-20},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://link.aps.org/abstract/PRD/v72/e032002},
   Abstract = {We present a measurement of the tt̄ production cross
             section using 194 pb-1 of CDF II data using events with a
             high transverse momentum electron or muon, three or more
             jets, and missing transverse energy. The measurement assumes
             100% t→Wb branching fraction. Events consistent with tt̄
             decay are found by identifying jets containing heavy-flavor
             semileptonic decays to muons. The dominant backgrounds are
             evaluated directly from the data. Based on 20 candidate
             events and an expected background of 9.5±1.1 events, we
             measure a production cross section of 5.3±3.3-1.0+1.3 pb,
             in agreement with the standard model. © 2005 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.72.032002},
   Key = {fds313357}
}

@article{fds311282,
   Author = {al, DAE},
   Title = {Study of jet shapes in inclusive jet production
             (CDF)},
   Journal = {Phys. Rev.},
   Volume = {D71},
   Pages = {092001},
   Year = {2005},
   Key = {fds311282}
}

@article{fds309600,
   Author = {Oh, SH and al, AAE},
   Title = {Search for high mas particles decaying to lepton pairs
             (CDF)},
   Journal = {Phys. Rev. lett},
   Volume = {95},
   Pages = {252001},
   Year = {2005},
   Key = {fds309600}
}

@article{fds309601,
   Author = {Oh, SH and al, DAE},
   Title = {Measurement of charged particle multiplicities in gluson and
             quark jets},
   Journal = {Phys. Rev. lett},
   Volume = {94},
   Pages = {171802},
   Year = {2005},
   Key = {fds309601}
}

@article{fds313361,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli,
             M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron,
             S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
             C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang,
             S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker,
             GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
             P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
             I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
             SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
             M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller,
             T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu,
             C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov,
             T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh,
             SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn,
             F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
             H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
             M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba,
             A},
   Title = {Measurement of the tt̄ production cross section in pp̄
             collisions at √s=1:96 TeV using kinematic fitting of
             b-tagged lepton+jet events},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {7},
   Pages = {1-11},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   url = {http://link.aps.org/abstract/PRD/v71/e072005},
   Abstract = {We report a measurement of the tt̄ production cross section
             using the CDF II detector at the Fermilab Tevatron. The data
             consist of events with an energetic electron or muon,
             missing transverse energy, and three or more hadronic jets,
             at least one of which is identified as a b-quark jet by
             reconstructing a secondary vertex. The background fraction
             is determined from a fit of the transverse energy of the
             leading jet. Using 162 ± 10 pb -1 of data, the total cross
             section is found to be 6.0 ± 1.6(stat.) ± 1.2(syst.) pb,
             which is consistent with the standard model prediction. ©
             2005 The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.072005},
   Key = {fds313361}
}

@article{fds340925,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
             J and Culbertson, R and Dagenhart, D and D'Auria, S and Barbaro, PD and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
             C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Flores-Castillo, LR and Foster, GW and Franklin, M and Friedman, J and Furic, I and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, SR and Halkiadakis, E and Handler, R and Happacher,
             F and Hara, K and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser,
             J and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hou, S and Huffman, BT and Hughes, R and Huston, J and Incandela, J and Introzzi, G and Iori, M and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jones, M and Kamon, T and Kang, J and Unel, MK and Kartal, S and Kasha, H and Kato, Y and Kennedy, RD and Kephart, R and Kilminster, B and Kim, DH and Kim, HS and Kim, MJ and Kim,
             SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lami, S and Lammel, S and Lancaster,
             J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Mangano, M and Mariotti, M and Martin, A and Martin, M and Martin, V and Martínez, M and Mazzanti, P and McFarland, KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer,
             A and Miao, T and Miller, JS and Miller, R and Miscetti, S and Mitselmakher, G and Moggi, N and Moore, R and Moulik, T and Mukherjee,
             A and Mulhearn, M and Muller, T and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napora, R and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Niell, F and Nigmanov, T and Nodulman, L and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Ratnikov,
             F and Ray, H and Reichold, A and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson,
             L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez,
             C and Sansoni, A and Santi, L and Sarkar, S and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Sill, A and Sinervo, P and Slaughter, AJ and Sliwa, K and Snider, FD and Snihur, R and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Stefanini, A and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
             K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Tecchio,
             M and Teng, PK and Terashi, K and Tesarek, RJ and Tether, S and Thom, J and Thompson, AS and Thomson, E and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tönnesmann, M and Toyoda, H and Trischuk, W and Tseng, J and Tsybychev, D and Turini, N and Ukegawa, F and Unverhau, T and Vaiciulis, T and Varganov, A and Vataga, E and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Wagner, RG and Wagner, RL and Wagner, W and Wan, Z and Wang, C and Wang, MJ and Wang, SM and Ward, B and Waschke, S and Waters, D and Watts, T and Weber, M and III, WCW and Whitehouse, B and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
             BL and Wolbers, S and Wolter, M and Worm, S and Wu, X and Würthwein, F and Yang, UK and Yao, W and Yeh, GP and Yi, K and Yoh, J and Yoshida, T and Yu, I and Yu, S and Yun, JC and Zanello, L and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Measurement of the W boson polarization in top decay at CDF
             at √s = 1.8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {3},
   Pages = {031101-1-031101-7},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.031101},
   Abstract = {The polarization of the W boson in t →Wb decay is
             unambiguously predicted by the standard model of electroweak
             interactions and is a powerful test of our understanding of
             the tbW vertex. We measure this polarization from the
             invariant mass of the b quark from t → Wb and the lepton
             from W → lν whose momenta measure the W decay angle and
             direction of motion, respectively. In this paper we present
             a measurement of the decay rate (f V+A) of the W produced
             from the decay of the top quark in the hypothesis of V + A
             structure of the tWb vertex. We find no evidence for the
             nonstandard V + A vertex and set a limit on fV+A &lt; 0.80
             at 95% confidence level. By combining this result with a
             complementary observable in the same data, we assign a limit
             on fv+A &lt; 0.61 at 95% CL. This corresponds to a
             constraint on the right-handed helicity component of the W
             polarization of f+ &lt; 0.18 at 95% CL. This limit is the
             first significant direct constraint on fV+A in top decay. ©
             2005 The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.031101},
   Key = {fds340925}
}

@article{fds340926,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
             J and Culbertson, R and Dagenhart, D and D'Auria, S and Barbaro, PD and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
             C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Farrington, S and Feild, RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Flores-Castillo, LR and Foster, GW and Franklin, M and Friedman, J and Furic, I and Gallinaro, M and Garfinkel, AF and Gay, C and Gerdes, DW and Gerstein, E and Giagu, S and Giannetti, P and Giolo, K and Giordani, M and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn,
             SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
             J and Hennecke, M and Herndon, M and Hill, C and Hocker, A and Hoffman, KD and Hou, S and Huffman, BT and Hughes, R and Huston, J and Incandela, J and Introzzi, G and Iori, M and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jones, M and Kamon, T and Kang, J and Unel, MK and Kartal, S and Kasha, H and Kato, Y and Kennedy, RD and Kephart, R and Kilminster, B and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, TH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Koehn,
             P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lami, S and Lammel, S and Lancaster, J and Lancaster,
             M and Lander, R and Lannon, K and Lath, A and Latino, G and LeCompte, T and Le, Y and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
             T and Lockyer, NS and Loginov, A and Loreti, M and Lucchesi, D and Lukens,
             P and Lyons, L and Lys, J and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Mangano, M and Mariotti, M and Martin, A and Martin, M and Martin, V and Martínez, M and Mazzanti, P and McFarland,
             KS and McIntyre, P and Menguzzato, M and Menzione, A and Merkel, P and Mesropian, C and Meyer, A and Miao, T and Miller, JS and Miller, R and Miscetti, S and Mitselmakher, G and Moggi, N and Moore, R and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napora, R and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Niell, F and Nigmanov, T and Nodulman, L and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš,
             A and Pondrom, L and Pope, G and Poukhov, O and Pratt, T and Prokoshin, F and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine,
             A and Ratnikov, F and Ray, H and Reichold, A and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robertson, WJ and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Ryan, D and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti, A and Sill, A and Sinervo, P and Slaughter, AJ and Sliwa, K and Snider, FD and Snihur, R and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Stefanini, A and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
             K and Suzuki, T and Takashima, R and Takikawa, K and Tanaka, M and Tecchio,
             M and Teng, PK and Terashi, K and Tesarek, RJ and Tether, S and Thorn, J and Thomas, TL and Thompson, AS and Thomson, E and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tonelli, D and Tönnesmann, M and Toyoda,
             H and Trischuk, W and Tseng, J and Tsybychev, D and Turini, N and Ukegawa,
             F and Unverhau, T and Vaiciulis, T and Varganov, A and Vataga, E and III,
             SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Wagner, RG and Wagner, RL and Wagner, W and Wan, Z and Wang, C and Wang, MJ and Wang, SM and Ward, B and Waschke, S and Waters, D and Watts, T and Weber, M and III, WCW and Whitehouse, B and Wicklund, AB and Wicklund, E and Williams, HH and Wilson, P and Winer,
             BL and Wolbers, S and Wolter, M and Worm, S and Wu, X and Würthwein, F and Yang, UK and Yao, W and Yeh, GP and Yi, K and Yoh, J and Yoshida, T and Yu, I and Yu, S and Yun, JC and Zanello, L and Zanetti, A and Zetti, F and Zucchelli,
             S},
   Title = {Comparison of three-jet events in pp̄ collisions at √s =
             1.8 TeV to predictions from a next-to-leading order QCD
             calculation},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {3},
   Pages = {032002-1-032002-12},
   Year = {2005},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.032002},
   Abstract = {The properties of three-jet events with total transverse
             energy greater than 320 GeV and individual jet energy
             greater than 20 GeV have been analyzed and compared to
             absolute predictions from a next-to-leading order (NLO)
             perturbative QCD calculation. These data, of integrated
             luminosity 86 pb -1, were recorded by the CDF Experiment for
             pp collisions at √s = 1.8 TeV This study tests a model of
             higher order QCD processes that result in gluon emission and
             may give some indication of the magnitude of the
             contribution of processes higher than NLO. The total cross
             section is measured to be 466 ± 3(stat.)-70+207(syst.) pb.
             The differential cross section is furthermore measured for
             all kinematically accessible regions of the Dalitz plane,
             including those for which the theoretical prediction is
             unreliable. While the measured cross section is consistent
             with the theoretical prediction in magnitude, the two differ
             somewhat in shape in the Dalitz plane. © 2005 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.71.032002},
   Key = {fds340926}
}

@article{fds329972,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
             M},
   Title = {Measurement of Wγ and Zγ production
             in pp̄ collisions at √s = 1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {94},
   Number = {4},
   Year = {2005},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevLett.94.041803},
   Abstract = {The standard model predictions for Wγ and Z γ production
             are tested using an integrated luminosity of 200 pb-1 of
             pp̄ collision data collected at the Collider Detector at
             Fermilab. The cross sections are measured by selecting
             leptonic decays of the W and Z bosons, and photons with
             transverse energy ET > 7 GeV that are well separated from
             leptons. The production cross sections and kinematic
             distributions for the Wγ and Zγ data are compared to SM
             predictions. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.94.041803},
   Key = {fds329972}
}

@article{fds309572,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
             JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
             D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko,
             I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
             E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
             I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
             SE and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu,
             R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller,
             L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
             C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
             R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompos, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
             D},
   Title = {Measurement of the lifetime difference between Bs mass
             eigenstates.},
   Journal = {Physical review letters},
   Volume = {94},
   Number = {10},
   Pages = {101803},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.94.101803},
   Abstract = {We present measurements of the lifetimes and polarization
             amplitudes for B(0)(s)-->J/psiphi and B(0)(d)-->J/psiK(*0)
             decays. Lifetimes of the heavy and light mass eigenstates in
             the B(0)(s) system are separately measured for the first
             time by determining the relative contributions of amplitudes
             with definite CP as a function of the decay time. Using
             203+/-15 B(0)(s) decays we obtain tau(L) =
             (1.05(+0.16)(-0.13) +/- 0.02) ps and tau(H) =
             (2.07(+0.58)(-0.46) +/- 0.03) ps. Expressed in terms of the
             difference DeltaGamma(s) and average Gamma(s), of the decay
             rates of the two eigenstates, the results are
             DeltaGamma(s)/Gamma(s) = (65(+25)(-33) +/- 1)% and
             DeltaGamma(s) = (0.47(+0.19)(-0.24) +/- 0.01)
             ps(-1).},
   Doi = {10.1103/physrevlett.94.101803},
   Key = {fds309572}
}

@article{fds309573,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
             JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
             J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
             N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
             H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
             DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson,
             K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
             M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
             H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
             JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
             C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
             H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
             M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna,
             G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
             S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A},
   Title = {Search for excited and exotic electrons in the egamma decay
             channel in pp collisions at sqrt[s] = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {94},
   Number = {10},
   Pages = {101802},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.94.101802},
   Abstract = {We present a search for excited and exotic electrons (e(*))
             decaying to an electron and a photon, both with high
             transverse momentum. We use 202 pb(-1) of data collected in
             pp collisions at sqrt[s] = 1.96 TeV with the Collider
             Detector at Fermilab II detector. No signal above standard
             model expectation is seen for associated ee(*) production.
             We discuss the e(*) sensitivity in the parameter space of
             the excited electron mass M(e(*)) and the compositeness
             energy scale Lambda. In the contact interaction model, we
             exclude 132 GeV/c(2)<M(e(*))<879 GeV/c(2) for Lambda =
             M(e(*)) at 95% confidence level (C.L.). In the
             gauge-mediated model, we exclude 126 GeV/c(2) < M(e(*)) <
             430 GeV/c(2) at 95% C.L. for the phenomenological coupling
             f/Lambda approximately 10(-2) GeV-1.},
   Doi = {10.1103/physrevlett.94.101802},
   Key = {fds309573}
}

@article{fds309583,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
             M},
   Title = {Measurement of the tt̄ production cross section in pp̄
             collisions at √s = 1.96 TeV using lepton + jets events
             with secondary vertex b -tagging},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {5},
   Pages = {1-28},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.052003},
   Abstract = {We present a measurement of the tt̄ production cross
             section using events with one charged lepton and jets from
             pp̄ collisions at a center-of-mass energy of 1.96 TeV. In
             these events, heavy flavor quarks from top quark decay are
             identified with a secondary vertex tagging algorithm. From
             162 pb<sup>-1</sup> of data collected by the Collider
             Detector at Fermilab, a total of 48 candidate events are
             selected, where 13.5 ± 1.8 events are expected from
             background contributions. We measure a tt̄ production cross
             section of 5.6<inf>-1.1</inf><sup>+1.2</sup>(stat.)<inf>-0.6</inf><sup>+0.9</sup>(syst.)
             pb. © 2005 The American Physical Society.},
   Doi = {10.1103/PhysRevD.71.052003},
   Key = {fds309583}
}

@article{fds309594,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
             J and Culbertson, R and Dagenhart, D and D'Auria, S and De Barbaro and P and De Cecco and S and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi,
             C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
             S},
   Title = {Erratum: Measurement of the W boson polarization in top
             decay at CDF at √s p = 1:8 TeV (Physical Review D (2005)
             71 (031101))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {5},
   Pages = {1-2},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.059901},
   Doi = {10.1103/PhysRevD.71.059901},
   Key = {fds309594}
}

@article{fds309576,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
             M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
             R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
             AG and Clark, D and Coca, M and Connolly, A},
   Title = {Search for ZZ and ZW production in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {9},
   Pages = {1-7},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.091105},
   Abstract = {We present a search for ZZ and ZW vector boson pair
             production in pp̄ collisions at s=1.96TeV using the
             leptonic decay channels ZZ→llνν, ZZ→lll′l′, and
             ZW→lll′ν. In a data sample corresponding to an
             integrated luminosity of 194pb-1 collected with the Collider
             Detector at Fermilab, 3 candidate events are found with an
             expected background of 1.0±0.2 events. We set a 95%
             confidence level upper limit of 15.2pb on the cross section
             for ZZ plus ZW production, compared to the standard model
             prediction of 5.0±0.4pb. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.71.091105},
   Key = {fds309576}
}

@article{fds309591,
   Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
             A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli,
             G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway,
             J},
   Title = {Search for scalar leptoquark pairs decaying to νν̄qq̄ in
             pp̄ collisions at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {71},
   Number = {11},
   Pages = {1-7},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.71.112001},
   Abstract = {We report on a search for the pair production of scalar
             leptoquarks (LQ), using 191pb-1 of proton-antiproton
             collision data recorded by the CDF experiment during Run II
             of the Tevatron. The leptoquarks are sought via their decay
             into a neutrino and quark yielding missing transverse energy
             and several jets of large transverse energy. No evidence for
             LQ production is observed, and limits are set on
             σ(pp̄→LQLQ̄X→νν̄qq̄X). Using a next-to-leading
             order theoretical prediction of the cross section for LQ
             production, we exclude first-generation LQ in the mass
             interval 78 to 117GeV/c2 at the 95% confidence level for
             BR(LQ→νq)=100%. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.71.112001},
   Key = {fds309591}
}

@article{fds309596,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
             J and Culbertson, R and Dagenhart, D and D'Auria, S and De Barbaro and P and Cecco, SD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi,
             C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
             S},
   Title = {KS0 and Λ0 production studies in pp̄ collisions at s=1800
             and 630 GeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {72},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.052001},
   Abstract = {We present a study of the production of KS0 and Λ0 in
             inelastic pp̄ collisions at s=1800 and 630 GeV using data
             collected by the CDF experiment at the Fermilab Tevatron.
             Analyses of KS0 and Λ0 multiplicity and transverse momentum
             distributions, as well as of the dependencies of the average
             number and pT of KS0 and Λ0 on charged particle
             multiplicity, are reported. Systematic comparisons are
             performed for the full sample of inelastic collisions, and
             for the low and high momentum transfer subsamples, at the
             two energies. The pT distributions extend above 8GeV/c,
             showing a pT higher than previous measurements. The
             dependence of the mean KS0(Λ0) pT on the charged particle
             multiplicity for the three samples shows a behavior
             analogous to that of charged primary tracks. © 2005 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.72.052001},
   Key = {fds309596}
}

@article{fds309595,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu, ML and Chung,
             JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw,
             J and Culbertson, R and Dagenhart, D and D'Auria, S and De Barbaro and P and De Cecco and S and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi,
             C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede, D and Errede,
             S},
   Title = {Search for supersymmetric Higgs bosons in the di-tau decay
             mode in pp̄ collisions at s=1.8TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {72},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.072004},
   Abstract = {A search for the direct production of Higgs bosons in the
             di-tau decay mode is performed with 86.3±3.5pb-1 of data
             collected with the Collider Detector at Fermilab during the
             1994-1995 data taking period of the Tevatron. We search for
             events where one tau decays to an electron plus neutrinos
             and the other tau decays hadronically. We perform a counting
             experiment and set limits on the cross section for
             supersymmetric Higgs boson production where tan β is large
             and mA is small. For a benchmark parameter space point where
             mA0=100GeV/c2 and tan β=50, we limit the production cross
             section multiplied by the branching ratio to be less than
             77.9 pb at the 95% confidence level compared to the
             theoretically predicted value of 11.0 pb. This is the first
             search for Higgs bosons decaying to tau pairs at a hadron
             collider. © 2005 The American Physical Society.},
   Doi = {10.1103/PhysRevD.72.072004},
   Key = {fds309595}
}

@article{fds309599,
   Author = {Cwetanski, P and Åkesson, T and Eerola, P and Lundberg, B and Mjornmark, U and Anghinolfi, F and Baron, S and Capeans, M and Cardiel-Sas, L and Catinaccio, A and Danielsson, H and Dittus, F and Farthouat, P and Froidevaux, D and Ghodbane, N and Grognuz, J and Krüger, K and Lichard, P and Mitsou, VA and Petti, R and Price, M and Rembser, C and Sprachmann, G and Arik, E and Cetin, SA and Baker, OK and McFarlane, KW and Shin, T and Vassilakopoulos, VI and Baná, E and Hajduk, Z and Olszowska, J and Benjamin, D and Ebenstein, WL and Oh, SH and Wang, C and Bertelsen, H and Dam, M and Hansen, P and Kittelmann, T and Mackeprang, R and Bondarenko, V and Dolgoshein, B and Markina, I and Morozov, S and Romaniouk, A and Smirnov, S and Sosnovtsev, V and Soutchkov, S and Bytchkov, V and Grigalashvili, N and Kekelidze, G and Mialkovski, V and Michine, S and Peshekhonov, V and Callahan, J and Gagnon, P and Luehring, F and Ogren, H and Rust, DR and Chandler, JT and Gay, C and Martin, AJ and Schmidt, MP and Dressnandt, N and Keener, PT and le Geyt, BC and Munar, A and Newcomer, FM and Rohne, O and van Berg, R and Williams, HH and Egorov, K and Fedin, O and Katunin, S and Khristatchev,
             A and Koudine, L and Kovalenko, S and Maleev, V and Nadtochy, A and Nesterov, S and Oleshko, S and Patritchev, S and Ryabov, Y and Schegelsky, V and Seliverstov, D and Zalite, A and Zalite, Y and Grichkevitch, Y and Kramarenko, VA and Laritchev, A and Nikitine, N and Kayumov, F and Konovalov, S and Muraviev, S and Shmeleva, A and Tikhomirov, V and Vassilieva, L and Kowalski, T and Mindur,
             B},
   Title = {Acceptance tests and criteria of the ATLAS transition
             radiation tracker},
   Journal = {IEEE Transactions on Nuclear Science},
   Volume = {52},
   Number = {6},
   Pages = {2911-2916},
   Publisher = {Institute of Electrical and Electronics Engineers
             (IEEE)},
   Year = {2005},
   Month = {December},
   url = {http://dx.doi.org/10.1109/TNS.2005.862799},
   Abstract = {The Transition Radiation Tracker (TRT) sits at the outermost
             part of the ATLAS Inner Detector, encasing the Pixel
             Detector and the Semi-Conductor Tracker (SCT). The TRT
             combines charged particle track reconstruction with electron
             identification capability. This is achieved by layers of
             xenonfilled straw tubes with periodic radiator foils or
             fibers providing TR photon emission. The design and choice
             of materials have been optimized to cope with the harsh
             operating conditions at the LHC, which are expected to lead
             to an accumulated radiation dose of 10 Mrad and a neutron
             fluence of up to 2 · 10 14 n/cm2 after ten years of
             operation. The TRT comprises a barrel containing 52 000
             axial straws and two end-cap parts with 320 000 radial
             straws. The total of 420 000 electronic channels (two
             channels per barrel straw) allows continuous tracking with
             many projective measurements (more than 30 straw hits per
             track). The assembly of the barrel modules in the US has
             recently been completed, while the end-cap wheel
             construction in Russia has reached the 50% mark. After
             testing at the production sites and shipment to CERN, all
             modules and wheels undergo a series of quality and
             conformity measurements. These acceptance tests survey
             dimensions, wire tension, gas-tightness, high-voltage
             stability and gas-gain uniformity along each individual
             straw. This paper gives details on the acceptance criteria
             and measurement methods. An overview of the most important
             results obtained to-date is also given. © 2005
             IEEE.},
   Doi = {10.1109/TNS.2005.862799},
   Key = {fds309599}
}

@article{fds309603,
   Author = {Åkesson, T and Anghinolfi, F and Arik, E and Baker, OK and Banas, E and Baron, S and Benjamin, D and Bertelsen, H and Bondarenko, V and Bytchkov, V and Callahan, J and Capeáns, M and Cardiel-Sas, L and Catinaccio, A and Cetin, SA and Chandler, JT and Cwetanski, P and Dam,
             M and Danielsson, H and Dittus, F and Dolgoshein, B and Dressnandt, N and Driouichi, C and Ebenstein, WL and Eerola, P and Egorov, K and Farthouat, P and Fedin, O and Froidevaux, D and Gagnon, P and Gay, C and Ghodbane, N and Grichkevitch, Y and Grigalashvili, N and Grognuz, J and Hajduk, Z and Hansen, P and Katunin, S and Kayumov, F and Keener, PT and Kekelidze, G and Khristatchev, A and Kittelmann, TH and Konovalov, S and Koudine, L and Kovalenko, S and Kowalski, T and Kramarenko, VA and Krüger, K and Laritchev, A and LeGeyt, B and Lichard, P and Luehring,
             F and Lundberg, B and Mackeprang, R and Maleev, V and Markina, I and Martin, AJ and McFarlane, KW and Mialkowski, V and Michine, S and Mindur, B and Mitsou, VA and Mjörnmark, U and Morozov, S and Munar, A and Muraviev, S and Nadtochy, A and Nesterov, S and Newcomer, FM and Nikitine, N and Ogren, H and Oh, SH and Oleshko, S and Olszowska, J and Patritchev, S and Peshekhonov, V and Petti, R and Price, M and Rembser,
             C and Røhne, O and Romaniouk, A and Rust, DR and Ryabov, Y and Ryjov, V and Schegelsky, V and Schmidt, MP and Seliverstoy, D and Shin, T and Shmeleva, A and Smirnov, S and Sosnovtsev, V and Soutchkov, S and Sprachmann, G and Tikhomirov, V and Van Berg and R and Vassilakopoulos,
             VI and Vassilieva, L and Wang, C and Williams, HH},
   Title = {Aging effects in the ATLAS transition radiation tracker and
             gas filtration studies},
   Journal = {IEEE Nuclear Science Symposium Conference
             Record},
   Volume = {2},
   Pages = {1185-1190},
   Publisher = {IEEE},
   Year = {2005},
   Month = {December},
   url = {http://dx.doi.org/10.1109/NSSMIC.2005.1596462},
   Abstract = {The Transition Radiation Tracker (TRT) is one of three
             particle tracking detectors now under construction for the
             ATLAS experiment, whose goal is to exploit the highly
             exciting new physics potential at CERN's next accelerator,
             the so called Large Hadron Collider (LHC). The TRT consists
             of 370000 straw proportional tubes of 4 mm diameter with a
             30 micron thick anode wire, which will be operated with a
             Xe/CO2/O2 gas mixture at a high voltage of approximately 1.5
             kV. While the construction of the TRT is now well under way,
             a number of interesting and challenging questions need to be
             solved with regard to wire aging phenomena, which are
             induced by pollution originating from very small amounts of
             silicon-based vacuum materials in some components of the gas
             system. Finally a guideline to avoid aging in wire chamber
             detectors in high luminosity experiments is given. © 2005
             IEEE.},
   Doi = {10.1109/NSSMIC.2005.1596462},
   Key = {fds309603}
}

@article{fds309575,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
   Title = {Erratum: Search for Bs0 → μ+μ and Bd0 → μ+μ decays
             in pp_ collisions with CDF II (Phys. Rev. Lett. (2005) 95
             (221805))},
   Journal = {Physical Review Letters},
   Volume = {95},
   Number = {24},
   Publisher = {American Physical Society (APS)},
   Year = {2005},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.95.249905},
   Doi = {10.1103/PhysRevLett.95.249905},
   Key = {fds309575}
}

@article{fds309525,
   Author = {Abulencia, and A, and others},
   Title = {Observation of $B^0_s \to K^{+} K^{-}$ and Measurements of
             Branching Fractions of Charmless Two-body Decays of $B^0$
             and $B^0_{s}$ Mesons in $\bar{p} p$ Collisions at $\sqrt{s}$
             = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {21},
   Pages = {211802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.211802},
   Abstract = {We search for decays of the type B(s)0-->h+h[prime]- (where
             h,h[prime]=K or pi) in 180 pb-1 of [overline p]p collisions
             collected at the Tevatron by the upgraded Collider Detector
             at Fermilab. We report the first observation of the new mode
             Bs0-->K+K- with a yield of 236$\pm$32 events, corresponding
             to (fs/fd)?[script B](Bs0-->K+K-)/[script
             B](B0-->K+pi-)=0.46$\pm$0.08(stat)$\pm$0.07(syst), where
             fs/fd is the ratio of production fractions of Bs0 and B0. We
             find results in agreement with world averages for the B0
             modes, and set the following new limits at 90\% C.L.:
             [script B](Bs0-->K-pi+)s0-->pi+pi-)},
   Doi = {10.1103/physrevlett.97.211802},
   Key = {fds309525}
}

@article{fds309526,
   Author = {Abulencia, and A, and others},
   Title = {Search for large extra dimensions in the production of jets
             and missing transverse energy in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {17},
   Pages = {171802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.171802},
   Abstract = {We present the results of a search for new physics in the
             jets plus missing transverse energy data sample collected
             from 368 pb-1 of p anti-p collisions at s**(1/2) = 1.96 TeV
             recorded by the Collider Detector at Fermilab. We compare
             the number of events observed in the data with a data-based
             estimate of the standard model backgrounds contributing to
             this signature. We observe no significant excess of events,
             and we interpret this null result in terms of lower limits
             on the fundamental Planck scale for a large extra dimensions
             scenario.},
   Doi = {10.1103/physrevlett.97.171802},
   Key = {fds309526}
}

@article{fds309528,
   Author = {Abulencia, and A, and others},
   Title = {Search for a neutral Higgs boson decaying to a W boson pair
             in $p\bar{p}$ collisions at $\sqrt{s} =$
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {8},
   Pages = {081802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.081802},
   Abstract = {We present the results of a search for standard model Higgs
             boson production with decay to WW*, identified through the
             leptonic final states e+e-nu-bar nu, e+/- mu-/+ nu-bar nu
             and mu+ mu- nu-bar nu. This search uses 360 pb-1 of data
             collected from p anti-p collisions at s**(1/2) = 1.96 TeV by
             the upgraded Collider Detector at Fermilab (CDF II). We
             observe no signal excess and set 95% confidence level upper
             limits on the production cross section times branching ratio
             for the Higgs boson to WW* or any new scalar particle with
             similar decay products. These upper limits range from 5.5 to
             3.2 pb for Higgs boson masses between 120 and 200
             GeV/c2.},
   Doi = {10.1103/physrevlett.97.081802},
   Key = {fds309528}
}

@article{fds309529,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the B/s0 anti-B/s0 oscillation
             frequency},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {6},
   Pages = {062003},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.062003},
   Abstract = {We measure the masses of $b$ hadrons in exclusively
             reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
             decay using $\rm 220 pb^{-1}$ of data collected by the CDF
             II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
             \pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
             \pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
             0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
             5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
             m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
             m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
             0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
             1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
             the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
             $m(\Lambda^0_b)-m(B^0)$ mass difference are of better
             precision than the current world averages.},
   Doi = {10.1103/physrevlett.97.062003},
   Key = {fds309529}
}

@article{fds309530,
   Author = {Abulencia, and A, and others},
   Title = {Search for new physics in lepton + photon + X events with
             305-pb**(-1) of p anti-p collisions at s**(1/2) = 1.96-
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {97},
   Number = {3},
   Pages = {031801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.97.031801},
   Abstract = {We present results of a search for anomalous production of
             events containing a charged lepton (either electron or muon)
             and a photon, both with high transverse momentum,
             accompanied by additional signatures, X, including missing
             transverse energy (MET) and additional leptons and photons.
             We use the same kinematic selection criteria as in a
             previous CDF search, but with a substantially larger data
             set, 305 pb-1, a ppbar collision energy of 1.96 TeV, and the
             upgraded CDF II detector. We find 42 Lepton+Photon+MET
             events versus a standard model expectation of 37.3 +- 5.4
             events. The level of excess observed in Run I, 16 events
             with an expectation of 7.6 +- 0.7 events (corresponding to a
             2.7 sigma effect), is not supported by the new data. In the
             signature of Multi-Lepton+Photon+X we observe 31 events
             versus an expectation of 23.0 +- 2.7 events. In this sample
             we find no events with an extra photon or MET and so find no
             events like the one ee+gg+MET event observed in Run
             I.},
   Doi = {10.1103/physrevlett.97.031801},
   Key = {fds309530}
}

@article{fds309532,
   Author = {Abulencia, and A, and others},
   Title = {Search for high-mass resonances decaying to e mu in
             $p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {21},
   Pages = {211802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.211802},
   Abstract = {We describe a general search for resonances decaying to a
             neutral e mu final state in p anti-p collisions at a
             center-of-mass energy of 1.96 TeV. Using a data sample
             representing 344 pb-1 of integrated luminosity recorded by
             the CDF II experiment, we compare Standard Model predictions
             with the number of observed events for invariant masses
             between 50 and 800 GeV/c2. Finding no significant excess (5
             events observed vs. 7.7 +/- 0.8 expected for M_e mu > 100
             GeV/c2), we set limits on sneutrino and Z' masses as
             functions of lepton family number violating
             couplings.},
   Doi = {10.1103/physrevlett.96.211802},
   Key = {fds309532}
}

@article{fds309533,
   Author = {Abulencia, and A, and others},
   Title = {Direct search for Dirac magnetic monopoles in $p\bar{p}$
             collisions at $\sqrt{s} = 1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {20},
   Pages = {201801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.201801},
   Abstract = {We search for pair-produced Dirac magnetic monopoles in 35.7
             pb-1 of proton-antiproton collisions at s**(1/2) = 1.96 TeV
             with the Collider Detector at Fermilab (CDF). We find no
             monopole candidates corresponding to a 95\% confidence-level
             cross-section limit sigma 360 GeV/c2.},
   Doi = {10.1103/physrevlett.96.201801},
   Key = {fds309533}
}

@article{fds309534,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the $t\bar{t}$ production cross section in
             $p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV using missing
             $E_t$ + jets events with secondary vertex $b-
             $tagging},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {20},
   Pages = {202002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.202002},
   Abstract = {We present a measurement of the tt-bar production cross
             section in p anti-p collisions at s**(1/2) = 1.96 TeV which
             uses events with an inclusive signature of significant
             missing transverse energy and jets. This is the first
             measurement which makes no explicit lepton identification
             requirements, so that sensitivity to W --> tau nu decays is
             maintained. Heavy flavor jets from top quark decay are
             identified with a secondary vertex tagging algorithm. From
             311 pb-1 of data collected by the Collider Detector at
             Fermilab we measure a production cross section of 5.8 +/-
             1.2(stat.)+0.9_-0.7(syst.) pb for a top quark mass of 178
             GeV/c2, in agreement with previous determinations and
             standard model predictions.},
   Doi = {10.1103/physrevlett.96.202002},
   Key = {fds309534}
}

@article{fds309535,
   Author = {Acosta, and D, and others},
   Title = {Measurement of $b$ hadron masses in exclusive $J/\psi$
             decays with the CDF detector},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {20},
   Pages = {202001},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.202001},
   Abstract = {We measure the masses of $b$ hadrons in exclusively
             reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
             decay using $\rm 220 pb^{-1}$ of data collected by the CDF
             II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
             \pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
             \pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
             0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
             5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
             m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
             m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
             0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
             1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
             the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
             $m(\Lambda^0_b)-m(B^0)$ mass difference are of better
             precision than the current world averages.},
   Doi = {10.1103/physrevlett.96.202001},
   Key = {fds309535}
}

@article{fds309536,
   Author = {Abulencia, and A, and others},
   Title = {A search for scalar bottom quarks from gluino decays in
             $\bar{p}p$ collisions at $\sqrt{s} =$ 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {17},
   Pages = {171802},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.171802},
   Abstract = {We searched for scalar bottom quarks in 156 pb-1 of p anti-p
             collisions at s**(1/2) = 1.96 TeV recorded by the CDF II
             experiment at the Tevatron. Scalar bottom quarks can be
             produced from gluino decays in R-parity conserving models of
             supersymmetry when the mass of the gluino exceeds that of
             the scalar bottom quark. Then, a scalar bottom quark. Then,
             a scalar bottom quark can decay into a bottom quark and a
             neutralino. To search for this scenario, we investigated
             events with large missing transverse energy and at least
             three jets, two or more of which were identified as
             containing a secondary vertex from the hadronization of b
             quarks. We found four candidate events, where 2.6 +/- 0.7
             are expected from standard model processes, and placed 95\%
             confidence level lower limits on gluino and scalar bottom
             quark masses of up to 280 and 240 GeV/c2,
             respectively.},
   Doi = {10.1103/physrevlett.96.171802},
   Key = {fds309536}
}

@article{fds309537,
   Author = {Abulencia, and A, and others},
   Title = {Top quark mass measurement from dilepton events at CDF
             II},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {15},
   Pages = {152002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.152002},
   Abstract = {We report a measurement of the top quark mass using events
             collected by the CDF II Detector from p anti-p collisions at
             s**(1/2) = 1.96 TeV at the Fermilab Tevatron. We calculate a
             likelihood function for the top mass in events that are
             consistent with t anti-t --> b-bar l- nu-bar_l bl'+ nu'_l
             decays. The likelihood is formed as the convolution of the
             leading-order matrix element and detector resolution
             functions. The joint likelihood is the product of
             likelihoods for each of 33 events collected in 340 pb-1 of
             integrated luminosity, yielding a top quark mass M_t = 165.2
             +/- 6.1(stat.) +/- 3.4(syst.) GeV/c2. This first application
             of a matrix-element technique to tt-bar --> bl+ nu_l b-bar
             l'- nu-bar_l' decays gives the most precise single
             measurement of M_t in dilepton events. Combined with other
             CDF Run II measurements using dilepton events, we measure
             M_t = 167.9 +/- 5.2(stat.) +/- 3.7(syst.)
             GeV/c2.},
   Doi = {10.1103/physrevlett.96.152002},
   Key = {fds309537}
}

@article{fds309539,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the dipion mass spectrum in X(3872) --> J/psi
             pi+ pi- decays},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {10},
   Pages = {102002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.102002},
   Abstract = {We measure the dipion mass spectrum in X(3872) --> J/psi
             pi++ pi+- decays using 360 pb-1 of p anti-p collisions at
             s**(1/2) = 1.96 TeV collected with the CDF II detector. The
             spectrum is fit with predictions for odd C-parity (3S_1,
             1P_1, and 3D_J) charmonia decaying to J/psi pi++ pi+-, as
             well as even C-parity states in which the pi+ons are from
             rho0 decay. The latter case also encompasses exotic
             interpretations, such as D0 D-bar*0 molecule. Only the 3S_1
             and J/psi rho hypotheses are compatible with our data. Since
             3S_1 is untenable on other grounds, decay via J/psi rho is
             favored, which implies C = +1 for the X(3872). Models for
             different J/psi-rho angular momenta L are considered.
             Flexibility in the models, especially the introduction of
             rho-omega interference, enable good descriptions of our data
             for both L = 0 and 1.},
   Doi = {10.1103/physrevlett.96.102002},
   Key = {fds309539}
}

@article{fds309541,
   Author = {Acosta, and D, and others},
   Title = {Evidence for the exclusive decay B/c+- --> J/psi pi+- and
             measurement of the mass of the B/c meson},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {8},
   Pages = {082002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.082002},
   Abstract = {We report first evidence for a fully reconstructed decay
             mode of the B+/-_c meson in the channel B+/-_c --> J/psi
             pi++/-, with J/psi --> mu+ mu-. The analysis is based on an
             integrated luminosity of 360 pb-1 in p anti-p collisions at
             1.96 TeV center of mass energy collected by the Collider
             Detector at Fermilab. We observe 14.6 +/- 4.6 signal events
             with a background of 7.1 +/- 0.9 events, and a fit to the
             J/psi pi++/- mass spectrum yields a B+/-_c mass of 6285.7
             +/- 5.3 (stat) +/- 1.2 (syst) MeV/c2. The probability of a
             peak of this magnitude occurring by random fluctuation in
             the search region is estimated as 0.012\%.},
   Doi = {10.1103/physrevlett.96.082002},
   Key = {fds309541}
}

@article{fds309542,
   Author = {Abulencia, and A, and others},
   Title = {Search for charged Higgs bosons from top quark decays in p
             anti-p collisions at $\sqrt{s}$ = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {4},
   Pages = {042003},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.042003},
   Abstract = {We report the results of a search for a charged Higgs boson
             in the decays of top quarks produced in p anti-p collisions
             at a center-of-mass energy of 1.96 GeV. We use a data sample
             corresponding to an integrated luminosity of 193 pb-1
             collected by the upgraded Collider Detector at Fermilab. No
             evidence for charged Higgs production is found, allowing 95%
             C.L. upper limits to be placed on BR(t --> H+b) for
             different charged Higgs decay scenarios. In addition, we
             present in the MSSM (m_H+/-, tan B) plane the first
             exclusion regions with radiative and Yukawa coupling
             corrections.},
   Doi = {10.1103/physrevlett.96.042003},
   Key = {fds309542}
}

@article{fds309543,
   Author = {Abulencia, and A, and others},
   Title = {Precision top quark mass measurement in the lepton + jets
             topology in p anti-p collisions at $\sqrt{s}=$
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {2},
   Pages = {022004},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.022004},
   Abstract = {We report two measurements of the top quark mass M_top using
             the CDF II detector at the Fermilab Tevatron in a 318 pb-1
             data sample observed in the lepton + jets final state. One
             method uses an event-based likelihood technique resulting in
             M_top = 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2 or
             173.2+4.1_-40 GeV/c2. The second method reconstructs a top
             quark mass in each event using the measured invariant mass
             of the hadronically decaying W boson to constrain the jet
             energy scale to obtain a value for M_top of 173.5+3.7_-3.6
             (stat.) +/- 1.3 (syst.) GeV/c2 or 173.5+3.9_-3.8 GeV/c2. We
             take the latter, which is more precise, as our
             result.},
   Doi = {10.1103/physrevlett.96.022004},
   Key = {fds309543}
}

@article{fds309545,
   Author = {Abulencia, and A, and others},
   Title = {Top quark mass measurement using the template method in the
             lepton + jets channel at CDF II},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.032003},
   Abstract = {This article presents a measurement of the top quark mass
             using the CDF II detector at Fermilab. Colliding beams of
             protons and anti-protons at Fermilab's Tevatron (s**(1/2) =
             1.96 TeV) produce top/anti-top pairs, which decay to W+ W-
             bb-bar; events are selected where one W decays to hadrons,
             and the other W decays to either e or mu plus a neutrino.
             The data sample corresponds to an integrated luminosity of
             approximately 318 pb-1. A total of 165 tt-bar events are
             separated into four subsamples based on jet transverse
             energy thresholds and the number of b jets identified by
             reconstructing a displaced vertex. In each event, the
             reconstructed top quark invariant mass is determined by
             minimizing a chi2 for the overconstrained kinematic system.
             At the same time, the mass of the hadronically decaying W
             boson is measured in the same event sample. The observed W
             boson mass provides an in situ improvement in the
             determination of the hadronic jet energy scale, JES. A
             simultaneous likelihood fit of the reconstructed top quark
             masses and the W boson invariant masses in the data sample
             to distributions from simulated signal and background events
             gives a top quark mass of 173.5+3.7_-3.6(stat. + JES) +/-
             1.3 (other syst.) GeV/c2, or 173.5+3.9_-3.8
             GeV/c2.},
   Doi = {10.1103/PhysRevD.73.032003},
   Key = {fds309545}
}

@article{fds309547,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of mass and width of the excited charmed meson
             states D10 and D2*0},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {5},
   Pages = {051104},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.051104},
   Abstract = {We report on precision measurements of the masses and widths
             of the narrow, orbitally excited states D0_1 and D*0_2 using
             the CDF II detector at the Fermilab Tevatron. Both states
             (collectively called D**) are reconstructed in the decay
             channel D** --> D*+ pi+-. The D*0_s is also reconstructed in
             the D** --> D+ pi+- channel. Using a dataset with an
             integrated luminosity of 210 pb-1, the measured masses and
             widths for the D0_1 are 2421.7 +/- 0.7 +/- 0.6 MeV/c2 and
             20.0 +/- 1.7 +/- 1.3 MeV/c2 respectively, while for the
             D*0_2 they are 2463.3 +/- 0.6 +/- 0.8 MeV/c2 and 49.2 +/-
             2.3 +/- 1.2 MeV/c2. These values are currently the single
             best measurements available.},
   Doi = {10.1103/PhysRevD.73.051104},
   Key = {fds309547}
}

@article{fds309550,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the inclusive jet cross section in ppbar
             Interactions at sqrt{s}=1.96 TeV Using a Cone-based Jet
             Algorithm},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {7},
   Pages = {071103},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.071103},
   Abstract = {We present a measurement of the inclusive jet cross section
             in ppbar interactions at sqrt{s}=1.96 TeV using 385 pb^{-1}
             of data collected with the CDF II detector at the Fermilab
             Tevatron. The results are obtained using an improved
             cone-based jet algorithm (Midpoint). The data cover the jet
             transverse momentum range from 61 to 620 GeV/c, extending
             the reach by almost 150 GeV/c compared with previous
             measurements at the Tevatron. The results are in good
             agreement with next-to-leading order perturbative QCD
             predictions using the CTEQ6.1M parton distribution
             functions.},
   Doi = {10.1103/PhysRevD.74.071103},
   Key = {fds309550}
}

@article{fds309551,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the top quark mass with the dynamical
             likelihood method using lepton plus jets events with b-tags
             in $p\bar{p}$ collisions at $\sqrt{s} =$
             1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.092002},
   Abstract = {This report describes a measurement of the top quark mass,
             M_top, with the dynamical likelihood method (DLM) using the
             CDF II detector at the Fermilab Tevatron. The Tevatron
             produces top/anti-top (t anti-t) pairs in p anti-p
             collisions at a center-of-mass energy of 1.96 TeV. The data
             sample used in this analysis was accumulated from March 2002
             through August 2004, which corresponds to an integrated
             luminosity of 318 pb-1. We use the tt-bar candidates in the
             ``epton+jets'' decay channel, requiring at least one jet
             identified as a b quark by finding a displaced secondary
             vertex. The DLM defines a likelihood for each event based on
             the differential cross section s a function of M_top per
             unit phase space volume of the final partons, multiplied by
             the transfer functions from jet to parton energies. The
             method takes into account all possible jet combinations in
             an event, and the likelihood is multiplied event by event to
             derive the top quark mass by the maximum likelihood method.
             Using 63 tt-bar candidates observed in the data, with 9.2
             events expected from background, we measure the top quark
             mass to be 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2, or
             173+4.1_-4.0 GeV/c2.},
   Doi = {10.1103/PhysRevD.73.092002},
   Key = {fds309551}
}

@article{fds309552,
   Author = {Abulencia, and A, and others},
   Title = {Search for anomalous semileptonic decay of heavy flavor
             hadrons produced in association with a W boson at CDF
             II},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {5},
   Pages = {051101},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.051101},
   Abstract = {We present a search for anomalous semileptonic decays of
             heavy flavor hadrons produced in association with a W boson,
             in proton-antiproton collisions at s**(1/2) = 1.96 TeV. We
             use 162 pb-1 of data collected with the CDF II detector at
             the Fermilab Tevatron Collider. We select events with one W
             boson and at least one jet with an identified secondary
             vertex. In the jets with a secondary vertex we look for a
             semileptonic decay to a muon. We compare the number of jets
             with both a secondary vertex and a semileptonic decay, and
             the kinematic properties of these jets, with the standard
             model expectation, and we set limits on the production cross
             section of a B-like hadron with an anomalously high
             semileptonic branching ratio.},
   Doi = {10.1103/PhysRevD.73.051101},
   Key = {fds309552}
}

@article{fds309554,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri,
             A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Ruzza, BD and Dionisi,
             C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro,
             M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn,
             SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer,
             A and Heinemann, B and Heinrich, J and Herndon, M and Hidas, D and Hill,
             CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden,
             M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon,
             EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart,
             R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
             YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
             M},
   Title = {Search for excited and exotic muons in the μy decay channel
             in pp - collisions at s=1.96 TeV},
   Journal = {Physical Review Letters},
   Volume = {97},
   Number = {19},
   Pages = {191802},
   Year = {2006},
   ISSN = {0031-9007},
   url = {http://www.ncbi.nlm.nih.gov/pubmed/17155615},
   Abstract = {We search for excited and exotic muon states * using an
             integrated luminosity of 371pb-1 of pp collision data at
             s=1.96TeV. We search for associated production of * followed
             by the decay *. We compare the data to model predictions as
             a function of the mass of the excited muon M *, the
             compositeness energy scale , and the gauge coupling factor
             f. No signal above the standard model expectation is
             observed. We exclude 107&lt;M *&lt;853GeV/c2 for =M * in the
             contact interaction model, and 100&lt;M *&lt;410GeV/c2 for
             f/=10-2GeV-1 in the gauge-mediated model, both at the 95%
             confidence level. © 2006 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.97.191802},
   Key = {fds309554}
}

@article{fds361228,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, J and DiTuro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Sciverez, MG and Garfinkel, AF and Gay,
             C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
             S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute,
             M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
             R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
             AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori,
             L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
             S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez,
             C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
             A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro,
             MD},
   Title = {Measurement of the ratios of branching fractions
             B(Bs0→Ds-π+)/ B(B0→D-π+) and B(B+→D̄0π+)/B(B0→D-π+)},
   Journal = {Physical Review Letters},
   Volume = {96},
   Number = {19},
   Pages = {191801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.96.191801},
   Abstract = {We report an observation of the decay Bs0→Ds-π+ in pp̄
             collisions at s=1.96TeV using 115pb-1 of data collected by
             the CDF II detector at the Fermilab Tevatron. We observe
             83±11(stat) Bs0→Ds-π+ candidates, representing a large
             increase in statistics over previous measurements and the
             first observation of this decay at a pp̄ collider. We
             present the first measurement of the relative branching
             fraction B(Bs0→Ds-π+)/B(B0→D-π+)=1.32±0.18(stat)±0.38(syst)
             . We also measure B(B+→D̄0π+)/B(B0→D-π+)=1.97±0.
             10(stat)±0.21(syst), which is consistent with previous
             measurements. © 2006 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.96.191801},
   Key = {fds361228}
}

@article{fds309559,
   Author = {Abulencia, and A, and others},
   Title = {Top quark mass measurement from dilepton events at CDF II
             with the matrix-element method},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {3},
   Pages = {032009},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.032009},
   Abstract = {We describe a measurement of the top quark mass using events
             with two charmed leptons collected by the CDF II detector
             from p anti-p collisions with s**(1/2) = 1.96 TeV at the
             Fermilab Tevatron. The likelihood in top mass is calculated
             for each event by convoluting the leading order matrix
             element describing qqbar --> t anti-t --> b l nu_l b-bar l'
             nu_l' with detector resolution functions. The presence of
             background events in the data sample is modeled using
             similar calculations involving the matrix elements for major
             background processes. In a data sample with integrated
             luminosity of 340 pb-1, we observe 33 candidate events and
             measure M_top = 165.2 +/- 6.1(stat.) +/- 3.4(syst.) GeV/c2.
             This measurement represents the first application of this
             method to events with two charged leptons and is the most
             precise single measurement of the top quark mass in this
             channel.},
   Doi = {10.1103/PhysRevD.74.032009},
   Key = {fds309559}
}

@article{fds309560,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
             T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
             N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser,
             J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon,
             M and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato,
             Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
             R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian,
             C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
             YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin,
             J},
   Title = {Measurement of the ratio of branching fractions
             B(D0→K+π-)/ B(D0→K-π+) using the CDF II
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {74},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.031109},
   Abstract = {We present a measurement of RB, the ratio of the branching
             fraction for the rare decay D0→K+π- to that for the
             Cabibbo-favored decay D0→K-π+. Charge-conjugate decays
             are implicitly included. A signal of 2005±104 events for
             the decay D0→K+π- is obtained using the CDF II detector
             at the Fermilab Tevatron collider. The data set corresponds
             to an integrated luminosity of 0.35fb-1 produced in p̄p
             collisions at s=1.96TeV. Assuming no mixing, we find
             RB=[4.05±0.21(stat)±0.11(syst)] ×10-3. This measurement
             is consistent with the world average, and comparable in
             accuracy with the best measurements from other experiments.
             © 2006 The American Physical Society.},
   Doi = {10.1103/PhysRevD.74.031109},
   Key = {fds309560}
}

@article{fds309562,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the top quark mass using template methods on
             dilepton events in proton antiproton collisions at $\sqrt{s}
             =$ 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {11},
   Pages = {112006},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.112006},
   Abstract = {We describe a measurement of the top quark mass from events
             produced in p anti-p collisions at a center-of-mass energy
             of 1.96 TeV, using the Collider Detector at Fermilab. We
             identify tt-bar candidates where both W bosons from the top
             quarks decay into leptons (e mu, mu nu, or tau nu) from a
             data sample of 360 pb-1. The top quark mass is reconstructed
             in each event separately by three different methods, which
             draw upon simulated distributions of the neutrino
             pseudorapi+dity, tt-bar longitudinal momentum, or neutrino
             azimuthal angle in order to extract probability
             distributions for the top quark mass. For each method,
             representative mass distributions, or templates, are
             constructed from simulated samples of signal and background
             events, and parametrized templates is then performed on the
             data sample masses in order to derive a final top quark
             mass. Combining the three template methods, taking into
             account correlations in their statistical and systematic
             uncertainties, results in a top quark mass measurement of
             170.1 +/- 6.0 (stat.) +/- 4.1 (syst.) GeV/c2.},
   Doi = {10.1103/PhysRevD.73.112006},
   Key = {fds309562}
}

@article{fds309564,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the b jet cross section in events with a Z
             boson in $p\bar{p}$ collisions at $\sqrt{s} =$
             1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {3},
   Pages = {032008},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.032008},
   Abstract = {A measurement of the inclusive bottom jet cross section is
             presented for events containing a Z boson in p anti-p
             collisions at s**(1/2) = 1.96 TeV using the Collider
             Detector at Fermilab. Z bosons are identified in their
             electron and muon decay modes, and b jets with E(t) > 20 GeV
             and |eta| l+ l-) = 0.93 +/- 0.36 pb is found, where B(Z -->
             l+ l-) is the branching ratio of the Z boson or gamma* into
             a single flavor dilepton pair (e or mu) in the mass range
             between 66 and 116 GeV/c2. The ratio of b jets to the total
             number of jets of any flavor in the Z sample, within the
             same kinematic range as the b jets, is 2.36 +/- 0.92\%.
             Here, the uncertainties are the quadratic sum of statistical
             and systematic uncertainties. Predictions made with NLO QCD
             agree, within experimental and theoretical uncertainties,
             with these measurements.},
   Doi = {10.1103/PhysRevD.74.032008},
   Key = {fds309564}
}

@article{fds309566,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the t anti-t production cross section in
             $p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV in the all
             hadronic decay mode},
   Journal = {Phys. Rev.},
   Volume = {D74},
   Number = {7},
   Pages = {072005},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.74.072005},
   Abstract = {We report a measurement of the tt-bar production cross
             section using the CDF II detector at the Fermilab Tevatron.
             The analysis is performed using 322 pb-1 of p anti-p
             collisions at s**(1/2) = 1.96 TeV. The data consist of
             events selected with six or more hadronic jets with
             additional kinematic requirements. At least one of these
             jets must be identified as a b-quark jet by the
             reconstruction of a secondary vertex. The cross section is
             measured to be sigma_tt-bar = 7.5 +/- 2.1(stat.)+3.3_-2.2(syst.)+0.5_-0.4(lumi.)
             pb, which is consistent with the standard model
             prediction.},
   Doi = {10.1103/PhysRevD.74.072005},
   Key = {fds309566}
}

@article{fds309569,
   Author = {Oh, SH and al, AAE},
   Title = {Search for Z'-e+e- using dielectron mass and angular
             distriubution},
   Journal = {Phys. Rev.Lett},
   Volume = {96},
   Pages = {211802},
   Year = {2006},
   Key = {fds309569}
}

@article{fds309570,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the inclusive jet cross section using the
             k(t) algorithm in p anti-p collisions at $\sqrt{s}=$ 1.96-
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {12},
   Pages = {122001},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.122001},
   Abstract = {We report on a measurement of the inclusive jet production
             cross section in p anti-p collisions at s**(1/2) = 1.96 TeV
             using data collected with the upgraded Collider Detector at
             Fermilab in Run II (CDF II) corresponding to an integrated
             luminosity of 385 pb-1. Jets are reconstructed using the K_T
             algorithm. The measurement is carried out for jets with
             rapidity $0.1},
   Doi = {10.1103/physrevlett.96.122001},
   Key = {fds309570}
}

@article{fds309586,
   Author = {Abulencia, and A, and others},
   Title = {Search for second-generation scalar leptoquarks in
             $p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D73},
   Number = {5},
   Pages = {051102},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.051107},
   Abstract = {Results on a search for pair production of second generation
             scalar leptoquark in p anti-p collisions at s**(1/2) = 1.96
             TeV are reported. The data analyzed were collected by the
             CDF detector during the 2002-2003 Tevatron Run II and
             correspond to an integrated luminosity of 198 pb-1.
             Leptoquarks (LQ) are sought through their decay into
             (charged) leptons and quarks, with final state signatures
             represented by two muons and jets and one muon, large
             transverse missing energy and jets. We observe no evidence
             for LQ production and derive 95% C.L. upper limits on the LQ
             production cross sections as well as lower limits on their
             mass as a function of Beta, where Beta is the branching
             fraction for LQ --> mu q.},
   Doi = {10.1103/PhysRevD.72.051107},
   Key = {fds309586}
}

@article{fds310123,
   Author = {Abulencia, and A, and others},
   Title = {Search for $Z^\prime \to e^+ e^-$ using dielectron mass and
             angular distribution},
   Journal = {Phys. Rev. Lett.},
   Volume = {96},
   Number = {21},
   Pages = {211801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/physrevlett.96.211801},
   Abstract = {We report results from a search for Z' bosons in high-mass
             dielectron events produced in p anti-p collisions at
             s**(1/2) = 1.96 TeV. The data were recorded with the CDF II
             detector at the Fermilab Tevatron and correspond to an
             integrated luminosity of 0.45 fb-1. To identify the Z' -->
             e+ e- signal, both the dielectron invariant mass
             distribution and the angular distribution of the electron
             pair are used. No evidence for a signal is found, and 95\%
             confidence level lower limits are set on the Z' mass for
             several models.},
   Doi = {10.1103/physrevlett.96.211801},
   Key = {fds310123}
}

@article{fds348713,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copie, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
             J and Culbertson, R and Cully, JC and Cyr, D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Ceceo,
             SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and DiTuro,
             P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin,
             M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
             C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
             A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hare, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez,
             PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nahn, S and Nakano, and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
             E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Porteil, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
             N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
             I},
   Title = {Observation of B s0 - B̄
             s0 oscillations},
   Journal = {Physical Review Letters},
   Volume = {97},
   Number = {24},
   Pages = {242003},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.97.242003},
   Abstract = {We report the observation of B s0- B̄ s0 oscillations from
             a time-dependent measurement of the B s0-B̄ s0 oscillation
             frequency Δm s. Using a data sample of 1 fb -1 of pp
             collisions at √ = 1.96 TeV collected with the CDF II
             detector at the Fermilab Tevatron, we find signals of 5600
             fully reconstructed hadronic B s decays, 3100 partially
             reconstructed hadronic B s decays, and 61500 partially
             reconstructed semileptonic B s decays. We measure the
             probability as a function of proper decay time that the B s
             decays with the same, or opposite, flavor as the flavor at
             production, and we find a signal for B s0-B̄ s0
             oscillations. The probability that random fluctuations could
             produce a comparable signal is 8 × 10 -8, which exceeds 5σ
             significance. We measure Δm s = 17.77 ± 0.10(stat) ±
             0.07(syst) ps -1 and extract |V td/V ts| = 0.2060 ±
             0.0007(Δm s) -0.0060+0.0081 (Δm d + theor). © 2006 The
             American Physical Society.},
   Doi = {10.1103/PhysRevLett.97.242003},
   Key = {fds348713}
}

@article{fds344680,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
             T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
             N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
             S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon, M and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun,
             SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp,
             Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
             YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee,
             YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
             A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
             E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava,
             R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin,
             A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton, P and Rescigno, M and Richter, S and Rimondi,
             F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers,
             E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz,
             A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
             D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
             A and Sinervo, P and Sisakyan, A and Sjolin, J},
   Title = {Observation of Bs0→ψ(2S) and measurement of the ratio of
             branching fractions B(Bs0→ψ(2S) /B(Bs0→J/ψ)},
   Journal = {Physical Review Letters},
   Volume = {96},
   Number = {23},
   Pages = {231801},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.96.231801},
   Abstract = {We report the first observation of Bs0→ψ(2S) decay in
             pp̄ collisions at s= 1.96 TeV using 360 pb-1 of data
             collected by the CDF II detector at the Fermilab Tevatron.
             We observe 20.2±5.0 and 12.3±4.1 Bs0→ψ(2S) candidates,
             in ψ(2S)→μ+μ- and ψ(2S)→J/ψπ+π- decay modes,
             respectively. We present a measurement of the relative
             branching fraction B(Bs0→ψ(2S) /B(Bs0→J/ψ)=0.52±0.13(stat)±0.04(syst)±0.06(BR)
             using the ψ(2S)→μ+μ- decay mode. © 2006 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.96.231801},
   Key = {fds344680}
}

@article{fds362147,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
             PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and DiTuro, P and Dorr, C and Donati, S and Donega, M and Dong, P and Donini,
             J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini,
             P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos,
             G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra,
             Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis,
             E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann,
             B and Heinrich, J and Herndon, M and Hidas, D and Hill, CS and Hirschbuehl,
             D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi,
             G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
             T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
             H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
             A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mulmenstadt, J and Mukherjee, A and Muller, T and Mumford, R and Murat,
             P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg,
             K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
             V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel,
             NV and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
             S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
   Title = {Measurement of the Bc+ meson lifetime using the decay mode
             Bc+→J/ψe+νe},
   Journal = {Physical Review Letters},
   Volume = {97},
   Number = {1},
   Pages = {012002},
   Year = {2006},
   url = {http://dx.doi.org/10.1103/PhysRevLett.97.012002},
   Abstract = {We present a measurement of the Bc+ meson lifetime in the
             decay mode Bc+→J/ψe+νe using the Collider Detector at
             Fermilab II detector at the Fermilab Tevatron Collider. From
             a sample of about 360pb-1 of pp̄ collisions at s=1.96TeV,
             we reconstruct J/ψe+ pairs with invariant mass in the
             kinematically allowed range 4&lt;MJ/ψe&lt;6GeV/c2. A fit to
             the decay-length distribution of 238 signal events yields a
             measured Bc+ meson lifetime of 0.463+0.073-0.065(stat)±0.036(syst)ps.
             © 2006 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.97.012002},
   Key = {fds362147}
}

@article{fds309544,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
             A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and Daronco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, J and Dituro,
             P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciveres and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong,
             DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis,
             JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss,
             TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama,
             T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
             R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
             AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov,
             A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi,
             I},
   Title = {Search for neutral Higgs bosons of the minimal
             supersymmetric standard model decaying to tau pairs in pp
             collisions at square root of s = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {96},
   Number = {1},
   Pages = {011802},
   Year = {2006},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.96.011802},
   Abstract = {We present a search for neutral supersymmetric Higgs bosons
             decaying to tau pairs produced in pp collisions at square
             root of s = 1.96 TeV. The data, corresponding to 310 pb(-1)
             integrated luminosity, were collected with the Collider
             Detector at Fermilab in run II of the Tevatron. No
             significant excess above the standard model backgrounds is
             observed. We set exclusion limits on the production cross
             section times branching fraction to tau pairs for Higgs
             boson masses in the range from 90 to 250
             GeV/c2.},
   Doi = {10.1103/physrevlett.96.011802},
   Key = {fds309544}
}

@article{fds309567,
   Author = {Acosta, D and Affolder, T and Albrow, MG and Ambrose, D and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello,
             D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld,
             B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bromberg, C and Brozovic, M and Brubaker, E and Budagov,
             J and Budd, HS and Burkett, K and Busetto, G and Byrum, KL and Cabrera, S and Campbell, M and Carithers, W and Carlsmith, D and Castro, A and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Chu,
             ML and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Clark, AG and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cranshaw, J and Culbertson, R and Dagenhart, D and D'Auria, S and de
             Barbaro, P and de Cecco, S and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and de Pedis, D and Derwent,
             PF and Dionisi, C and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, T and Eddy, N and Erbacher, R and Errede,
             D},
   Title = {Search for W and Z bosons in the reaction p̄p→twojets+γ
             at s=1.8TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {73},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2006},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.73.012001},
   Abstract = {We present a study of the dijet invariant mass distribution
             for the reaction p̄p→twojets+γ+X, at a center of mass
             energy of 1.8 TeV, using data collected by the CDF
             experiment. We compare the data to predictions for the
             production of a photon with two jets, together with the
             resonant processes p̄p→W/Z+γ+X, in which the W and Z
             bosons decay hadronically. A fit is made to the dijet
             invariant mass distribution combining the nonresonant
             background and resonant processes. We use the result to
             establish a limit for the inclusive production cross section
             of W/Z+γ with hadronic decay of the W and Z bosons. © 2006
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.73.012001},
   Key = {fds309567}
}

@article{fds309540,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
             A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro,
             P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
             LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciverez and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and di
             Giovanni, GP and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
             C and Giokaris, N and Giolo, K and Giordani, M and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
             K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
             C and Grundler, U and Guimaraes da Costa and J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer,
             A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang,
             D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel,
             M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen,
             AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
             DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca,
             G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin,
             M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
             A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr,
             B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa,
             T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
             WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
             T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria,
             F},
   Title = {Search for Higgs bosons decaying to bb and produced in
             association with W bosons in pp collisions at square root of
             s = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {96},
   Number = {8},
   Pages = {081803},
   Year = {2006},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.96.081803},
   Abstract = {We present a search for Higgs bosons decaying into bb and
             produced in association with W bosons in pp collisions at
             square root of s = 1.96 TeV. This search uses 320 pb(-1) of
             the data set accumulated by the upgraded Collider Detector
             at Fermilab. Events are selected that have a high-transverse
             momentum electron or muon, missing transverse energy, and
             two jets, at least one of which is consistent with the
             hadronization of a b quark. Both the number of events and
             the dijet mass distribution are consistent with standard
             model background expectations, and we set 95% confidence
             level upper limits on the production cross section times
             branching ratio for the Higgs boson or any new particle with
             similar decay kinematics. These upper limits range from 10
             pb for mH = 110 GeV/c2 to 3 pb for mH = 150
             GeV/c2.},
   Doi = {10.1103/physrevlett.96.081803},
   Key = {fds309540}
}

@article{fds309548,
   Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
             A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
             J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
             J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
   Title = {A search for t → τ ν q in t over(t, ̄)
             production},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {639},
   Number = {3-4},
   Pages = {172-178},
   Publisher = {Elsevier BV},
   Year = {2006},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2006.06.030},
   Abstract = {We present a search for t over(t, ̄) events with a tau
             lepton in the final state. The data sample corresponds to an
             integrated luminosity of 194 pb-1 collected with the CDF II
             detector from p over(p, ̄) collisions at a center of mass
             energy of 1.96 TeV. We observe two events with an expected
             signal of 1.0 ± 0.2 events and a background of 1.3 ± 0.3
             events. We determine a 95% confidence level upper limit on
             rτ, the ratio of the measured rate of t → τ ν q to the
             expectation, of 5.2. © 2006 Elsevier B.V. All rights
             reserved.},
   Doi = {10.1016/j.physletb.2006.06.030},
   Key = {fds309548}
}

@article{fds309487,
   Author = {Aaltonen, T and others},
   Title = {Search for Chargino-Neutralino Production in $p\overline p$
             Collisions at $\sqrt{s}$=1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {19},
   Pages = {191806},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.191806},
   Abstract = {We present a search for associated production of the
             chargino and neutralino supersymmetric particles using up to
             1.1 fb-1 of integrated luminosity collected by the CDF II
             experiment at the Tevatron p[overline p] collider at
             sqrt(s)=1.96 TeV. We analyze events with a large transverse
             momentum imbalance and either three charged leptons or two
             charged leptons of the same electric charge. The numbers of
             observed events are consistent with standard model
             expectations. Upper limits on the production cross section
             are derived in different theoretical models.},
   Doi = {10.1103/physrevlett.99.191806},
   Key = {fds309487}
}

@article{fds309488,
   Author = {Abulencia, and A, and others},
   Title = {Precise measurement of the top quark mass in the lepton+jets
             topology at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {18},
   Pages = {182002},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.182002},
   Abstract = {We present a measurement of the mass of the top quark from
             proton-antiproton collisions recorded at the CDF experiment
             in Run II of the Fermilab Tevatron. We analyze events from
             the single lepton plus jets final state (t[overline
             t]-->W+bW-[overline b]-->lnubq[overline q][prime][overline
             b]). The top-quark mass is extracted using a direct
             calculation of the probability density that each event
             corresponds to the t[overline t] final state. The
             probability is a function of both the mass of the top quark
             and the energy scale of the calorimeter jets, which is
             constrained in situ by the hadronic W boson mass. Using 167
             events observed in 955 pb-1 of integrated luminosity, we
             achieve the single most precise measurement of the top-quark
             mass, 170.8$\pm$2.2(stat.)$\pm$1.4(syst.)
             GeV/c2.},
   Doi = {10.1103/physrevlett.99.182002},
   Key = {fds309488}
}

@article{fds309489,
   Author = {Aaltonen, and T, and others},
   Title = {Search for new physics in high mass electron-positron events
             in $p \bar{p}$ collisions at $\sqrt{s}$ =
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {17},
   Pages = {171802},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.171802},
   Abstract = {We report the results of a search for a narrow resonance in
             electron-positron events in the invariant mass range of
             150--950 GeV/c2 using 1.3 fb-1 of p[overline p] collision
             data at sqrt(s)=1.96 TeV collected by the CDF II detector at
             Fermilab. No significant evidence of such a resonance is
             observed and we interpret the results to exclude the
             standard-model-like Z[prime] with a mass below 923 GeV/c2
             and the Randall-Sundrum graviton with a mass below 807
             GeV/c2 for k/[overline M]pl=0.1, both at the 95\% confidence
             level. Combining with diphoton data excludes the
             Randall-Sundrum graviton for masses below 889 GeV/c2 for
             k/[overline M]pl=0.1.},
   Doi = {10.1103/physrevlett.99.171802},
   Key = {fds309489}
}

@article{fds309490,
   Author = {Aaltonen, and T, and others},
   Title = {Search for a high-mass diphoton state and limits on
             Randall-Sundrum gravitons at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {17},
   Pages = {171801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.171801},
   Abstract = {e have performed a search for new particles which decay to
             two photons using 1.2 fb-1 of integrated luminosity from
             p[overline p] collisions at sqrt(s)=1.96 TeV collected using
             the CDF II detector at the Fermilab Tevatron. We find the
             diphoton mass spectrum to be in agreement with the standard
             model expectation, and set limits on the cross section times
             branching ratio for the Randall-Sundrum graviton, as a
             function of diphoton mass. We subsequently derive lower
             limits for the graviton mass of 230 GeV/c2 and 850 GeV/c2,
             at the 95\% confidence level, for coupling parameters
             (k/[overline M]Pl) of 0.01 and 0.1, respectively.},
   Doi = {10.1103/physrevlett.99.171801},
   Key = {fds309490}
}

@article{fds309491,
   Author = {Aaltonen, and T, and others},
   Title = {First Measurement of the W Boson Mass in Run II of the
             Tevatron},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {15},
   Pages = {151801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.151801},
   Abstract = {We present a measurement of the W-boson mass using 200 pb-1
             of data collected in p[overline p] collisions at
             sqrt(s)=1.96 TeV by the CDF II detector at run II of the
             Fermilab Tevatron. With a sample of 63 964 W-->enu
             candidates and 51 128 W-->µnu candidates, we measure MW=80
             413$\pm$34stat$\pm$34syst=80 413$\pm$48 MeV/c2. This is the
             most precise single measurement of the W-boson mass to
             date.},
   Doi = {10.1103/physrevlett.99.151801},
   Key = {fds309491}
}

@article{fds309492,
   Author = {Abulencia, and A, and others},
   Title = {Search for heavy, long-lived particles that decay to photons
             at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {12},
   Pages = {121801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.121801},
   Abstract = {We present the first search for heavy, long-lived particles
             that decay to photons at a hadron collider. We use a sample
             of gamma+jet+missing transverse energy events in p[overline
             p] collisions at sqrt(s)=1.96 TeV taken with the CDF II
             detector. Candidate events are selected based on the arrival
             time of the photon at the detector. Using an integrated
             luminosity of 570 pb-1 of collision data, we observe 2
             events, consistent with the background estimate of
             1.3$\pm$0.7 events. While our search strategy does not rely
             on model-specific dynamics, we set cross section limits in a
             supersymmetric model with chi-tilde10-->gammaG-tilde and
             place the world-best 95\% C.L. lower limit on the
             chi-tilde10 mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup
             0]=5 ns.},
   Doi = {10.1103/physrevlett.99.121801},
   Key = {fds309492}
}

@article{fds309493,
   Author = {Aaltonen, and T, and others},
   Title = {Observation and mass measurement of the baryon
             $Xi_b^-$},
   Journal = {Phys. Rev. Lett.},
   Volume = {99},
   Number = {5},
   Pages = {052002},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.99.052002},
   Abstract = {We report the observation and measurement of the mass of the
             bottom, strange baryon Xib- through the decay chain
             Xib--->J/psiXi-, where J/psi-->µ+µ-, Xi--->Lambdapi-, and
             Lambda-->ppi-. A signal is observed whose probability of
             arising from a background fluctuation is 6.6{\AA}~10-15, or
             7.7 Gaussian standard deviations. The Xib- mass is measured
             to be 5792.9$\pm$2.5(stat) $\pm$1.7(syst)
             MeV/c2.},
   Doi = {10.1103/physrevlett.99.052002},
   Key = {fds309493}
}

@article{fds309494,
   Author = {Abulencia, and A, and others},
   Title = {First Measurement of the Ratio of Central-Electron to
             Forward-Electron W Partial Cross Sections in p-pbar
             Collisions at sqrt{s} = 1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {25},
   Pages = {251801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.251801},
   Abstract = {We present a measurement of sigma(p[overline
             p]-->W){\AA}~[script B](W-->enu) at sqrt(s)=1.96 TeV, using
             electrons identified in the forward region
             (1.2-90+95(syst)$\pm$162(lum) pb. Combining this result with
             a previous CDF measurement obtained using electrons in the
             central region (|eta|},
   Doi = {10.1103/physrevlett.98.251801},
   Key = {fds309494}
}

@article{fds309495,
   Author = {Abulencia, and A, and others},
   Title = {Inclusive search for new physics with like-sign dilepton
             events in $p \bar{p}$ collisions at $\sqrt{s}$ =
             1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {22},
   Pages = {221803},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.221803},
   Abstract = {We describe a search for anomalous production of events with
             two leptons (e or µ) of the same electric charge in
             p[overline p] collisions at a center-of-mass energy of 1.96
             TeV. Many extensions to the standard model predict the
             production of two leptons of the same electric charge. This
             search has a significant increase in sensitivity compared to
             earlier searches. Using a data sample corresponding to 1
             fb-1 of integrated luminosity recorded by the CDF II
             detector, we observe no significant excess in an inclusive
             selection (expect 33.2$\pm$4.7 events, observe 44) or in a
             supersymmetry-optimized selection (expect 7.8$\pm$1.1
             events, observe 13.)},
   Doi = {10.1103/physrevlett.98.221803},
   Key = {fds309495}
}

@article{fds309496,
   Author = {Abulencia, and A, and others},
   Title = {Observation of $WZ$ Production},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {16},
   Pages = {161801},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.161801},
   Abstract = {We report the first observation of the associated production
             of a W boson and a Z boson. This result is based on 1.1 fb-1
             of integrated luminosity from p[overline p] collisions at
             sqrt(s)=1.96 TeV collected with the CDF II detector at the
             Fermilab Tevatron. We observe 16 WZ candidates passing our
             event selection with an expected background of 2.7$\pm$0.4
             events. A fit to the missing transverse energy distribution
             indicates an excess of events compared to the background
             expectation corresponding to a significance equivalent to 6
             standard deviations. The measured cross section is
             sigma(p[overline p]-->WZ)=5.0-1.6+1.8 pb, consistent with
             the standard model expectation.},
   Doi = {10.1103/physrevlett.98.161801},
   Key = {fds309496}
}

@article{fds309497,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the top-quark mass in all-hadronic decays in
             p anti-p collisions at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {14},
   Pages = {142001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.142001},
   Abstract = {We present a measurement of the top-quark mass Mtop in the
             all-hadronic decay channel t[overline t]-->W+bW-[overline
             b]-->q1[overline q]2bq3[overline q]4[overline b]. The
             analysis is performed using 310 pb-1 of sqrt(s)=1.96 TeV
             p[overline p] collisions collected with the CDF II detector
             using a multijet trigger. The mass measurement is based on
             an event-by-event likelihood which depends on both the
             sample purity and the value of the top-quark mass, using 90
             possible jet-to-parton assignments in the six-jet final
             state. The joint likelihood of 290 selected events yields a
             value of Mtop=177.1$\pm$4.9(stat)$\pm$4.7(syst)
             GeV/c2.},
   Doi = {10.1103/physrevlett.98.142001},
   Key = {fds309497}
}

@article{fds309499,
   Author = {Abulencia, and A, and others},
   Title = {Analysis of the quantum numbers J(PC) of the
             X(3872)},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {13},
   Pages = {132002},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.132002},
   Abstract = {We present an analysis of angular distributions and
             correlations of the X(3872) particle in the exclusive decay
             mode X(3872)-->J/psipi+pi- with J/psi-->µ+µ-. We use 780
             pb-1 of data from p[overline p] collisions at sqrt(s)=1.96
             TeV collected with the CDF II detector at the Fermilab
             Tevatron. We derive constraints on spin, parity, and charge
             conjugation parity of the X(3872) particle by comparing
             measured angular distributions of the decay products with
             predictions for different JPC hypotheses. The assignments
             JPC=1++ and 2-+ are the only ones consistent with the
             data.},
   Doi = {10.1103/physrevlett.98.132002},
   Key = {fds309499}
}

@article{fds309500,
   Author = {Abulencia, and A, and others},
   Title = {Observation of exclusive electron positron production in
             hadron hadron collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {11},
   Pages = {112001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.112001},
   Abstract = {We present the first observation of exclusive e+e-
             production in hadron-hadron collisions, using p[overline p]
             collision data at sqrt(s)=1.96 TeV taken by the run II
             Collider Detector at Fermilab, and corresponding to an
             integrated luminosity of 532 pb-1. We require the absence of
             any particle signatures in the detector except for an
             electron and a positron candidate, each with transverse
             energy ET>5 GeV and pseudorapidity |eta|p+e+e-+[overline p]
             through two-photon exchange. The measured cross section is
             1.6-0.3+0.5(stat)$\pm$0.3(syst) pb. This agrees with the
             theoretical prediction of 1.71$\pm$0.01 pb.},
   Doi = {10.1103/physrevlett.98.112001},
   Key = {fds309500}
}

@article{fds309501,
   Author = {Abulencia, and A, and others},
   Title = {Search for V + A current in top quark decay in p anti-p
             collisions at s**(1/2) = 1.96-TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {7},
   Pages = {072001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/physrevlett.98.072001},
   Abstract = {We report an upper limit on the fraction of V+A current,
             fV+A, in top-quark decays, using approximately 700 pb-1 of
             p[overline p] collisions at sqrt(s)=1.96 TeV acquired by the
             upgraded Collider Detector at Fermilab. For the decay
             t-->Wb-->[script-l]nub (where [script-l]=e or µ), the
             invariant mass of the charged lepton and the bottom quark
             jet is sensitive to the polarization of the W boson. We
             determine fV+A=-0.06$\pm$0.25 given a top-quark mass of 175
             GeV/c2. We set an upper limit on fV+A of 0.29 at the 95\%
             confidence level, an improvement by a factor of 2 on the
             previous best direct limit.},
   Doi = {10.1103/physrevlett.98.072001},
   Key = {fds309501}
}

@article{fds309502,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the top-quark mass using missing $E_T$ + jets
             events with secondary vertex $b-$tagging at CDF
             II},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {11},
   Pages = {111103},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.111103},
   Abstract = {We present a measurement of the top-quark mass in p[overline
             p] collisions at sqrt(s)=1.96 TeV which uses events with an
             inclusive signature of missing transverse energy and jets.
             The event selection is sensitive to t[overline
             t]-->W+bW-[overline b]-->lnubqq[prime][overline b]
             independent of the lepton flavor and results in a large
             acceptance for W-->taunu decays. All-hadronic t[overline t]
             decays and events with identified electrons or muons are
             vetoed to provide a statistically independent sample with
             respect to all previous measurements. The top-quark mass is
             inferred from the distribution of the scalar sum of all jet
             transverse energies and the missing transverse energy. Using
             311 pb-1 of integrated luminosity recorded by the Collider
             Detector at Fermilab, we measure a top-quark mass
             mt=172.3-9.6+10.8(stat)$\pm$10.8(syst) GeV/c2. While the
             uncertainty on mt is larger than that of other measurements,
             the result is statistically uncorrelated with those of other
             methods and thus can help to reduce the overall mt
             uncertainty when combined with other existing
             measurements.},
   Doi = {10.1103/PhysRevD.75.111103},
   Key = {fds309502}
}

@article{fds309504,
   Author = {Aaltonen, T and others},
   Title = {Searches for direct pair production of supersymmetric top
             and supersymmetric bottom quarks in p[overline p] collisions
             at $\sqrt{s}$=1.96 TeV},
   Journal = {Phys. Rev.},
   Volume = {D76},
   Number = {7},
   Pages = {072010},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.072010},
   Abstract = {We search for direct pair production of supersymmetric top
             quarks and supersymmetric bottom quarks in proton-antiproton
             collisions at sqrt(s)=1.96 TeV, using 295 pb-1 of data
             recorded by the Collider Detector at Fermilab (CDF II)
             experiment. The supersymmetric top (supersymmetric bottom)
             quarks are selected by reconstructing their decay into a
             charm (bottom) quark and a neutralino, which is assumed to
             be the lightest supersymmetric particle. The signature of
             such processes is two energetic heavy-flavor jets and
             missing transverse energy. The number of events that pass
             our selection for each search process is consistent with the
             expected standard model background. By comparing our results
             to the theoretical production cross sections of the
             supersymmetric top and supersymmetric bottom quarks in the
             minimal supersymmetric standard model, we exclude, at a 95%
             confidence level in the frame of that model, a
             supersymmetric top quark mass up to 132 GeV/c2 for a
             neutralino mass of 48 GeV/c2, and a supersymmetric bottom
             quark mass up to 193 GeV/c2 for a neutralino mass of 40
             GeV/c2.},
   Doi = {10.1103/PhysRevD.76.072010},
   Key = {fds309504}
}

@article{fds309506,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Particles Leading to $Z +$ jets Final States
             in $p \bar{p}$ Collisions at $\sqrt{s}$ =
             1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D76},
   Number = {7},
   Pages = {072006},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.072006},
   Abstract = {We present the results of a search for new particles that
             lead to a Z boson plus jets in p[overline p] collisions at
             sqrt(s)=1.96 TeV using the Collider Detector at Fermilab
             (CDF II). A data sample with a luminosity of 1.06 fb-1
             collected using Z boson decays to ee and µµ is used. We
             describe a completely data-based method to predict the
             dominant background from standard model Z+jet events. This
             method can be similarly applied to other analyses requiring
             background predictions in multijet environments, as shown
             when validating the method by predicting the background from
             W+jets in t[overline t] production. No significant excess
             above the background prediction is observed, and a limit is
             set using a fourth generation quark model to quantify the
             acceptance. Assuming BR(b[prime]-->bZ)=100\% and using a
             leading-order calculation of the b[prime] cross section,
             b[prime] quark masses below 268 GeV/c2 are excluded at 95%
             confidence level.},
   Doi = {10.1103/PhysRevD.76.072006},
   Key = {fds309506}
}

@article{fds309507,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $p \bar{p} \to t \bar{t}$ production
             cross- section and the top quark mass at $\sqrt{s}$ = 1.96-
             TeV in the all-hadronic decay mode},
   Journal = {Phys. Rev.},
   Volume = {D76},
   Number = {7},
   Pages = {072009},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.072009},
   Abstract = {We report the measurements of the t[overline t] production
             cross section and of the top quark mass using 1.02 fb-1 of
             p[overline p] data collected with the CDF II detector at the
             Fermilab Tevatron. We select events with six or more jets on
             which a number of kinematical requirements are imposed by
             means of a neural network algorithm. At least one of these
             jets must be identified as initiated by a b-quark candidate
             by the reconstruction of a secondary vertex. The cross
             section is measured to be sigmat[overline
             t]=8.3$\pm$1.0(stat)-1.5+2.0(syst)$\pm$0.5(lumi) pb, which
             is consistent with the standard model prediction. The top
             quark mass of 174.0$\pm$2.2(stat)$\pm$4.8(syst) GeV/c2 is
             derived from a likelihood fit incorporating reconstructed
             mass distributions representative of signal and
             background.},
   Doi = {10.1103/PhysRevD.76.072009},
   Key = {fds309507}
}

@article{fds309508,
   Author = {Abulencia, A and others},
   Title = {Measurements of Inclusive W and Z Cross Sections in p anti-p
             Collisions at $\sqrt{s} = 1.96$ TeV},
   Journal = {J. Phys. G: Nucl. Part. Phys.},
   Volume = {34},
   Number = {12},
   Pages = {2457-2544},
   Publisher = {IOP Publishing},
   Year = {2007},
   url = {http://dx.doi.org/10.1088/0954-3899/34/12/001},
   Abstract = {We report the first measurements of inclusive W and Z boson
             cross-sections times the corresponding leptonic branching
             ratios for p anti-p collisions at s**(1/2) = 1.96 TeV based
             on the decays of the W and Z bosons into electrons and
             muons. The data were recorded with the CDF II detector at
             the Fermilab Tevatron and correspond to an integrated
             luminosity of 72.0 +/- 4.3 pb-1. We test e-mu lepton
             universality in W decays by measuring the ratio of the W -->
             mu nu to W --> e nu cross sections and determine a value to
             0.991 +/- 0.004(stat.) +/- 0.011(syst.) for the ratio of W -
             l - nu couplings (g_mu/g_e). Since there is no sign of
             non-universality, we combine our cross-section measurements
             in the different lepton decay modes and obtain sigma_W x
             Br(p anti-p --> W --> l nu) = 2.749 +/- 0.010(stat.) +/-
             0.053(syst.) +/- 0.165(lum.) nb and sigma_gamma*/Z x BR(p
             anti-p --> gamma*/Z --> ll) = 254.9 +/- 3.3(stat.) +/-
             4.6(syst.) +/- 15.2(lum.) pb for dilepton pairs in the mass
             range between 66 GeV/c2 and 116 GeV/c2. We compute the ratio
             R of the W --> l nu to Z --> ll cross section taking all
             correlations among channels into account and obtain R =
             10.84 +/- 0.15(stat.) +/- 0.14(syst.) including a correction
             for the virtual photon exchange component in our measured
             gamma*/Z --> ll cross section. Based on the measured value
             of R, we extract values for the W leptonic branching ratio,
             Br(W --> l nu) = 0.1082 +/- 0.0022; the total width of the W
             boson, Gamma(W) = 2092 +/- 42 MeV; and the ratio of W and Z
             boson total widths, Gamma(W)/Gamma(Z) = 0.838 +/- 0.017. In
             addition, we use our extracted value of Gamma(W) whose value
             depends on various electroweak parameters and certain CKM
             matrix elements to constrain the V_cs CKM matrix element,
             |V_cs| = 0.976 +/- 0.030.},
   Doi = {10.1088/0954-3899/34/12/001},
   Key = {fds309508}
}

@article{fds309509,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the Top Quark Mass in $p\bar{p}$Collisions at
             $\sqrt{s} = 1.96$ TeV using the Decay Length
             Technique},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {7},
   Pages = {071102},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.071102},
   Abstract = {We report the first measurement of the top quark mass using
             the decay length technique in p[overline p] collisions at a
             center-of-mass energy of 1.96 TeV. This technique uses the
             measured flight distance of the b hadron to infer the mass
             of the top quark in lepton plus jets events with missing
             transverse energy. It relies solely on tracking and avoids
             the jet energy scale uncertainty that is common to all other
             methods used so far. We apply our novel method to a 695 pb-1
             data sample recorded by the CDF II detector at Fermilab and
             extract a measurement of mt=180.7-13.4+15.5(stat.)$\pm$8.6(syst.)
             GeV/c2. While the uncertainty of this result is larger than
             that of other measurements, the dominant uncertainties in
             the decay length technique are uncorrelated with those in
             other methods. This result can help reduce the overall
             uncertainty when combined with other existing measurements
             of the top quark mass.},
   Doi = {10.1103/PhysRevD.75.071102},
   Key = {fds309509}
}

@article{fds309510,
   Author = {Abulencia, and A, and others},
   Title = {Search for Exotic $S=-2$ Baryons in $p\bar{p}$ Collisions at
             $\sqrt{s}=1.96\,TeV$},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.032003},
   Abstract = {A search for a manifestly exotic S=-2 baryon state decaying
             to Xi-pi-, and its neutral partner decaying to Xi-pi+, has
             been performed using 220 pb-1 of p[overline p] collisions at
             sqrt(s)=1.96 TeV collected by the Collider Detector at
             Fermilab. The Xi- trajectories were measured in a silicon
             tracker before their decay, resulting in a sample with low
             background and excellent position resolution. No evidence
             was found for S=-2 pentaquark candidates in the invariant
             mass range of 1600--2100 MeV/c2. Upper limits on the product
             of pentaquark production cross section times its branching
             fraction to Xi-pi+,-, relative to the cross section of the
             well-established Xi(1530) resonance, are presented for
             neutral and doubly negative candidates with pT>2 GeV/c and
             |y|},
   Doi = {10.1103/PhysRevD.75.032003},
   Key = {fds309510}
}

@article{fds309511,
   Author = {Abulencia, and A, and others},
   Title = {Precision measurement of the top quark mass from dilepton
             events at CDF II},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {3},
   Pages = {031105},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.031105},
   Abstract = {We report a measurement of the top-quark mass, Mt, in the
             dilepton decay channel of t[overline t]-->b[script-l][prime]+nu[script-l][prime][overline
             b][script-l]-[overline nu ][script-l] using an integrated
             luminosity of 1.0 fb-1 of p[overline p] collisions collected
             with the CDF II detector. We apply a method that convolutes
             a leading-order matrix element with detector resolution
             functions to form event-by-event likelihoods; we have
             enhanced the leading-order description to describe the
             effects of initial-state radiation. The joint likelihood is
             the product of the likelihoods from 78 candidate events in
             this sample, which yields a measurement of
             Mt=164.5$\pm$3.9(stat.)$\pm$3.9(syst.) GeV/c2, the most
             precise measurement of Mt in the dilepton
             channel.},
   Doi = {10.1103/PhysRevD.75.031105},
   Key = {fds309511}
}

@article{fds309516,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the Helicity Fractions of W Bosons from Top
             Quark Decays using Fully Reconstructed \boldmath${t\bar{t}}$
             Events with CDF II},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {5},
   Pages = {052001},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.052001},
   Abstract = {We present a measurement of the fractions F0 and F+ of
             longitudinally polarized and right-handed W bosons in
             top-quark decays using data collected with the CDF II
             detector. The data set used in the analysis corresponds to
             an integrated luminosity of approximately 318 pb-1. We
             select t[overline t] candidate events with one lepton, at
             least four jets, and missing transverse energy. Our helicity
             measurement uses the decay angle theta*, which is defined as
             the angle between the momentum of the charged lepton in the
             W boson rest frame and the W momentum in the top-quark rest
             frame. The costheta* distribution in the data is determined
             by full kinematic reconstruction of the t[overline t]
             candidates. We find F0=0.85-0.22+0.15(stat)$\pm$0.06(syst)
             and F+=0.05-0.05+0.11(stat)$\pm$0.03(syst), which is
             consistent with the standard model prediction. We set an
             upper limit on the fraction of right-handed W bosons of
             F+},
   Doi = {10.1103/PhysRevD.75.052001},
   Key = {fds309516}
}

@article{fds309517,
   Author = {Abulencia, and A, and others},
   Title = {Search for W' boson decaying to electron-neutrino pairs in p
             anti-p collisions at s**(1/2) = 1.96-TeV},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {9},
   Pages = {091101},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.091101},
   Abstract = {We present the results of a search for W[prime] boson
             decaying to electron-neutrino pairs in p[overline p]
             collisions at a center-of-mass energy of 1.96 TeV, using a
             data sample corresponding to 205 pb-1 of integrated
             luminosity collected by the CDF II detector at Fermilab. We
             observe no evidence for this decay mode and set limits on
             the production cross section times branching fraction,
             assuming the neutrinos from W[prime] boson decays to be
             light. If we assume the manifest left-right symmetric model,
             we exclude a W[prime] boson with mass less than 788 GeV/c2
             at the 95\% confidence level.},
   Doi = {10.1103/PhysRevD.75.091101},
   Key = {fds309517}
}

@article{fds309518,
   Author = {Abulencia, and A, and others},
   Title = {Measurement of the B+ production cross section in p anti-p
             collisions at s**(1/2) = 1960-GeV},
   Journal = {Phys. Rev.},
   Volume = {D75},
   Number = {5},
   Pages = {012010},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052001},
   Abstract = {We present a new measurement of the B+ meson differential
             cross section dsigma/dpT at sqrt(s)=1960 GeV. The data
             correspond to an integrated luminosity of 739 pb-1 collected
             with the upgraded CDF detector (CDF II) at the Fermilab
             Tevatron collider. B+ candidates are reconstructed through
             the decay B+-->J/psiK+, with J/psi-->µ+µ-. The integrated
             cross section for producing B+ mesons with pT>=6 GeV/c and
             |y|},
   Doi = {10.1103/PhysRevD.93.052001},
   Key = {fds309518}
}

@article{fds309520,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart,
             D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
             BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher,
             R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster,
             GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
             C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
             A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
             M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
             J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J and Slaughter,
             AJ},
   Title = {Measurement of the ratios of branching fractions B(Bs0→Ds-
             π+π+π-)/B(B0→D-π+π+π-) and B(Bs0→Ds-π+)/
             B(B0→D-π+)},
   Journal = {Physical Review Letters},
   Volume = {98},
   Number = {6},
   Pages = {061802},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.98.061802},
   Abstract = {Using 355pb-1 of data collected by the CDF II detector in
             pp̄ collisions at s=1.96TeV at the Fermilab Tevatron, we
             study the fully reconstructed hadronic decays
             B(s)0→D(s)-π+ and B(s)0→D(s)- π+π+π-. We present the
             first measurement of the ratio of branching fractions
             B(Bs0→Ds-π+π+π-)/B(B0→D-π+π+π-)=1.
             05±0.10(stat)±0.22(syst). We also update our measurement
             of B(Bs0→Ds-π+)/B(B0→D-π+) to 1.13±0.08(stat)±0.
             23(syst), improving the statistical uncertainty by more than
             a factor of 2. We find B(Bs0→Ds-π+)=[3.8±0.3(stat)±1.3(syst)]×10-3
             and B(Bs0→Ds-π+π+π-)=[8.4±0.8(stat)±3.2(syst)]
             ×10-3. © 2007 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.98.061802},
   Key = {fds309520}
}

@article{fds309523,
   Author = {S. Oh and Oh, SH},
   Title = {Search for Exotic S = -2 Baryons in p anti-p Collisions at
             sqrt(s) = 1.96 TeV},
   Journal = {Phys. Rev. D},
   Volume = {75},
   Number = {03},
   Pages = {2003},
   Year = {2007},
   Key = {fds309523}
}

@article{fds309524,
   Author = {S. Oh and Oh, SH},
   Title = {Search for Anomalous Production of Multilepton Events in p
             anti-p Collisions at sqrt(s) = 1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {98},
   Number = {13},
   Pages = {1804},
   Publisher = {Springer Nature},
   Year = {2007},
   url = {http://dx.doi.org/10.1007/JHEP06(2012)169},
   Abstract = {We report a search for the anomalous production of events
             with multiple charged leptons in p[overline p] collisions at
             sqrt(s)=1.96 TeV using a data sample corresponding to an
             integrated luminosity of 346 pb-1 collected by the CDF II
             detector at the Fermilab Tevatron. The search is divided
             into three-lepton and four-or-more-lepton data samples. We
             observe six events in the three-lepton sample and zero
             events in the >=4-lepton sample. Both numbers of events are
             consistent with standard model background expectations.
             Within the framework of an R-parity-violating supergravity
             model, the results are interpreted as mass limits on the
             lightest neutralino (chi-tilde10) and chargino
             (chi-tilde1[plus-minus]) particles. For one particular
             choice of model parameters, the limits are
             M(chi-tilde10)>110 GeV/c2 and M(chi-tilde1[plus-minus])>203
             GeV/c2 at 95\% confidence level; the variation of these mass
             limits with model parameters is presented.},
   Doi = {10.1007/JHEP06(2012)169},
   Key = {fds309524}
}

@article{fds344677,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
             JC and Cyr, D and Daronco, S and Datta, M and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
             A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
             S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
             C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
             SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
             J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
             P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
   Title = {Measurement of σχc2B(χc2→J/ψγ)/ σχc1B(χc1→J/ψγ)
             in pp̄ Collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {98},
   Number = {23},
   Pages = {232001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.98.232001},
   Abstract = {We measure the ratio of cross section times branching
             fraction, Rp=σχc2B(χc2→J/ψγ)/σχc1B(χc1→J/ ψγ),
             in 1.1fb-1 of pp̄ collisions at s=1.96TeV. This measurement
             covers the kinematic range pT(J/ψ)&gt;4.0GeV/c,
             η(J/ψ)&lt;1.0, and pT(γ)&gt;1.0GeV/c. For events due to
             prompt processes, we find Rp=0.395±0.016(stat)±0.015(syst).
             This result represents a significant improvement in
             precision over previous measurements of prompt χc1,2 hadro
             production. © 2007 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.98.232001},
   Key = {fds344677}
}

@article{fds344678,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
             J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria,
             S and Davies, T and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
             A and Lentdecker, GD and Lorenzo, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Dörr, C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
             D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg,
             C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
             U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
             T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy,
             L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
             PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A},
   Title = {Polarizations of J/ψ and ψ(2S) mesons produced in pp̄
             collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {99},
   Number = {13},
   Pages = {132001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.99.132001},
   Abstract = {We have measured the polarizations of J/ψ and ψ(2S) mesons
             as functions of their transverse momentum pT when they are
             produced promptly in the rapidity range |y|&lt;0.6 with pT
             5GeV/c. The analysis is performed using a data sample with
             an integrated luminosity of about 800pb-1 collected by the
             CDF II detector. For both vector mesons, we find that the
             polarizations become increasingly longitudinal as pT
             increases from 5 to 30GeV/c. These results are compared to
             the predictions of nonrelativistic quantum chromodynamics
             and other contemporary models. The effective polarizations
             of J/ψ and ψ(2S) mesons from B-hadron decays are also
             reported. © 2007 The American Physical Society.},
   Doi = {10.1103/PhysRevLett.99.132001},
   Key = {fds344678}
}

@article{fds344679,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
             JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng,
             J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
             S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
             I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
             C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute,
             M and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Labarga, L and Lai, S and Lami, S and Lammel,
             S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
             J and Nagano, A and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos, F and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic,
             V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
             A},
   Title = {Measurement of the Λb0 Lifetime in Λb0→J/ψΛ0 in pp̄
             Collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {98},
   Number = {12},
   Pages = {122001},
   Year = {2007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.98.122001},
   Abstract = {We report a measurement of the Λb0 lifetime in the
             exclusive decay Λb0→J/ψΛ0 in pp̄ collisions at
             s=1.96TeV using an integrated luminosity of 1.0fb-1 of data
             collected by the CDF II detector at the Fermilab Tevatron.
             Using fully reconstructed decays, we measure
             τ(Λb0)=1.593-0.078+0.083(stat)±0.033(syst)ps. This is the
             single most precise measurement of τ(Λb0) and is 3.2σ
             higher than the current world average. © 2007 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.98.122001},
   Key = {fds344679}
}

@article{fds309519,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
             A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
             A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Cyr,
             D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De
             Lentdecker, G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni,
             GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and DiTuro, P and Dörr,
             C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
             D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell,
             JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
             A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
             S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Le, Y and LeCompte, T and Lee, J and Lee,
             YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
             A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
             M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla
             Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
             E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
             N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J},
   Title = {Measurement of sigma Lambda b0/sigma B0 x B(Lambda
             b0-->Lambda c+pi-)/B(B0-->D+pi-) in pp collisions at square
             root s=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {98},
   Number = {12},
   Pages = {122002},
   Year = {2007},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.98.122002},
   Abstract = {We present the first observation of the baryon decay Lambda
             b0-->Lambda c+pi- followed by Lambda c+-->pK-pi+ in 106 pb-1
             pp collisions at square root s=1.96 TeV in the CDF
             experiment. In order to reduce systematic error, the
             measured rate for Lambda b0 decay is normalized to the
             kinematically similar meson decay B0-->D+pi- followed by
             D+-->pi+K-pi+. We report the ratio of production cross
             sections (sigma) times the ratio of branching fractions (B)
             for the momentum region integrated above pT>6 GeV/c and
             pseudorapidity range |eta|<1.3: sigma(pp-->Lambda
             b0X)/sigma(pp-->B0X)xB(Lambda b0-->Lambda
             c+pi-)/B(B0-->D+pi-)=0.82+/-0.08(stat)+/-0.11(syst)+/-0.22[B(Lambda
             c+-->pK-pi+)].},
   Doi = {10.1103/physrevlett.98.122002},
   Key = {fds309519}
}

@article{fds309512,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Measurement of σ(pp̄→Z)•B(Z→ττ) in pp̄ collisions
             at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {75},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.092004},
   Abstract = {We present a measurement of the inclusive production cross
             section for Z bosons decaying to tau leptons in pp̄
             collisions at s=1.96TeV. We use a channel with one
             hadronically-decaying and one electronically-decaying tau.
             This measurement is based on 350pb-1 of CDF Run II data.
             Using a sample of 504 opposite sign eτ events with a total
             expected background of 190 events, we obtain
             σ(pp̄→4Z)•B(Z→ττ)=264±23(stat)
             ±14(syst)±15(lumi)pb, in agreement with the
             next-to-next-to- leading order QCD prediction. This is the
             first CDF cross section measurement using
             hadronically-decaying taus in Run II. © 2007 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.75.092004},
   Key = {fds309512}
}

@article{fds309515,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Erratum: Measurement of the inclusive jet cross section
             using the kT algorithm in pp̄ collisions at s=1.96TeV with
             the CDF II detector (Physical Review D - Particles, Fields,
             Gravitation and Cosmology (2007) 75, (092006))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {75},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.119901},
   Doi = {10.1103/PhysRevD.75.119901},
   Key = {fds309515}
}

@article{fds309514,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Measurement of the inclusive jet cross section using the kT
             algorithm in pp̄ collisions at s=1.96TeV with the CDF II
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {75},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.75.092006},
   Abstract = {We report on measurements of the inclusive jet production
             cross section as a function of the jet transverse momentum
             in pp̄ collisions at s=1.96TeV, using the kT algorithm and
             a data sample corresponding to 1.0fb-1 collected with the
             Collider Detector at Fermilab in run II. The measurements
             are carried out in five different jet rapidity regions with
             |yjet|<2.1 and transverse momentum in the range
             54<pTjet<700GeV/c. Next-to-leading order perturbative QCD
             predictions are in good agreement with the measured cross
             sections. © 2007 The American Physical Society.},
   Doi = {10.1103/PhysRevD.75.092006},
   Key = {fds309514}
}

@article{fds309505,
   Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
             K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and DaRonco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
             Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
             C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
             M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
             C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
             D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
             U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
             R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
             J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
             G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
             R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
             A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
             A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
             S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
             M and Shochet, M and Shon, Y},
   Title = {Observation of the Heavy Baryons Sigma b and Sigma
             b*.},
   Journal = {Physical review letters},
   Volume = {99},
   Number = {20},
   Pages = {202001},
   Year = {2007},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.99.202001},
   Abstract = {We report an observation of new bottom baryons produced in
             pp collisions at the Tevatron. Using 1.1 fb(-1) of data
             collected by the CDF II detector, we observe four Lambda b 0
             pi+/- resonances in the fully reconstructed decay mode
             Lambda b 0-->Lambda c + pi-, where Lambda c+-->pK* pi+. We
             interpret these states as the Sigma b(*)+/- baryons and
             measure the following masses: m Sigma b+=5807.8 -2.2
             +2.0(stat.)+/-1.7(syst.) MeV/c2, m Sigma b-
             =5815.2+/-1.0(stat.)+/-1.7(syst.) MeV/c2, and m(Sigma
             b*)-m(Sigma b)=21.2-1.9 +2.0(stat.)-0.3+0.4(syst.)
             MeV/c2.},
   Doi = {10.1103/physrevlett.99.202001},
   Key = {fds309505}
}

@article{fds309486,
   Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
             K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carrillo, S and Carlsmith, D and Caron, B and Carosi, R and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
             Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
             C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
             J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
             M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
             M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
             C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
             D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
             U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
             J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
             R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
             R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
             P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
             J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
             G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
             R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee,
             A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
             R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
             A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
             S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
             A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
             M},
   Title = {Search for exclusive gammagamma production in Hadron-Hadron
             collisions.},
   Journal = {Physical review letters},
   Volume = {99},
   Number = {24},
   Pages = {242002},
   Year = {2007},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.99.242002},
   Abstract = {We have searched for exclusive gammagamma production in
             proton-antiproton collisions at sqrt[s]=1.96 TeV, using 532
             pb(-1) of integrated luminosity taken by the run II Collider
             Detector at Fermilab. The event signature requires two
             electromagnetic showers, each with transverse energy E(T)>5
             GeV and pseudorapidity |eta|<1.0, with no other particles
             detected in the event. Three candidate events are observed.
             We discuss the consistency of the three events with
             gammagamma, pi(0)pi(0), or eta eta production. The
             probability that other processes fluctuate to >or=3 events
             is 1.7x10(-4). An upper limit on the cross section of pp-->p
             + gammagamma + p production is set at 410 fb with 95%
             confidence level.},
   Doi = {10.1103/physrevlett.99.242002},
   Key = {fds309486}
}

@article{fds309503,
   Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
             T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
             K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
             S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak,
             M},
   Title = {Limits on anomalous triple gauge couplings in pp̄
             collisions at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {76},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2007},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.76.111103},
   Abstract = {We present a search for anomalous triple gauge couplings
             (ATGC) in WW and WZ boson production. The boson pairs are
             produced in pp̄ collisions at s=1.96TeV, and the data
             sample corresponds to 350pb-1 of integrated luminosity
             collected with the CDF II detector at the Fermilab Tevatron.
             In this search one W decays to leptons, and the other boson
             (W or Z) decays hadronically. Combining with a previously
             published CDF measurement of Wγ boson production yields
             ATGC limits of -0.18<λ<0.17 and -0.46<Δκ<0.39 at the 95%
             confidence level, using a cutoff scale Λ=1.5TeV. © 2007
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.76.111103},
   Key = {fds309503}
}

@article{fds361227,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
             A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Lorenzo,
             GD and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and Pedis,
             DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
             D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
             A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
             SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
             Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
             YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
             B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
             S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
             F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Griso,
             SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
             V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
             O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
             A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
             M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ},
   Title = {Observation of the decay Bc±→J/ψπ± and measurement of
             the Bc± mass},
   Journal = {Physical Review Letters},
   Volume = {100},
   Number = {18},
   Pages = {182002},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevLett.100.182002},
   Abstract = {The Bc± meson is observed through the decay Bc±→J/
             ψπ±, in data corresponding to an integrated luminosity of
             2.4fb-1 recorded by the Collider Detector at Fermilab II
             detector at the Fermilab Tevatron. A signal of 108±15
             candidates is observed, with a significance that exceeds
             8σ. The mass of the Bc± meson is measured to be
             6275.6±2.9(stat)±2.5(syst)MeV/c2. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevLett.100.182002},
   Key = {fds361227}
}

@article{fds309437,
   Author = {Aaltonen, T and others},
   Title = {Search for Supersymmetry in pp̅ Collisions at √ s
             =1.96 TeV Using the Trilepton Signature for
             Chargino-Neutralino Production},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {25},
   Pages = {251801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.251801},
   Abstract = {We use the three lepton and missing energy trilepton
             signature to search for chargino-neutralino production with
             2.0  fb-1 of integrated luminosity collected by the CDF
             II experiment at the Tevatron pp̅ collider. We expect an
             excess of approximately 11 supersymmetric events for a
             choice of parameters of the mSUGRA model, but our
             observation of 7 events is consistent with the standard
             model expectation of 6.4 events. We constrain the mSUGRA
             model of supersymmetry and rule out chargino masses up to
             145  GeV/c2 for a specific choice of
             parameters.},
   Doi = {10.1103/physrevlett.101.251801},
   Key = {fds309437}
}

@article{fds309438,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the Single-Top-Quark Production Cross Section
             at CDF},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {25},
   Pages = {252001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.252001},
   Abstract = {We report a measurement of the single-top-quark production
             cross section in 2.2  fb-1 of pp̅ collision data
             collected by the Collider Detector at Fermilab at
             sqrt[s]=1.96  TeV. Candidate events are classified as
             signal-like by three parallel analyses which use likelihood,
             matrix element, and neural network discriminants. These
             results are combined in order to improve the sensitivity. We
             observe a signal consistent with the standard model
             prediction, but inconsistent with the background-only model
             by 3.7 standard deviations with a median expected
             sensitivity of 4.9 standard deviations. We measure a cross
             section of 2.2-0.6+0.7(stat+syst)  pb, extract the
             Cabibbo-Kobayashi-Maskawa matrix-element value
             |Vtb|=0.88-0.12+0.13(stat+syst) &plusmn; 0.07(theory), and
             set the limit |Vtb|&gt;0.66 at the 95% C.L.},
   Doi = {10.1103/physrevlett.101.252001},
   Key = {fds309438}
}

@article{fds309439,
   Author = {Aaltonen, T and others},
   Title = {Search for the Higgs Boson Produced in Association with
             Z→ℓ+ℓ- in pp̅ Collisions at sqrt[s] =1.96
             TeV},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {25},
   Pages = {251803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.251803},
   Abstract = {We present a search for the Higgs boson in the process qq̅
             →ZH→ℓ+ℓ-bb̅ . The analysis uses an integrated
             luminosity of 1  fb-1 of pp̅ collisions produced at
             sqrt[s]=1.96  TeV and accumulated by the upgraded
             Collider Detector at Fermilab (CDF II). We employ artificial
             neural networks both to correct jets mismeasured in the
             calorimeter and to distinguish the signal kinematic
             distributions from those of the background. We see no
             evidence for Higgs boson production, and set 95% C.L. upper
             limits on σZHB(H→bb̅ ), ranging from 1.5 to 1.2 pb for a
             Higgs boson mass (mH) of 110 to 150  GeV/c2.},
   Doi = {10.1103/physrevlett.101.251803},
   Key = {fds309439}
}

@article{fds309440,
   Author = {Aaltonen, and T, and others},
   Title = {{Forward-Backward Asymmetry in Top Quark Production in
             $p\bar{p}$ Collisions at $sqrt{s}=1.96$ TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {20},
   Pages = {202001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.202001},
   Abstract = {We present measurements of the forward-backward charge
             asymmetry in top pair production using 1.9 fb-1 of
             $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV recorded with
             the Collider Detector at Fermilab II. Correcting for
             acceptance and measurement dilutions we obtain parton-level
             asymmetries of AFB$p\bar{p}$=0.17\pm 0.08 in the $p\bar{p}$
             frame and AFB$t\bar{t}$=0.24+/-0.14 in the $t\bar{t}$ frame.
             The values are consistent with the standard model
             expectation and disfavor exotic production mechanisms with
             significant negative values.},
   Doi = {10.1103/physrevlett.101.202001},
   Key = {fds309440}
}

@article{fds309442,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for large extra dimensions in final states
             containing one photon or jet and large missing transverse
             energy produced in $p \bar{p}$ collisions at $\sqrt{s}$ =
             1.96-TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {18},
   Pages = {181602},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.181602},
   Abstract = {We present the results of searches for large extra
             dimensions in samples of events with large missing
             transverse energy E-slash T and either a photon or a jet
             produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             collected with the Collider Detector at Fermilab II. For
             gamma+E-slash T and jet+E-slash T candidate samples
             corresponding to 2.0 and 1.1 fb-1 of integrated luminosity,
             respectively, we observe good agreement with standard model
             expectations and obtain a combined lower limit on the
             fundamental parameter of the large extra dimensions model MD
             as a function of the number of extra dimensions in the
             model.},
   Doi = {10.1103/physrevlett.101.181602},
   Key = {fds309442}
}

@article{fds309443,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Doubly Charged Higgs Bosons with Lepton-Flavor-
             Violating Decays involving Tau Leptons}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {12},
   Pages = {121801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.121801},
   Abstract = {We search for pair production of doubly charged Higgs
             particles ($H^{\pm\pm}$) followed by decays into
             electron-tau (etau) and muon-tau (mu tau) pairs using data
             (350 pb-1) collected from $\bar{p} p$ collisions at
             $\sqrt{s}=1.96$ TeV by the CDF II experiment. We search
             separately for cases where three or four final-state leptons
             are detected, and combine results for exclusive decays to
             left-handed etau (\mu tau) pairs. We set an $H^{\pm\pm}$
             lower mass limit of 114(112) GeV/c2 at the 95% confidence
             level.},
   Doi = {10.1103/physrevlett.101.121801},
   Key = {fds309443}
}

@article{fds309444,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Pair Production of Scalar Top Quarks Decaying to
             a $\tau$ Lepton and a $b$ Quark in $p\bar{p}$ Collisions at
             sqrt{s}=1.96 TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {101},
   Number = {7},
   Pages = {071802},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.101.071802},
   Abstract = {We search for pair production of supersymmetric top quarks
             (t-tilde1), followed by R-parity violating decay
             t-tilde1-->taub with a branching ratio beta, using 322 pb-1
             of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected by
             the upgraded Collider Detector at Fermilab. Two candidate
             events pass our final selection criteria, consistent with
             the standard model expectation. We set upper limits on the
             cross section sigma(t-tilde1[overline t-tilde ]1)×beta2 as
             a function of the top-squark mass m(t-tilde1). Assuming
             beta=1, we set a 95% confidence level limit m(t-tilde1)>153
             GeV/c2. The limits are also applicable to the case of a
             third-generation scalar leptoquark (LQ3) decaying
             LQ3-->taub.},
   Doi = {10.1103/physrevlett.101.071802},
   Key = {fds309444}
}

@article{fds309445,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for the Higgs boson in events with missing
             transverse energy and $b$ quark jets produced in proton-
             antiproton collisions at $\sqrt{s}$ =1.96
             TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {21},
   Pages = {211801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.211801},
   Abstract = {We search for the standard model Higgs boson produced in
             association with an electroweak vector boson in events with
             no identified charged leptons, large imbalance in transverse
             momentum, and two jets where at least one contains a
             secondary vertex consistent with the decay of b hadrons. We
             use ~1 fb-1 integrated luminosity of $p\bar{p}$ collisions
             at $\sqrt{s}=1.96$ TeV recorded by the Collider Detector at
             Fermilab II experiment at the Tevatron. We find 268 (16)
             single (double) b-tagged candidate events, where $248\pm 43$
             ($14.4\pm 2.7$) are expected from standard model background
             processes. We observe no significant excess over the
             expected background and thus set 95% confidence level upper
             limits on the Higgs boson production cross section for
             several Higgs boson masses ranging from 110 to 140 GeV/c2.
             For a mass of 115 GeV/c2, the observed (expected) limit is
             20.4 (14.2) times the standard model prediction.},
   Doi = {10.1103/physrevlett.100.211801},
   Key = {fds309445}
}

@article{fds309446,
   Author = {Aaltonen, and T, and others},
   Title = {{Strong Evidence for $Z Z$ Production in panti-p Collisions
             at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {20},
   Pages = {201801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.201801},
   Abstract = {We report the first evidence of Z boson pair production at a
             hadron collider with a significance exceeding 4 standard
             deviations. This result is based on a data sample
             corresponding to 1.9 fb-1 of integrated luminosity from
             $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected with
             the Collider Detector at Fermilab II detector. In the
             [script-l][script-l][script-l][prime][script-l][prime]
             channel, we observe three ZZ candidates with an expected
             background of 0.096-0.063+0.092 events. In the
             [script-l][script-l]nunu channel, we use a leading-order
             calculation of the relative ZZ and WW event probabilities to
             discriminate between signal and background. In the
             combination of [script-l][script-l][script-l][prime][script-l][prime]
             and [script-l][script-l]nunu channels, we observe an excess
             of events with a probability of 5.1×10-6 to be due to the
             expected background. This corresponds to a significance of
             4.4 standard deviations. The measured cross section is
             sigma($p\bar{p}$-->ZZ)=1.4-0.6+0.7(stat+syst) pb, consistent
             with the standard model expectation.},
   Doi = {10.1103/physrevlett.100.201801},
   Key = {fds309446}
}

@article{fds309447,
   Author = {Aaltonen, and T, and others},
   Title = {{First Flavor-Tagged Determination of Bounds on Mixing-
             Induced CP Violation in Bs -> J/psi phi Decays}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {16},
   Pages = {161802},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.161802},
   Abstract = {This Letter describes the first determination of bounds on
             the CP-violation parameter 2betas using Bs0 decays in which
             the flavor of the bottom meson at production is identified.
             The result is based on approximately 2000 Bs0-->J/psiphi
             decays reconstructed in a 1.35 fb-1 data sample collected
             with the CDF II detector using $p\bar{p}$ collisions
             produced at the Fermilab Tevatron. We report confidence
             regions in the two-dimensional space of 2betas and the
             decay-width difference DeltaGamma. Assuming the standard
             model predictions of 2betas and DeltaGamma, the probability
             of a deviation as large as the level of the observed data is
             15%, corresponding to 1.5 Gaussian standard
             deviations.},
   Doi = {10.1103/physrevlett.100.161802},
   Key = {fds309447}
}

@article{fds309448,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Heavy Top-like Quarks Using Lepton Plus Jets
             Events in 1.96-TeV $p \bar{p}$ Collisions}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {16},
   Pages = {161803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.161803},
   Abstract = {We present the results of a search for pair production of a
             new heavy toplike quark t[prime] decaying to a ${W}$ boson
             and another quark using the Collider Detector at Fermilab II
             detector in run II of the Tevatron $p\bar{p}$ collider.
             Using a data sample corresponding to 760 pb-1 of integrated
             luminosity, we fit the observed spectrum of total transverse
             energy and reconstructed t[prime] quark mass to a
             combination of standard model processes and t[prime] pair
             production. We see no evidence for t[prime][overline
             t][prime] production, and we infer a lower limit of 256
             GeV/c2 on the mass of the t[prime] at 95% C.L. assuming
             standard strong couplings for the t[prime].},
   Doi = {10.1103/physrevlett.100.161803},
   Key = {fds309448}
}

@article{fds309449,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of Lifetime and Decay-Width Difference in
             $B^0_s \to J/\psi \phi$ Decays}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {12},
   Pages = {121803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.121803},
   Abstract = {We measure the mean lifetime ${\tau=2/(\Gamma_L+\Gamma_H)}$
             and the decay-width difference ${\Delta\Gamma=\Gamma_L-\Gamma_H}$
             of the light and heavy mass eigenstates of the ${B_s^0}$
             meson, ${B_{sL}^0}$ and ${B_{sH}^0}$, in ${B_s^0\to
             J/\psi\phi}$ decays using 1.7 fb-1 of data collected with
             the CDF II detector at the Fermilab Tevatron $p\bar{p}$
             collider. Assuming CP conservation, a good approximation for
             the ${B_s^0}$ system in the standard model, we obtain
             ${\Delta\Gamma=0.076_{-0.063}^{+0.059}}$(stat)$\pm
             0.006$(syst) ps-1 and $\tau=1.52\pm 0.04$(stat)$\pm
             0.02$(syst) ps, the most precise measurements to date. Our
             constraints on the weak phase and ${\Delta\Gamma}$ are
             consistent with CP conservation.},
   Doi = {10.1103/physrevlett.100.121803},
   Key = {fds309449}
}

@article{fds309450,
   Author = {Aaltonen, and T, and others},
   Title = {{Evidence for D0-D0bar mixing using the CDF II
             Detector}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {12},
   Pages = {121802},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.121802},
   Abstract = {We measure the time dependence of the ratio of decay rates
             for the rare decay D0-->K+pi- to the Cabibbo-favored decay
             D0-->K-pi+. A signal of 12.7×103 D0-->K+pi- decays was
             obtained using the Collider Detector at Fermilab II detector
             at the Fermilab Tevatron with an integrated luminosity of
             1.5 fb-1. We measure the D0-[overline D]0 mixing parameters
             (RD,y[prime],x[prime]2), and find that the data are
             inconsistent with the no-mixing hypothesis with a
             probability equivalent to 3.8 Gaussian standard
             deviations.},
   Doi = {10.1103/physrevlett.100.121802},
   Key = {fds309450}
}

@article{fds309451,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of Inclusive Jet Cross Sections in $Z/\gamma^*
             (\to ee)+$ jets Production in $p\bar{p}$ Collisions at
             $\sqrt{s}=1.96$ TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {10},
   Pages = {102001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.102001},
   Abstract = {Inclusive jet cross sections in Z/gamma* events, with
             Z/gamma* decaying into an electron-positron pair, are
             measured as a function of jet transverse momentum and jet
             multiplicity in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             with the upgraded Collider Detector at Fermilab in run II,
             based on an integrated luminosity of 1.7 fb-1. The
             measurements cover the rapidity region |yjet|Tjet>30 GeV/c.
             Next-to-leading order perturbative QCD predictions are in
             good agreement with the measured cross sections.},
   Doi = {10.1103/physrevlett.100.102001},
   Key = {fds309451}
}

@article{fds309453,
   Author = {Aaltonen, and T, and others},
   Title = {{Observation of Orbitally Excited ${B_s}$
             Mesons}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {8},
   Pages = {082001},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.082001},
   Abstract = {We report the observation of two narrow resonances
             consistent with states of orbitally excited (L=1) Bs mesons
             using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             collected with the Collider Detector at Fermilab II detector
             at the Fermilab Tevatron. We use two-body decays into K- and
             B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu^+\mu^-
             or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
             the masses of the two states to be m(Bs1)=5829.4\pm 0.7
             MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
   Doi = {10.1103/physrevlett.100.082001},
   Key = {fds309453}
}

@article{fds309455,
   Author = {Aaltonen, and T, and others},
   Title = {{Cross Section Constrained Top Quark Mass Measurement from
             Dilepton Events at the Tevatron}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {6},
   Pages = {062005},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.062005},
   Abstract = {We report the first top-quark mass measurement that uses a
             cross-section constraint to improve the mass determination.
             This measurement is made with a dilepton $t\bar{t}$ event
             candidate sample collected with the Collider Detector II at
             Fermilab. From a data sample corresponding to an integrated
             luminosity of 1.2 fb-1, we measure a top-quark mass of
             170.7-3.9+4.2(stat)\pm 2.6(syst)\pm 2.4(theory) GeV/c2. The
             measurement without the cross-section constraint is
             169.7-4.9+5.2(stat)\pm 3.1(syst) GeV/c2.},
   Doi = {10.1103/physrevlett.100.062005},
   Key = {fds309455}
}

@article{fds309456,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Standard Model Higgs Bosons Produced in
             Association with ${W}$ Bosons}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {4},
   Pages = {041801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.041801},
   Abstract = {We report the observation of two narrow resonances
             consistent with states of orbitally excited (L=1) Bs mesons
             using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             collected with the Collider Detector at Fermilab II detector
             at the Fermilab Tevatron. We use two-body decays into K- and
             B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu +\mu -
             or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
             the masses of the two states to be m(Bs1)=5829.4\pm 0.7
             MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
   Doi = {10.1103/physrevlett.100.041801},
   Key = {fds309456}
}

@article{fds309457,
   Author = {Aaltonen, and T, and others},
   Title = {{First observation of the decay $B^0_s \to D^-_s D^+_s$ and
             measurement of its branching ratio}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {2},
   Pages = {021803},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.021803},
   Abstract = {We report the observation of the exclusive decay
             Bs0-->Ds-Ds+ at the 7.5 standard deviation level using 355
             pb-1 of data collected by the CDF II detector in $p\bar{p}$
             collisions at $\sqrt{s}=1.96$ TeV at the Fermilab Tevatron.
             We measure the relative branching ratio [script
             B](Bs0-->Ds-Ds+)/[script B](B0-->D-Ds+) =1.44-0.44+0.48.
             Using the world average value for [script B](B0-->D-Ds+), we
             find [script B](Bs0-->Ds-Ds+) =(9.4-4.2+4.4)×10-3. This
             provides a lower bound DeltaGammasCP/Gammas> =2[script
             B](Bs0-->Ds-Ds+)>1.2×10-2 at 95% C.L.},
   Doi = {10.1103/physrevlett.100.021803},
   Key = {fds309457}
}

@article{fds309458,
   Author = {al, GAE},
   Title = {The ATLAS Experiment at the CERN Large Hadron
             Collider},
   Journal = {JINST 3S08003},
   Volume = {3},
   Number = {8},
   Pages = {S08003-S08003},
   Publisher = {IOP Publishing},
   Year = {2008},
   url = {http://dx.doi.org/10.1088/1748-0221/3/08/S08003},
   Doi = {10.1088/1748-0221/3/08/S08003},
   Key = {fds309458}
}

@article{fds309459,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for third generation vector leptoquarks in
             $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {9},
   Pages = {091105},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.091105},
   Abstract = {We search for a third generation vector leptoquark (VLQ3)
             that decays to a $b$ quark and tau lepton using the CDF II
             detector and 320 pb-1 of integrated luminosity from the
             Fermilab Tevatron. Observing a number of events in agreement
             with standard model expectations, we obtain, assuming
             Yang-Mills (minimal) couplings, the most stringent upper
             limit on the VLQ3 pair production cross section of 344 fb
             (493 fb) and lower limit on the VLQ3 mass of 317 GeV/c2 (251
             GeV/c2) at 95% C.L.},
   Doi = {10.1103/PhysRevD.77.091105},
   Key = {fds309459}
}

@article{fds309460,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of correlated b-bbar production in ${p
             \bar{p}}$ collisions at s**(1/2) = 1960 GeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {7},
   Pages = {072004},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.072004},
   Abstract = {We present a measurement of the correlated b[overline b]
             production cross section. The data used in this analysis
             were taken with the upgraded CDF detector (CDF II) at the
             Fermilab Tevatron collider, and correspond to an integrated
             luminosity of 742 pb-1. We utilize muon pairs with invariant
             mass 5=3 GeV/c and |eta|=2 GeV/c and |y| mu,[overline b] -->
             mu=1549\pm 133 pb. We compare this result with theoretical
             predictions and previous measurements. We also report the
             measurement of sigmac --> mu,[overline c] --> mu, a
             by-product of the study of the background to b[overline b]
             production.},
   Doi = {10.1103/PhysRevD.77.072004},
   Key = {fds309460}
}

@article{fds309462,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for resonant $t \bar{t}$ production in $p \bar{p}$
             collisions at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev. Lett.},
   Volume = {100},
   Number = {23},
   Pages = {231801},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/physrevlett.100.231801},
   Abstract = {We report on a search for narrow-width particles decaying to
             a top and antitop quark pair. The data set used in the
             analysis corresponds to an integrated luminosity of 680 pb-1
             collected with the Collider Detector at Fermilab in run II.
             We present 95% confidence level upper limits on the cross
             section times branching ratio. Assuming a specific
             top-color-assisted technicolor production model, the
             leptophobic Z[prime] with width GammaZ[prime]=0.012MZ[prime],
             we exclude the mass range MZ[prime]},
   Doi = {10.1103/physrevlett.100.231801},
   Key = {fds309462}
}

@article{fds309463,
   Author = {Aaltonen, and T, and others},
   Title = {{Model-Independent and Quasi-Model-Independent Search for
             New Physics at CDF}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {1},
   Pages = {012002},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.012002},
   Abstract = {Data collected in run II of the Fermilab Tevatron are
             searched for indications of new electroweak scale physics.
             Rather than focusing on particular new physics scenarios,
             CDF data are analyzed for discrepancies with respect to the
             standard model prediction. A model-independent approach
             (Vista) considers the gross features of the data and is
             sensitive to new large cross section physics. A
             quasi-model-independent approach (Sleuth) searches for a
             significant excess of events with large summed transverse
             momentum and is particularly sensitive to new electroweak
             scale physics that appears predominantly in one final state.
             This global search for new physics in over 300 exclusive
             final states in 927 pb-1 of $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV reveals no such significant indication
             of physics beyond the standard model.},
   Doi = {10.1103/PhysRevD.78.012002},
   Key = {fds309463}
}

@article{fds309465,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for chargino-neutralino production in ${p \bar{p}}$
             collisions at 1.96 TeV with high pT leptons}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {5},
   Pages = {052002},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.052002},
   Abstract = {We present a search for the associated production of
             charginos and neutralinos in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV. The data were collected at the Collider
             Detector at Fermilab (CDF II) and correspond to integrated
             luminosities between 0.7 and 1.0 fb-1. We look for final
             states with one high-pT electron or muon, and two additional
             leptons. Our results are consistent with the standard model
             expectations, and we set limits on the cross section as a
             function of the chargino mass in three different
             supersymmetric scenarios. For a specific minimal
             supersymmetric standard model scenario with no slepton
             mixing, we set a 95% C.L. limit at 151 GeV/c2.},
   Doi = {10.1103/PhysRevD.77.052002},
   Key = {fds309465}
}

@article{fds309466,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of Ratios of Fragmentation Fractions for Bottom
             Hadrons in $p \bar{p}$ Collisions at $\sqrt{s}$ =
             1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.072003},
   Abstract = {This paper describes the first measurement of b-quark
             fragmentation fractions into bottom hadrons in Run II of the
             Tevatron Collider at Fermilab. The result is based on a 360
             pb-1 sample of data collected with the CDF II detector in
             $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. Semileptonic
             decays of [overline B]0, B-, and [overline B]s0 mesons, as
             well as Lambdab0 baryons, are reconstructed. For an
             effective bottom hadron pT threshold of 7 GeV/c, the
             fragmentation fractions are measured to be fu/fd=1.054\pm
             0.018(stat)-0.045+0.025(sys)\pm 0.058([script B]),
             fs/(fu+fd)=0.160\pm 0.005(stat)-0.010+0.011(sys)-0.034+0.057([script
             B]), and fLambdab/(fu+fd)=0.281\pm 0.012(stat)-0.056+0.058(sys)-0.087+0.128([script
             B]), where the uncertainty [script B] is due to
             uncertainties on measured branching ratios. The value of
             fs/(fu+fd) agrees within one standard deviation with
             previous CDF measurements and the world average of this
             quantity, which is dominated by LEP measurements. However,
             the ratio fLambdab/(fu+fd) is approximately twice the value
             previously measured at LEP. The approximately 2sigma
             discrepancy is examined in terms of kinematic differences
             between the two production environments.},
   Doi = {10.1103/PhysRevD.77.072003},
   Key = {fds309466}
}

@article{fds309467,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for New Heavy Particles Decaying to $Z^0 Z^0 \to
             eeee$ in $p$ - $\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-
             TeV}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {1},
   Pages = {012008},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.012008},
   Abstract = {We report the results of a search for the anomalous
             production of a massive particle decaying to four electrons
             via two Z0 bosons in 1.1 fb-1 of $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV collected by the CDF II detector at
             Fermilab. We employ optimized electron identification
             criteria to maximize acceptance and efficiency. We estimate
             the backgrounds in the invariant mass range 500–1000
             GeV/c2 to be 0.028\pm 0.009(stat)\pm 0.011(syst) events. We
             observe zero events in this search region. Assuming a
             Randall-Sundrum graviton production model, we set 95% C.L.
             limits on sigma×BF(G-->Z0Z0)},
   Doi = {10.1103/PhysRevD.78.012008},
   Key = {fds309467}
}

@article{fds309468,
   Author = {Aaltonen, and T, and others},
   Title = {{Observation of Exclusive Dijet Production at the Fermilab
             Tevatron ${p \bar{p}}$ Collider}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {5},
   Pages = {052004},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.052004},
   Abstract = {We present the first observation and cross section
             measurement of exclusive dijet production in [overline p]p
             interactions, [overline p]p-->[overline p]+dijet+p. Using a
             data sample of 310 pb-1 collected by the Run II Collider
             Detector at Fermilab at $\sqrt{s}=1.96$ TeV, exclusive cross
             sections for events with two jets of transverse energy
             ETjet>=10 GeV have been measured as a function of minimum
             ETjet. The exclusive signal is extracted from fits to data
             distributions based on Monte Carlo simulations of expected
             dijet signal and background shapes. The simulated background
             distribution shapes are checked in a study of a largely
             independent data sample of 200 pb-1 of b-tagged jet events,
             where exclusive dijet production is expected to be
             suppressed by the Jz=0 total angular momentum selection
             rule. Results obtained are compared with theoretical
             expectations, and implications for exclusive Higgs boson
             production at the pp Large Hadron Collider at sqrt(s)=14 TeV
             are discussed.},
   Doi = {10.1103/PhysRevD.77.052004},
   Key = {fds309468}
}

@article{fds309471,
   Author = {Aaltonen, and T, and others},
   Title = {{Two-particle momentum correlations in jets produced in $p
             \bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {9},
   Pages = {092001},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.092001},
   Abstract = {We present the first measurement of two-particle momentum
             correlations in jets produced in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV. Results are obtained for charged
             particles within a restricted cone with an opening angle of
             0.5 radians around the jet axis and for events with dijet
             masses between 66 and 563 GeV/c2. A comparison of the
             experimental data to theoretical predictions obtained for
             partons within the framework of resummed perturbative QCD in
             the next-to-leading log approximation shows that the parton
             momentum correlations survive the hadronization stage of jet
             fragmentation, giving further support to the hypothesis of
             local parton-hadron duality. The extracted value of the
             next-to-leading-log-approximation parton shower cutoff scale
             Qeff set equal to LambdaQCD is found to be
             (1.4-0.7+0.9)×100 MeV.},
   Doi = {10.1103/PhysRevD.77.092001},
   Key = {fds309471}
}

@article{fds309472,
   Author = {Aaltonen, and T, and others},
   Title = {{Limits on the Production of Narrow $t\bar{t}$ Resonances in
             $p\bar{p}$ Collisions at $\sqrt{s}=1.96$
             TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {5},
   Pages = {051102},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.051102},
   Abstract = {We search for evidence of resonant top quark pair production
             in 955 pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
             recorded with the CDF II detector at the Fermilab Tevatron.
             For fully reconstructed candidate $t\bar{t}$ events
             triggered on leptons with large transverse momentum and
             containing at least one identified b-quark jet, we compare
             the invariant mass spectrum of $t\bar{t}$ pairs to the
             expected superposition of standard model $t\bar{t}$,
             non-$t\bar{t}$ backgrounds, and a simple resonance model
             based on a sequential Z[prime] boson. We establish upper
             limits for sigma($p\bar{p}$-->Z[prime])·Br(Z[prime]-->$t\bar{t}$)
             in the Z[prime] mass interval from 450 GeV/c2 to 900 GeV/c2.
             A topcolor leptophobic Z[prime] is ruled out below 720
             GeV/c2, and the cross section of any narrow Z[prime]-like
             state decaying to $t\bar{t}$ is found to be less than 0.64
             pb at 95% C.L. for MZ[prime] above 700 GeV/c2.},
   Doi = {10.1103/PhysRevD.77.051102},
   Key = {fds309472}
}

@article{fds309475,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of the cross section for ${W}$-boson production
             in association with jets in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV}},
   Journal = {Phys. Rev.},
   Volume = {D77},
   Number = {6},
   Pages = {011108},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1007/JHEP06(2013)084},
   Abstract = {We present a measurement of the cross section for W-boson
             production in association with jets in $p\bar{p}$ collisions
             at $\sqrt{s}=1.96$ TeV. The analysis uses a data sample
             corresponding to an integrated luminosity of 320 pb-1
             collected with the CDF II detector. W bosons are identified
             in their electron decay channel and jets are reconstructed
             using a cone algorithm. For each W+>=n-jet sample (n=1-4) we
             measure the differential cross section dsigma($p\bar{p}$-->W+>=n-jet)/dETnth-jet×[script
             B](W-->enu) with respect to the transverse energy ET of the
             nth-highest ET jet above 20 GeV, and the total cross section
             sigma($p\bar{p}$-->W+>=n-jet;ETnth-jet>25 GeV)×[script
             B](W-->enu), for a restricted W-->enu decay phase space. The
             cross sections, corrected for all detector effects, can be
             directly compared to particle level W+jet(s) predictions. We
             present here comparisons to leading order and
             next-to-leading order predictions.},
   Doi = {10.1007/JHEP06(2013)084},
   Key = {fds309475}
}

@article{fds309476,
   Author = {Aaltonen, and T, and others},
   Title = {{Search for Heavy, Long-Lived Neutralinos that Decay to
             Photons at CDF II Using Photon Timing}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {3},
   Pages = {032015},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.032015},
   Abstract = {We present the results of the first hadron collider search
             for heavy, long-lived neutralinos that decay via
             chi-tilde10-->gammaG-tilde in gauge-mediated supersymmetry
             breaking models. Using an integrated luminosity of 570\pm 34
             pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV, we
             select gamma+jet+missing transverse energy candidate events
             based on the arrival time of a high-energy photon at the
             electromagnetic calorimeter as measured with a timing system
             that was recently installed on the CDF II detector. We find
             2 events, consistent with the background estimate of 1.3\pm
             0.7 events. While our search strategy does not rely on
             model-specific dynamics, we set cross section limits and
             place the world-best 95% C.L. lower limit on the chi-tilde10
             mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup 0]=5
             ns.},
   Doi = {10.1103/PhysRevD.78.032015},
   Key = {fds309476}
}

@article{fds309477,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of $b$-jet Shapes in Inclusive Jet Production
             in $p \bar{p}$ Collisions at $\sqrt{s}$ =
             1.96-TeV}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {7},
   Pages = {072005},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.072005},
   Abstract = {We present a measurement of the shapes of b-jets using 300
             pb-1 of data obtained with the upgraded Collider Detector at
             Fermilab (CDF II) in $p \bar{p}$ collisions at
             center-of-mass energy $\sqrt{s}=1.96$ TeV. This measurement
             covers a wide transverse momentum range, from 52 to 300
             GeV/c. Samples of heavy-flavor enhanced jets together with
             inclusive jets are used to extract the average shapes of
             b-jets. The b-jets are expected to be broader than inclusive
             jets. Moreover, b-jets containing a single b-quark are
             expected to be narrower than those containing a $b \bar{b}$
             pair from gluon splitting. The measured b-jet shapes are
             found to be significantly broader than expected from the
             pythia and herwig Monte Carlo simulations. This effect may
             arise from an underestimation of the fraction of b-jets
             originating from gluon splitting in these simulations. The
             jet shape distributions provided in this paper could be
             compared to any full Monte Carlo simulation and could be
             used to further constrain the various parameters.},
   Doi = {10.1103/PhysRevD.78.072005},
   Key = {fds309477}
}

@article{fds309478,
   Author = {Aaltonen, and T, and others},
   Title = {{Measurement of the Inclusive Jet Cross Section at the
             Fermilab Tevatron $p \bar{p}$ Collider Using a Cone-Based
             Jet Algorithm}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {5},
   Pages = {052006},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.052006},
   Abstract = {We present a measurement of the inclusive jet cross section
             in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV based on
             data collected by the CDF II detector with an integrated
             luminosity of 1.13 fb-1. The measurement was made using the
             cone-based midpoint jet clustering algorithm in the rapidity
             region of |y|},
   Doi = {10.1103/PhysRevD.78.052006},
   Key = {fds309478}
}

@article{fds309479,
   Author = {al, EAE},
   Title = {Combined performance tests before installation of the ATLAS
             Semiconductor and Transition Radiation Tracking
             Detectors},
   Journal = {Jinst 3 P08003},
   Volume = {3},
   Number = {8},
   Pages = {P08003-P08003},
   Publisher = {IOP Publishing},
   Year = {2008},
   url = {http://dx.doi.org/10.1088/1748-0221/3/08/P08003},
   Abstract = {The ATLAS (A Toroidal LHC ApparatuS) Inner Detector provides
             charged particle tracking in the centre of the ATLAS
             experiment at the Large Hadron Collider (LHC). The Inner
             Detector consists of three subdetectors: the Pixel Detector,
             the Semiconductor Tracker (SCT), and the Transition
             Radiation Tracker (TRT). This paper summarizes the tests
             that were carried out at the final stage of SCT+TRT
             integration prior to their installation in ATLAS. The
             combined operation and performance of the SCT and TRT barrel
             and endcap detectors was investigated through a series of
             noise tests, and by recording the tracks of cosmic rays.
             This was a crucial test of hardware and software of the
             combined tracker detector systems. The results of noise and
             cross-talk tests on the SCT and TRT in their final assembled
             configuration, using final readout and supply hardware and
             software, are reported. The reconstruction and analysis of
             the recorded cosmic tracks allowed testing of the offline
             analysis chain and verification of basic tracker performance
             parameters, such as efficiency and spatial resolution, in
             combined operation before installation. © 2008 IOP
             Publishing Ltd. and SISSA.},
   Doi = {10.1088/1748-0221/3/08/P08003},
   Key = {fds309479}
}

@article{fds309480,
   Author = {collaboration, ATRT},
   Title = {The ATLAS TRT end-cap detectors},
   Journal = {JINST 3 P10003},
   Volume = {3},
   Number = {10},
   Pages = {P10003-P10003},
   Publisher = {IOP Publishing},
   Year = {2008},
   url = {http://dx.doi.org/10.1088/1748-0221/3/10/P10003},
   Abstract = {The ATLAS TRT end-cap is a tracking drift chamber using
             245,760 individual tubular drift tubes. It is a part of the
             TRT tracker which consist of the barrel and two end-caps.
             The TRT end-caps cover the forward and backward
             pseudo-rapidity region 1.0 < |η| < 2.0, while the TRT
             barrel central η region |η| < 1.0. The TRT system provides
             a combination of continuous tracking with many measurements
             in individual drift tubes (or straws) and of electron
             identification based on transition radiation from fibers or
             foils interleaved between the straws themselves. Along with
             other two sub-system, namely the Pixel detector and Semi
             Conductor Tracker (SCT), the TRT constitutes the ATLAS Inner
             Detector. This paper describes the recently completed and
             installed TRT end-cap detectors, their design, assembly,
             integration and the acceptance tests applied during the
             construction. © 2008 IOP Publishing Ltd and
             SISSA.},
   Doi = {10.1088/1748-0221/3/10/P10003},
   Key = {fds309480}
}

@article{fds309483,
   Author = {collaboration, ATLASTRT},
   Title = {The ATLAS TRT Electronics},
   Journal = {JINST 3 P06007},
   Volume = {3},
   Number = {6},
   Pages = {P06007-P06007},
   Publisher = {IOP Publishing},
   Year = {2008},
   url = {http://dx.doi.org/10.1088/1748-0221/3/06/P06007},
   Abstract = {The ATLAS inner detector consists of three sub-systems: the
             pixel detector spanning the radius range 4cm-20cm, the
             semiconductor tracker at radii from 30 to 52 cm, and the
             transition radiation tracker (TRT), tracking from 56 to 107
             cm. The TRT provides a combination of continuous tracking
             with many projective measurements based on individual drift
             tubes (or straws) and of electron identification based on
             transition radiation from fibres or foils interleaved
             between the straws themselves. This paper describes the on
             and off detector electronics for the TRT as well as the TRT
             portion of the data acquisition (DAQ) system. © 2008 IOP
             Publishing Ltd and SISSA.},
   Doi = {10.1088/1748-0221/3/06/P06007},
   Key = {fds309483}
}

@article{fds309484,
   Author = {Aaltonen, and T, and others},
   Title = {{Cross section measurements of high-pT dilepton final-state
             processes using a global fitting method}},
   Journal = {Phys. Rev.},
   Volume = {D78},
   Number = {1},
   Pages = {012003},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.012003},
   Abstract = {We present a new method for studying high-pT dilepton events
             $(e^\pm e^{-/+}, \mu^\pm \mu^{-/+}, e^\pm\mu^{-/+})$ and
             simultaneously extracting the production cross sections of
             $p\bar{p}$-->$t\bar{t}$, $p\bar{p}$-->W+W-, and
             $p\bar{p}$-->Z0-->tau+tau- at a center-of-mass energy of
             $\sqrt{s}=1.96$ TeV. We perform a likelihood fit to the
             dilepton data in a parameter space defined by the missing
             transverse energy and the number of jets in the event. Our
             results, which use 360 pb-1 of data recorded with the CDF II
             detector at the Fermilab Tevatron Collider, are
             sigma($t\bar{t}$)=8.5-2.2+2.7 pb, sigma(W+W-)=16.3-4.4+5.2
             pb, and sigma(Z0-->tau+tau-)=291-46+50 pb.},
   Doi = {10.1103/PhysRevD.78.012003},
   Key = {fds309484}
}

@article{fds309485,
   Author = {Lee, JH and Schmieg, SJ and Oh, SH},
   Title = {Improved NOx reduction over the staged Ag/Al2O3
             catalyst system},
   Journal = {Applied Catalysis A: General},
   Volume = {342},
   Number = {1-2},
   Pages = {78-86},
   Year = {2008},
   url = {http://dx.doi.org/10.1016/j.apcata.2008.03.012},
   Abstract = {The reaction mechanism of reducing NOx with hydrocarbons
             over Ag/Al2O3 has been examined to improve its NOx reduction
             performance at lower temperatures, using ethanol and
             n-octane as representative hydrocarbon reductants. Based on
             the results obtained at the early stages of the hydrocarbon
             oxidation and NO reduction, it is proposed that the partial
             oxidation of hydrocarbons and the oxidation of NO are the
             first reaction steps over Ag/Al2O3. n-Octane is broken up
             into smaller hydrocarbon molecules, which are then
             subsequently oxidized to form various aldehydes, while
             ethanol is also rapidly converted to acetaldehyde. At the
             same time, NO is oxidized effectively to NO2 in the presence
             of reductants. These observations and additional experiments
             with variable amounts of Al2O3 placed downstream of the
             Ag/Al2O3 catalyst suggest that the NO reduction by
             hydrocarbons over Ag/Al2O3 may occur via a bifunctional
             reaction mechanism; NO and hydrocarbons are converted into
             NO2 and more reactive hydrocarbon species (i.e., smaller
             alkenes, oxygenated hydrocarbons), respectively, over the Ag
             sites, while N2 is produced from the subsequent reactions
             between these intermediate species over different sites
             including Al2O3. The proposed bifunctional reaction
             mechanism offers an opportunity to improve the overall NOx
             reduction performance of Ag/Al2O3 by optimizing individual
             reaction steps separately. Thus, the concept of a staged
             catalyst system has been examined using Ag/Al2O3 for the
             formation of reaction intermediates, and a secondary
             catalyst (e.g., Al2O3 or BaY) for the subsequent N2
             production reaction. Significant improvement in NOx
             reduction to N2 was obtained at lower temperatures, when BaY
             was used as the second catalyst and ethanol was used as
             reductant. © 2008 Elsevier B.V. All rights
             reserved.},
   Doi = {10.1016/j.apcata.2008.03.012},
   Key = {fds309485}
}

@article{fds153306,
   Author = {Aaltonen, T. et al},
   Title = {Search for large extra dimensions in final states containing
             one photon and large missing Et},
   Journal = {PRL 101},
   Year = {2008},
   Key = {fds153306}
}

@article{fds153307,
   Author = {Aaltonen, T. et al},
   Title = {Strong Evidence of ZZ production},
   Journal = {PRL 100},
   Year = {2008},
   Key = {fds153307}
}

@article{fds336991,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
             A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {Measurement of the cross section for W-boson production in
             association with jets in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {77},
   Number = {1},
   Year = {2008},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.011108},
   Abstract = {We present a measurement of the cross section for W-boson
             production in association with jets in pp̄ collisions at
             s=1.96TeV. The analysis uses a data sample corresponding to
             an integrated luminosity of 320pb-1 collected with the CDF
             II detector. W bosons are identified in their electron decay
             channel and jets are reconstructed using a cone algorithm.
             For each W+≥n-jet sample (n=1-4) we measure the
             differential cross section dσ(pp̄→W+≥
             n-jet)/dETnth-jet×B(W→eν) with respect to the transverse
             energy ET of the nth-highest ET jet above 20GeV, and the
             total cross section σ(pp̄→W+≥n-jet;ETnth-jet>25GeV)×B(W→eν),
             for a restricted W→eν decay phase space. The cross
             sections, corrected for all detector effects, can be
             directly compared to particle level W+jet(s) predictions. We
             present here comparisons to leading order and
             next-to-leading order predictions. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.77.011108},
   Key = {fds336991}
}

@article{fds309452,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
             Lorenzo, G and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
             Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
             J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
             W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
             K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci,
             C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak,
             R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Mangano, ML and Manousakis, A and Margaroli, F and Marino,
             C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
             M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso,
             S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
             V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
             O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
             A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
             M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A},
   Title = {First measurement of W boson production in association with
             a single Charm quark in pp collisions at sqrt(s)=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {100},
   Number = {9},
   Pages = {091803},
   Year = {2008},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.100.091803},
   Abstract = {We present the first measurement of the production cross
             section of a W boson with a single charm quark (c) in pp
             collisions at sqrt(s)=1.96 TeV, using soft muon tagging of c
             jets. In a data sample of approximately 1.8 fb(-1), recorded
             with the Collider Detector at Fermilab II detector at the
             Fermilab Tevatron, we select events with W+1 or 2 jets. We
             use the charge correlation between the W and the muon from
             the semileptonic decay of a charm hadron to extract the Wc
             signal. We measure sigma Wc(PTc >20 GeV/c,|eta c|<1.5) x
             BR(W-->l nu)=9.8+/-3.2 pb, in agreement with theoretical
             expectations.},
   Doi = {10.1103/physrevlett.100.091803},
   Key = {fds309452}
}

@article{fds309470,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
             Lorenzo, G and Dell'orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
             Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
             J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
             V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
             W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
             K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
             J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
             C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marino, C and Marino, CP and Martin,
             A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello,
             M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
             J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna,
             G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria,
             A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J},
   Title = {Search for Bs0 --> micro+ micro- and B0 --> micro+ micro-
             decays with 2 fb-1 of pp collisions.},
   Journal = {Physical review letters},
   Volume = {100},
   Number = {10},
   Pages = {101802},
   Year = {2008},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.100.101802},
   Abstract = {We have performed a search for B(s)(0) --> micro(+) micro(-)
             and B(0) --> micro(+) micro(-) decays in pp collisions at
             square root s = 1.96 TeV using 2 fb(-1) of integrated
             luminosity collected by the CDF II detector at the Fermilab
             Tevatron Collider. The observed number of B(s)(0) and B0
             candidates is consistent with background expectations. The
             resulting upper limits on the branching fractions are
             B(B(s)0) --> micro(+) micro(-)) <5.8 x 10(-8) and B(B(0) -->
             micro(+) micro(-))<1.8 x 10(-8) at 95% C.L.},
   Doi = {10.1103/physrevlett.100.101802},
   Key = {fds309470}
}

@article{fds309461,
   Author = {Aaltonen, T and Abulencia, A and Adelman, J and Akimoto, T and Albrow,
             MG and Álvarez González, B and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli,
             F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci,
             MA},
   Title = {First run II measurement of the W boson mass at the Fermilab
             Tevatron},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {77},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.77.112001},
   Abstract = {We describe a measurement of the W boson mass mW using
             200pb-1 of s=1.96TeV pp̄ collision data taken with the CDF
             II detector. With a sample of 63964 W→eν candidates and
             51128 W→μν candidates, we measure mW=[80.413±0.034(stat)±0.034(sys)=80.413±0.048]GeV/c2.
             This is the single most precise mW measurement to date. When
             combined with other measured electroweak parameters, this
             result further constrains the properties of new unobserved
             particles coupling to W and Z bosons. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.77.112001},
   Key = {fds309461}
}

@article{fds313348,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
             M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
   Title = {Search for standard model Higgs boson production in
             association with a W boson at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {78},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {August},
   ISSN = {1550-7998},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000258975300012&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We present a search for standard model Higgs boson
             production in association with a W boson in
             proton-antiproton collisions (pp̄→ W±H→ νbb̄) at a
             center of mass energy of 1.96 TeV. The search employs data
             collected with the CDF II detector which correspond to an
             integrated luminosity of approximately 1fb-1. We select
             events consistent with a signature of a single lepton
             (e±/μ±), missing transverse energy, and two jets. Jets
             corresponding to bottom quarks are identified with a
             secondary vertex tagging method and a neural network filter
             technique. The observed number of events and the dijet mass
             distributions are consistent with the standard model
             background expectations, and we set 95% confidence level
             upper limits on the production cross section times branching
             ratio ranging from 3.9 to 1.3 pb for Higgs boson masses from
             110 to 150GeV/c2, respectively. © 2008 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.78.032008},
   Key = {fds313348}
}

@article{fds309464,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {Erratum: Search for pair production of scalar top quarks
             decaying to a τ Lepton and a b quark in pp̄ collisions at
             s=1.96TeV (Physical Review Letters (2008) 101
             (071802))},
   Journal = {Physical Review Letters},
   Volume = {101},
   Number = {8},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.101.089901},
   Doi = {10.1103/PhysRevLett.101.089901},
   Key = {fds309464}
}

@article{fds309473,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {First measurement of the fraction of top-quark pair
             production through gluon-gluon fusion},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {78},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2008},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.78.111101},
   Abstract = {We present the first measurement of σ(gg→tt̄)/
             σ(pp̄→tt̄). We use 0.96fb-1 of s=1.96TeV pp̄ collision
             data recorded with the CDF II detector at Fermilab. Using
             charged particles with low transverse momentum in tt̄
             events, we find σ(gg→ tt̄)/σ(pp̄→tt̄)=0.07±0.14(stat)±0.
             07(syst), corresponding to a 95% confidence level upper
             limit of 0.33, in agreement with the standard model
             next-to-leading-order prediction of 0.15±0.05. © 2008 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.78.111101},
   Key = {fds309473}
}

@article{fds309481,
   Author = {Abat, E and Addy, TN and Åkesson, TPA and Alison, J and Anghinolfi, F and Arik, E and Arik, M and Atoian, G and Auerbach, B and Baker, OK and Banas,
             E and Baron, S and Bault, C and Becerici, N and Beddall, A and Beddall, AJ and Bendotti, J and Benjamin, DP and Bertelsen, H and Bingul, A and Blampey,
             H and Bocci, A and Bochenek, M and Bondarenko, VG and Bychkov, V and Callahan, J and Capeáns Garrido and M and Cardiel Sas and L and Catinaccio, A and Cetin, SA and Chandler, T and Chritin, R and Cwetanski, P and Dam, M and Danielsson, H and Danilevich, E and David,
             E and Degenhardt, J and Di Girolamo and B and Dittus, F and Dixon, N and Dogan, OB and Dolgoshein, BA and Dressnandt, N and Driouchi, C and Ebenstein, WL and Eerola, P and Egede, U and Egorov, K and Evans, H and Farthouat, P and Fedin, OL and Fowler, AJ and Fratina, S and Froidevaux,
             D and Fry, A and Gagnon, P and Gavrilenko, IL and Gay, C and Ghodbane, N and Godlewski, J and Goulette, M and Gousakov, I and Grigalashvili, N and Grishkevich, Y and Grognuz, J and Hajduk, Z and Hance, M and Hansen, F and Hansen, JB and Hansen, PH and Hanson, G and Hare, GA and Harvey, A and Hauviller, C and High, A and Hulsbergen, W and Huta, W and Issakov, V and Istin, S and Jain, V and Jarlskog, G and Jeanty, L and Kantserov, VA and Kaplan, B and Kapliy, AS and Katounine, S and Kayumov, F and Keener, PT and Kekelidze, GD and Khabarova, E and Khristachev, A and Kisielewski, B and Kittelmann, TH and Kline, C and Klinkby, EB and Klopov, NV and Ko, BR and Koffas, T and Kondratieva, NV},
   Title = {The ATLAS TRT barrel detector},
   Journal = {Journal of Instrumentation},
   Volume = {3},
   Number = {2},
   Pages = {P02014-P02014},
   Publisher = {IOP Publishing},
   Year = {2008},
   Month = {December},
   url = {http://dx.doi.org/10.1088/1748-0221/3/02/P02014},
   Abstract = {The ATLAS TRT barrel is a tracking drift chamber using
             52,544 individual tubular drift tubes. It is one part of the
             ATLAS Inner Detector, which consists of three sub-systems:
             the pixel detector spanning the radius range 4 to 20 cm, the
             semiconductor tracker (SCT) from 30 to 52 cm, and the
             transition radiation tracker (TRT) from 56 to 108 cm. The
             TRT barrel covers the central pseudo-rapidity region |η| 1,
             and the TRT while endcaps cover the forward and backward eta
             regions. These TRT systems provide a combination of
             continuous tracking with many measurements in individual
             drift tubes (or straws) and of electron identification based
             on transition radiation from fibers or foils interleaved
             between the straws themselves. This paper describes the
             recently-completed construction of the TRT Barrel detector,
             including the quality control procedures used in the
             fabrication of the detector. © 2008 IOP Publishing Ltd and
             SISSA.},
   Doi = {10.1088/1748-0221/3/02/P02014},
   Key = {fds309481}
}

@article{fds309482,
   Author = {Abat, E and Addy, TN and Åkesson, TPA and Alison, J and Anghinolfi, F and Arik, E and Arik, M and Atoian, G and Auerbach, B and Baker, OK and Banas,
             E and Baron, S and Bault, C and Becerici, N and Beddall, A and Beddall, AJ and Bendotti, J and Benjamin, DP and Bertelsen, H and Bingul, A and Blampey,
             H and Bocci, A and Bochenek, M and Bondarenko, VG and Bychkov, V and Callahan, J and Capeáns Garrido and M and Cardiel Sas and L and Catinaccio, A and Cetin, SA and Chandler, T and Chritin, R and Cwetanski, P and Dam, M and Danielsson, H and Danilevich, E and David,
             E and Degenhardt, J and Di Girolamo and B and Dittus, F and Dixon, N and Dogan, OB and Dolgoshein, BA and Dressnandt, N and Driouchi, C and Ebenstein, WL and Eerola, P and Egede, U and Egorov, K and Evans, H and Farthouat, P and Fedin, OL and Fowler, AJ and Fratina, S and Froidevaux,
             D and Fry, A and Gagnon, P and Gavrilenko, IL and Gay, C and Ghodbane, N and Godlewski, J and Goulette, M and Gousakov, I and Grigalashvili, N and Grishkevich, Y and Grognuz, J and Hajduk, Z and Hance, M and Hansen, F and Hansen, JB and Hansen, PH and Hare, GA and Harvey, A and Hauviller, C and High, A and Hulsbergen, W and Huta, W and Issakov, V and Istin, S and Jain,
             V and Jarlskog, G and Jeanty, L and Kantserov, VA and Kaplan, B and Kapliy,
             AS and Katounine, S and Kayumov, F and Keener, PT and Kekelidze, GD and Khabarova, E and Khristachev, A and Kisielewski, B and Kittelmann,
             TH and Kline, C and Klinkby, EB and Klopov, NV and Ko, BR and Koffas, T and Kondratieva, NV and Konovalov, SP},
   Title = {The ATLAS Transition Radiation Tracker (TRT) proportional
             drift tube: Design and performance},
   Journal = {Journal of Instrumentation},
   Volume = {3},
   Number = {2},
   Pages = {P02013-P02013},
   Publisher = {IOP Publishing},
   Year = {2008},
   Month = {December},
   url = {http://dx.doi.org/10.1088/1748-0221/3/02/P02013},
   Abstract = {A straw proportional counter is the basic element of the
             ATLAS Transition Radiation Tracker (TRT). Its detailed
             properties as well as the main properties of a few TRT
             operating gas mixtures are described. Particular attention
             is paid to straw tube performance in high radiation
             conditions and to its operational stability. © 2008 IOP
             Publishing Ltd and SISSA.},
   Doi = {10.1088/1748-0221/3/02/P02013},
   Key = {fds309482}
}

@article{fds361226,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BÁ and Amerio,
             S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
             D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
             BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
             J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
             M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
             RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
             J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
             DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens,
             P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
             T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
             MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia,
             E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks,
             B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus,
             C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt,
             M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer,
             B},
   Title = {First measurement of the tt̄ differential cross section
             dσ/dMtt̄ in pp̄ collisions at s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {102},
   Number = {22},
   Pages = {222003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevLett.102.222003},
   Abstract = {We present a measurement of the tt̄ differential cross
             section with respect to the tt̄ invariant mass, dσ/dMtt̄,
             in pp̄ collisions at s=1.96TeV using an integrated
             luminosity of 2.7fb-1 collected by the CDF II experiment.
             The tt̄ invariant mass spectrum is sensitive to a variety
             of exotic particles decaying into tt̄ pairs. The result is
             consistent with the standard model expectation, as modeled
             by PYTHIA with CTEQ5L parton distribution functions. © 2009
             The American Physical Society.},
   Doi = {10.1103/PhysRevLett.102.222003},
   Key = {fds361226}
}

@article{fds309107,
   Author = {Aaltonen, T and others},
   Title = {Observation of Exclusive Charmonium Production and
             γγ→μ+μ- in pp̅ Collisions at sqrt[s] =1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {24},
   Pages = {242001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.108.081801},
   Abstract = {In CDF we have observed the reactions p+p̅ →p+X+p̅ ,
             with X being a centrally produced J/ψ, ψ(2S), or χc0, and
             γγ→μ+μ- in pp̅ collisions at sqrt[s]=1.96  TeV.
             The event signature requires two oppositely charged central
             muons, and either no other particles or one additional
             photon detected. Exclusive vector meson production is as
             expected for elastic photoproduction, γ+p→J/ψ(ψ(2S))+p,
             observed here for the first time in hadron-hadron
             collisions. We also observe exclusive χc0→J/ψ+γ. The
             cross sections dσ / dy|y=0 for J/ψ, ψ(2S), and χc0 are
             3.92 &plusmn; 0.25(stat) &plusmn; 0.52(syst)  nb, 0.53
             &plusmn; 0.09(stat) &plusmn; 0.10(syst)  nb, and 76
             &plusmn; 10(stat) &plusmn; 10(syst)  nb, respectively,
             and the continuum is consistent with QED. We put an upper
             limit on the cross section for Odderon exchange in exclusive
             J/ψ production.},
   Doi = {10.1103/physrevlett.108.081801},
   Key = {fds309107}
}

@article{fds321463,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
             M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson,
             R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro,
             PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler,
             A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
             D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
             RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori,
             M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck,
             J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
             A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
             K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn,
             F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi,
             G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle,
             T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
             AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi,
             S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith,
             JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B},
   Title = {Measurement of the fraction of tt̄ production via
             gluon-gluon fusion in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {3},
   Pages = {031101},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.031101},
   Abstract = {We present a measurement of the ratio of the tt̄ production
             cross section via gluon-gluon fusion to the total tt̄
             production cross section in pp̄ collisions at s=1.96TeV at
             the Tevatron. Using a data sample with an integrated
             luminosity of 955pb-1 recorded by the CDF II detector at
             Fermilab, we select events based on the tt̄ decay to
             lepton+jets. Using an artificial neural network technique we
             discriminate between tt̄ events produced via qq̄
             annihilation and gg fusion, and find Gf=σ(gg→tt̄)/
             σ(pp̄→tt̄)&lt;0.33 at the 68% confidence level. This
             result is combined with a previous measurement to obtain the
             most stringent measurement of this quantity by CDF to date,
             Gf=0.07-0.07+0.15. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.031101},
   Key = {fds321463}
}

@article{fds309374,
   Author = {Aaltonen, T and others},
   Title = {Search for the Associated Production of the Standard-Model
             Higgs Boson in the All-Hadronic Channel},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {22},
   Pages = {221801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.221801},
   Abstract = {We report on a search for the standard-model Higgs boson in
             pp̅ collisions at sqrt[s]=1.96  TeV using an integrated
             luminosity of 2.0  fb-1. We look for production of the
             Higgs boson decaying to a pair of bottom quarks in
             association with a vector boson V (W or Z) decaying to
             quarks, resulting in a four-jet final state. Two of the jets
             are required to have secondary vertices consistent with
             B-hadron decays. We set the first 95% confidence level upper
             limit on the VH production cross section with V(→qq̅
             /qq′)H(→bb̅ ) decay for Higgs boson masses of
             100--150  GeV/c2 using data from run II at the Fermilab
             Tevatron. For mH=120  GeV/c2, we exclude cross sections
             larger than 38 times the standard-model prediction.},
   Doi = {10.1103/physrevlett.103.221801},
   Key = {fds309374}
}

@article{fds309375,
   Author = {Aaltonen, T and others},
   Title = {Search for Higgs Bosons Predicted in Two-Higgs-Doublet
             Models via Decays to Tau Lepton Pairs in 1.96 TeV pp̅
             Collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {20},
   Pages = {201801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.201801},
   Abstract = {We present the results of a search for Higgs bosons
             predicted in two-Higgs-doublet models, in the case where the
             Higgs bosons decay to tau lepton pairs, using 1.8  fb-1
             of integrated luminosity of pp̅ collisions recorded by the
             CDF II experiment at the Fermilab Tevatron. Studying the
             mass distribution in events where one or both tau leptons
             decay leptonically, no evidence for a Higgs boson signal is
             observed. The result is used to infer exclusion limits in
             the two-dimensional space of tan⁡β versus mA (the ratio
             of the vacuum expectation values of the two Higgs doublets
             and the mass of the pseudoscalar boson, respectively).},
   Doi = {10.1103/physrevlett.103.201801},
   Key = {fds309375}
}

@article{fds309376,
   Author = {Aaltonen, T and others},
   Title = {First Observation of B̅ s0→Ds ± K∓ and
             Measurement of the Ratio of Branching Fractions B(B̅
             s0→Ds ± K∓)/B(B̅ s0→Ds+π-)},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {19},
   Pages = {191802},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.191802},
   Abstract = {A combined mass and particle identification fit is used to
             make the first observation of the decay B̅ s0→Ds &plusmn;
             K∓ and measure the branching fraction of B̅ s0→Ds
             &plusmn; K∓ relative to B̅ s0→Ds+π-. This analysis
             uses 1.2  fb-1 integrated luminosity of pp̅ collisions
             at sqrt[s]=1.96  TeV collected with the CDF II detector
             at the Fermilab Tevatron collider. We observe a B̅ s0→Ds
             &plusmn; K∓ signal with a statistical significance of
             8.1σ and measure B(B̅ s0→Ds &plusmn; K∓)/B(B̅
             s0→Ds+π-)=0.097 &plusmn; 0.018(stat) &plusmn;
             0.009(syst).},
   Doi = {10.1103/physrevlett.103.191802},
   Key = {fds309376}
}

@article{fds309377,
   Author = {Aaltonen, T and others},
   Title = {Precision Measurement of the Ξ(3872) Mass in J/ψ π
             + π- Decays},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {15},
   Pages = {152001},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.152001},
   Abstract = {We present an analysis of the mass of the X(3872)
             reconstructed via its decay to J/ψπ+π- using
             2.4  fb-1 of integrated luminosity from pp̅ collisions
             at sqrt[s]=1.96  TeV, collected with the CDF II detector
             at the Fermilab Tevatron. The possible existence of two
             nearby mass states is investigated. Within the limits of our
             experimental resolution the data are consistent with a
             single state, and having no evidence for two states we set
             upper limits on the mass difference between two hypothetical
             states for different assumed ratios of contributions to the
             observed peak. For equal contributions, the 95% confidence
             level upper limit on the mass difference is 3.6  MeV/c2.
             Under the single-state model the X(3872) mass is measured to
             be 3871.61 &plusmn; 0.16(stat) &plusmn; 0.19(syst)  MeV/c2,
             which is the most precise determination to
             date.},
   Doi = {10.1103/physrevlett.103.152001},
   Key = {fds309377}
}

@article{fds309378,
   Author = {Aaltonen, T and others},
   Title = {Search for a Standard Model Higgs Boson in WH→ℓvbb̅ in
             pp̅ Collisions at sqrt[s] =1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {10},
   Pages = {101802},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.101802},
   Abstract = {We present a search for a standard model Higgs boson
             produced in association with a W boson using 2.7  fb-1
             of integrated luminosity of pp̅ collision data taken at
             sqrt[s]=1.96  TeV. Limits on the Higgs boson production
             rate are obtained for masses between 100 and
             150  GeV/c2. Through the use of multivariate techniques,
             the analysis achieves an observed (expected) 95% confidence
             level upper limit of 5.6 (4.8) times the theoretically
             expected production cross section for a standard model Higgs
             boson with a mass of 115  GeV/c2.},
   Doi = {10.1103/physrevlett.103.101802},
   Key = {fds309378}
}

@article{fds309379,
   Author = {Aaltonen, T and others},
   Title = {Search for Charged Higgs Bosons in Decays of Top Quarks in
             pp̅ Collisions at sqrt[s] =1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {10},
   Pages = {101803},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.101803},
   Abstract = {We report on the first direct search for charged Higgs
             bosons decaying into cs̅ in tt̅ events produced by pp̅
             collisions at sqrt[s]=1.96  TeV. The search uses a data
             sample corresponding to an integrated luminosity of
             2.2  fb-1 collected by the CDF II detector at Fermilab
             and looks for a resonance in the invariant mass distribution
             of two jets in the lepton+jets sample of tt̅ candidates. We
             observe no evidence of charged Higgs bosons in top quark
             decays. Hence, 95% upper limits on the top quark decay
             branching ratio are placed at B(t→H+b)&lt; 0.1 to 0.3 for
             charged Higgs boson masses of 60 to 150  GeV/c2 assuming
             B(H+→cs̅ )=1.0. The upper limits on B(t→H+b) are also
             used as model-independent limits on the decay branching
             ratio of top quarks to generic scalar charged bosons beyond
             the standard model.},
   Doi = {10.1103/physrevlett.103.101803},
   Key = {fds309379}
}

@article{fds309380,
   Author = {Aaltonen, T and others},
   Title = {First Observation of Vector Boson Pairs in a Hadronic Final
             State at the Tevatron Collider},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {9},
   Pages = {091803},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.091803},
   Abstract = {We present the first observation in hadronic collisions of
             the electroweak production of vector boson pairs (VV, V=W,
             Z) where one boson decays to a dijet final state. The data
             correspond to 3.5  fb-1 of integrated luminosity of pp̅
             collisions at sqrt[s]=1.96  TeV collected by the CDF II
             detector at the Fermilab Tevatron. We observe 1516 &plusmn;
             239(stat) &plusmn; 144(syst) diboson candidate events and
             measure a cross section σ(pp̅ →VV+X) of 18.0 &plusmn;
             2.8(stat) &plusmn; 2.4(syst) &plusmn; 1.1(lumi)  pb, in
             agreement with the expectations of the standard
             model.},
   Doi = {10.1103/physrevlett.103.091803},
   Key = {fds309380}
}

@article{fds309381,
   Author = {Aaltonen, T and others},
   Title = {Observation of Electroweak Single Top-Quark
             Production},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {9},
   Pages = {092002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.092002},
   Abstract = {We report the observation of single top-quark production
             using 3.2  fb-1 of pp̅ collision data with
             sqrt[s]=1.96  TeV collected by the Collider Detector at
             Fermilab. The significance of the observed data is 5.0
             standard deviations, and the expected sensitivity for
             standard model production and decay is in excess of 5.9
             standard deviations. Assuming mt=175  GeV/c2, we measure
             a cross section of 2.3-0.5+0.6(stat+syst)  pb, extract
             the CKM matrix-element value |Vtb|=0.91 &plusmn;
             0.11(stat+syst) &plusmn; 0.07(theory), and set the limit
             |Vtb|&gt;0.71 at the 95% C.L.},
   Doi = {10.1103/physrevlett.103.092002},
   Key = {fds309381}
}

@article{fds309382,
   Author = {Aaltonen, T and others},
   Title = {Search for a Fermiophobic Higgs Boson Decaying into
             Diphotons in pp̅ Collisions at sqrt[s]=1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {6},
   Pages = {061803},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.061803},
   Abstract = {A search for a narrow diphoton mass resonance is presented
             based on data from 3.0  fb-1 of integrated luminosity
             from pp̅ collisions at sqrt[s]=1.96  TeV collected by
             the CDF experiment. No evidence of a resonance in the
             diphoton mass spectrum is observed, and upper limits are set
             on the cross section times branching fraction of the
             resonant state as a function of Higgs boson mass. The
             resulting limits exclude Higgs bosons with masses below
             106  GeV/c2 at a 95% Bayesian credibility level for one
             fermiophobic benchmark model.},
   Doi = {10.1103/physrevlett.103.061803},
   Key = {fds309382}
}

@article{fds309383,
   Author = {Aaltonen, T and others},
   Title = {Search for the Production of Narrow tb̅ Resonances in 1.9
             fb-1 of pp̅ Collisions at sqrt[s] =1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {4},
   Pages = {041801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.041801},
   Abstract = {We present new limits on resonant tb̅ production in pp̅
             collisions at sqrt[s]=1.96  TeV, using 1.9  fb-1 of
             data recorded with the CDF II detector at the Fermilab
             Tevatron. We reconstruct a candidate tb̅ mass in events
             with a lepton, neutrino candidate, and two or three jets,
             and search for anomalous tb̅ production as modeled by
             W′→tb̅ . We set a new limit on a right-handed W′ with
             standard model-like coupling, excluding any mass below
             800  GeV/c2 at 95% C.L. The cross section for any
             narrow, resonant tb̅ production between 750 and
             950  GeV/c2 is found to be less than 0.28 pb at 95% C.L.
             We also present an exclusion of the W′ coupling strength
             versus W′ mass over the range 300--950  GeV/c2.},
   Doi = {10.1103/physrevlett.103.041801},
   Key = {fds309383}
}

@article{fds309384,
   Author = {Aaltonen, T and others},
   Title = {Observation of New Charmless Decays of Bottom
             Hadrons},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {3},
   Pages = {031801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.031801},
   Abstract = {We search for new charmless decays of neutral b hadrons to
             pairs of charged hadrons, using 1  fb-1 of data
             collected by the CDF II detector at the Fermilab Tevatron.
             We report the first observation of the Bs0→K-π+ decay and
             measure B(Bs0→K-π+)=(5.0 &plusmn; 0.7(stat) &plusmn;
             0.8(syst))×10-6. We also report the first observation of
             charmless b-baryon decays, and measure B(Λb0→pπ-)=(3.5
             &plusmn; 0.6(stat) &plusmn; 0.9(syst))×10-6 and
             B(Λb0→pK-)=(5.6 &plusmn; 0.8(stat) &plusmn;
             1.5(syst))×10-6. No evidence is found for other modes, and
             we set the limit B(Bs0→π+π-)&lt;1.2×10-6 at 90%
             C.L.},
   Doi = {10.1103/physrevlett.103.031801},
   Key = {fds309384}
}

@article{fds309385,
   Author = {Aaltonen, T and others},
   Title = {Search for Long-Lived Massive Charged Particles in 1.96 TeV
             pp̅ Collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {103},
   Number = {2},
   Pages = {021802},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.103.021802},
   Abstract = {We performed a signature-based search for long-lived charged
             massive particles produced in 1.0  fb-1 of pp̅
             collisions at sqrt[s]=1.96  TeV, collected with the CDF
             II detector using a high transverse-momentum (pT) muon
             trigger. The search used time of flight to isolate slowly
             moving, high-pT particles. One event passed our selection
             cuts with an expected background of 1.9 &plusmn; 0.2 events.
             We set an upper bound on the production cross section and,
             interpreting this result within the context of a stable
             scalar top-quark model, set a lower limit on the particle
             mass of 249  GeV/c2 at 95% C.L.},
   Doi = {10.1103/physrevlett.103.021802},
   Key = {fds309385}
}

@article{fds309386,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the k[sub T] Distribution of Particles in
             Jets Produced in p[overline p] Collisions at sqrt(s) = 1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {23},
   Pages = {232002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.232002},
   Abstract = {We present a measurement of the transverse momentum with
             respect to the jet axis (k(t)) of particles in jets produced
             in pp collisions at sqrt(s)=1.96 TeV. Results are obtained
             for charged particles in a cone of 0.5 radians around the
             jet axis in events with dijet invariant masses between 66
             and 737 GeV/c(2). The experimental data are compared to
             theoretical predictions obtained for fragmentation partons
             within the framework of resummed perturbative QCD using the
             modified leading log and next-to-modified leading log
             approximations. The comparison shows that trends in data are
             successfully described by the theoretical predictions,
             indicating that the perturbative QCD stage of jet
             fragmentation is dominant in shaping basic jet
             characteristics.},
   Doi = {10.1103/physrevlett.102.232002},
   Key = {fds309386}
}

@article{fds309387,
   Author = {Aaltonen, T and others},
   Title = {Search for Gluino-Mediated Bottom Squark Production in
             p[overline p] Collisions at sqrt(s) = 1.96
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {22},
   Pages = {221801},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.221801},
   Abstract = {We report on a search for the supersymmetric partner of the
             bottom quark produced from gluino decays in data from 2.5
             fb;{-1} of integrated luminosity collected by the Collider
             Detector at Fermilab at sqrt[s]=1.96 TeV. Candidate events
             are selected requiring two or more jets and large missing
             transverse energy. At least two of the jets are required to
             be tagged as originating from a b quark to enhance the
             sensitivity. The results are in good agreement with the
             prediction of the standard model processes, giving no
             evidence for gluino decay to bottom squarks. This result
             constrains the gluino-pair-production cross section to be
             less than 40 fb at 95% credibility level for a gluino mass
             of 350 GeV/c;{2}.},
   Doi = {10.1103/physrevlett.102.221801},
   Key = {fds309387}
}

@article{fds309389,
   Author = {Aaltonen, T and others},
   Title = {Direct Measurement of the W Production Charge Asymmetry in
             pp̅ Collisions at sqrt[s] =1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {18},
   Pages = {181801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.181801},
   Abstract = {We present the first direct measurement of the W production
             charge asymmetry as a function of the W boson rapidity yW in
             pp̅ collisions at sqrt[s]=1.96  TeV. We use a sample of
             W→eν events in data from 1  fb-1 of integrated
             luminosity collected using the CDF II detector. In the
             region |yW|&lt;3.0, this measurement is capable of
             constraining the ratio of up- and down-quark momentum
             distributions in the proton more directly than in previous
             measurements of the asymmetry that are functions of the
             charged-lepton pseudorapidity.},
   Doi = {10.1103/physrevlett.102.181801},
   Key = {fds309389}
}

@article{fds309390,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the Top-Quark Mass with Dilepton Events
             Selected Using Neuroevolution at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {15},
   Pages = {152001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.152001},
   Abstract = {We present an analysis of the mass of the X(3872)
             reconstructed via its decay to J/ψπ+π- using
             2.4  fb-1 of integrated luminosity from pp̅ collisions
             at sqrt[s]=1.96  TeV, collected with the CDF II detector
             at the Fermilab Tevatron. The possible existence of two
             nearby mass states is investigated. Within the limits of our
             experimental resolution the data are consistent with a
             single state, and having no evidence for two states we set
             upper limits on the mass difference between two hypothetical
             states for different assumed ratios of contributions to the
             observed peak. For equal contributions, the 95% confidence
             level upper limit on the mass difference is 3.6  MeV/c2.
             Under the single-state model the X(3872) mass is measured to
             be 3871.61$\pm$0.16(stat)$\pm$0.19(syst)  MeV/c2, which
             is the most precise determination to date.},
   Doi = {10.1103/physrevlett.102.152001},
   Key = {fds309390}
}

@article{fds309391,
   Author = {Aaltonen, T and others},
   Title = {Search for Top-Quark Production via Flavor-Changing Neutral
             Currents in W + 1 Jet Events at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {15},
   Pages = {151801},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.151801},
   Abstract = {We report on a search for the non-standard-model process
             u(c) + g --> t using pp[over ] collision data collected by
             the Collider Detector at Fermilab II detector corresponding
             to 2.2 fb;{-1}. The candidate events are classified as
             signal-like or backgroundlike by an artificial neural
             network. The observed discriminant distribution yields no
             evidence for flavor-changing neutral current top-quark
             production, resulting in an upper limit on the production
             cross section sigma(u(c) + g --> t) < 1.8 pb at the 95% C.L.
             Using theoretical predictions we convert the cross section
             limit to upper limits on flavor-changing neutral current
             branching ratios: B(t --> u + g) < 3.9 x 10;{-4} and B(t -->
             c + g) < 5.7 x 10;{-3}.},
   Doi = {10.1103/physrevlett.102.151801},
   Key = {fds309391}
}

@article{fds309393,
   Author = {Aaltonen, T and others},
   Title = {Measurement of Resonance Parameters of Orbitally Excited
             Narrow B[sup 0] Mesons},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {10},
   Pages = {102003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.102003},
   Abstract = {We report a measurement of resonance parameters of the
             orbitally excited (L=1) narrow B0 mesons in decays to
             B;{(*)+}pi;{-} using 1.7 fb;{-1} of data collected by the
             CDF II detector at the Fermilab Tevatron. The mass and width
             of the B_{2};{*0} state are measured to be
             m(B_{2};{*0})=5740.2_{-1.8};{+1.7}(stat)-0.8+0.9(syst)
             MeV/c;{2} and Gamma(B_{2};{*0})=22.7_{-3.2};{+3.8}(stat)-10.2+3.2(syst)
             MeV/c;{2}. The mass difference between the B_{2};{*0} and
             B10 states is measured to be 14.9_{-2.5};{+2.2}(stat)-1.4+1.2(syst)
             MeV/c;{2}, resulting in a B10 mass of 5725.3_{-2.2};{+1.6}(stat)-1.5+1.4(syst)
             MeV/c;{2}. This is currently the most precise measurement of
             the masses of these states and the first measurement of the
             B_{2};{*0} width.},
   Doi = {10.1103/physrevlett.102.102003},
   Key = {fds309393}
}

@article{fds309394,
   Author = {Aaltonen, T and others},
   Title = {Search for High-Mass Resonances Decaying to Dimuons at
             CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {9},
   Pages = {091805},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.091805},
   Abstract = {We present a search for high-mass neutral resonances using
             dimuon data corresponding to an integrated luminosity of 2.3
             fb(-1) collected in pp[over ] collisions at sqrt[s]=1.96 TeV
             by the CDF II detector at the Fermilab Tevatron. No
             significant excess above the standard model expectation is
             observed in the dimuon invariant-mass spectrum. We set 95%
             confidence level upper limits on sigmaBR(pp-->X-->micromicro),
             where X is a boson with spin-0, 1, or 2. Using these cross
             section limits, we determine lower mass limits on sneutrinos
             in R-parity-violating supersymmetric models, Z' bosons, and
             Kaluza-Klein gravitons in the Randall-Sundrum
             model.},
   Doi = {10.1103/physrevlett.102.091805},
   Key = {fds309394}
}

@article{fds309397,
   Author = {Aaltonen, T and others},
   Title = {Search for High-Mass e+e- Resonances in ppbar Collisions at
             1.96 TeV},
   Journal = {PRL},
   Volume = {102},
   Number = {3},
   Pages = {031801},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.031801},
   Abstract = {A search for high-mass resonances in the e+e- final state is
             presented based on 2.5 fb(-1) of sqrt[s]=1.96 TeV pp
             collision data from the CDF II detector at the Fermilab
             Tevatron. The largest excess over the standard model
             prediction is at an e+e- invariant mass of 240 GeV/c2. The
             probability of observing such an excess arising from
             fluctuations in the standard model anywhere in the mass
             range of 150-1000 GeV/c2 is 0.6% (equivalent to 2.5sigma).
             We exclude the standard model coupling Z' and the
             Randall-Sundrum graviton for k/MPl=0.1 with masses below 963
             and 848 GeV/c2 at the 95% credibility level,
             respectively.},
   Doi = {10.1103/physrevlett.102.031801},
   Key = {fds309397}
}

@article{fds309400,
   Author = {Aaltonen, T and others},
   Title = {Search for hadronic decays of W and Z bosons in photon
             events in pp̅ collisions at sqrt[s] =1.96
             TeV},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {052011},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.052011},
   Abstract = {We report on a search for the process pp̅ →γ+W/Z with
             W/Z→qq̅ in events containing two jets and a photon at the
             center-of-mass energy sqrt[s]=1.96  TeV, using
             184  pb-1 of data collected by the CDF II detector. A
             neural network event selection has been developed to
             optimize the rejection of the large QCD production
             background; it is shown that this method gives a significant
             improvement in both signal-to-noise ratio and signal
             sensitivity, as compared with an event selection based on
             conventional cuts. An upper limit is presented for the
             γ+W/Z production cross section with the W and Z decaying
             hadronically.},
   Doi = {10.1103/PhysRevD.80.052011},
   Key = {fds309400}
}

@article{fds309406,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
             D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
             BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
             J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
             C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
             M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
             RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
             KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
             PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
             AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
             MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
             G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
             MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
             FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
             J},
   Title = {First measurement of the ratio of branching fractions B(Λb
             0→Λc+μ-ν̄μ)/B(Λb 0→Λc+π-)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.032001},
   Abstract = {This article presents the first measurement of the ratio of
             branching fractions B(Λb0→Λc+μ-ν̄μ)/
             B(Λb0→Λc+π-). Measurements in two control samples using
             the same technique B(B̄0→D+μ- ν̄μ)/B(B̄0→D+π-)
             and B(B̄ 0→D*(2010)+μ-ν̄μ)/ B(B̄0→D*(2010)+π-)
             are also reported. The analysis uses data from an integrated
             luminosity of approximately 172pb-1 of pp̄ collisions at
             s=1.96TeV, collected with the CDF II detector at the
             Fermilab Tevatron. The relative branching fractions are
             measured to be B(Λb 0→Λc+μ-ν̄μ)B(Λb
             0→Λc+π-)=16.6±3.0(stat) ±1.0(syst)+2.6-3.4(PDG)
             ±0.3(EBR), B(B̄0→D+μ-ν̄μ) B(B̄0→D+π-)=9.9±1.0(stat)
             ±0.6(syst)±0.4(PDG)± 0.5(EBR), and B(B̄0→D*(
             2010)+μ-ν̄μ)B(B̄0→D*( 2010)+π-)=16.5±2.3(stat)
             ±0.6(syst)±0.5(PDG)± 0.8(EBR). The uncertainties are from
             statistics (stat), internal systematics (syst), world
             averages of measurements published by the Particle Data
             Group or subsidiary measurements in this analysis (PDG), and
             unmeasured branching fractions estimated from theory (EBR),
             respectively. This article also presents measurements of the
             branching fractions of four new Λb 0 semileptonic decays:
             Λb0→Λc( 2595)+μ-ν̄μ, Λb0→Λc( 2625)+μ-ν̄μ,
             Λb0→Σc( 2455)0π+μ-ν̄μ, and Λb 0→Σc(2455)++π-μ-ν̄μ,
             relative to the branching fraction of the Λb0→Λc+μ-
             ν̄μ decay. Finally, the transverse-momentum distribution
             of Λb0 baryons produced in pp̄ collisions is measured and
             found to be significantly different from that of B̄0
             mesons, which results in a modification in the production
             cross-section ratio σΛb0/σB̄0 with respect to the CDF I
             measurement. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.032001},
   Key = {fds309406}
}

@article{fds309407,
   Author = {Aaltonen, T and others},
   Title = {Search for new physics in the mu mu + e/mu + E-slash [sub T]
             channel with a low-p[sub T] lepton threshold at the Collider
             Detector at Fermilab},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {5},
   Pages = {052004},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.052004},
   Abstract = {A search for new physics using three-lepton (trilepton) data
             collected with the CDF II detector and corresponding to an
             integrated luminosity of 976 pb-1 is presented. The standard
             model predicts a low rate of trilepton events, which makes
             some supersymmetric processes, such as chargino-neutralino
             production, measurable in this channel. The μμ+ signature
             is investigated, where ℓ is an electron or a muon, with
             the additional requirement of large missing transverse
             energy. In this analysis, the lepton transverse momenta with
             respect to the beam direction (pT) are as low as 5GeV/c, a
             selection that improves the sensitivity to particles that
             are light as well as to ones that result in leptonically
             decaying tau leptons. At the same time, this low-pT
             selection presents additional challenges due to the
             non-negligible heavy-quark background at low lepton momenta.
             This background is measured with an innovative technique
             using experimental data. Several dimuon and trilepton
             control regions are investigated, and good agreement between
             experimental results and standard-model predictions is
             observed. In the signal region, we observe one three-muon
             event and expect 0.4±0.1μμ+ events from standard-model
             processes. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.052004},
   Key = {fds309407}
}

@article{fds309409,
   Author = {Aaltonen, T and others},
   Title = {First simultaneous measurement of the top quark mass in the
             lepton + jets and dilepton channels at CDF},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {9},
   Pages = {092005},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.092005},
   Abstract = {We present a measurement of the mass of the top quark using
             data corresponding to an integrated luminosity of 1.9fb-1 of
             pp̄ collisions collected at s=1.96TeV with the CDF II
             detector at Fermilab's Tevatron. This is the first
             measurement of the top quark mass using top-antitop pair
             candidate events in the lepton+jets and dilepton decay
             channels simultaneously. We reconstruct two observables in
             each channel and use a nonparametric kernel density
             estimation technique to derive two-dimensional probability
             density functions from simulated signal and background
             samples. The observables are the top quark mass and the
             invariant mass of two jets from the W decay in the
             lepton+jets channel, and the top quark mass and the scalar
             sum of transverse energy of the event in the dilepton
             channel. We perform a simultaneous fit for the top quark
             mass and the jet energy scale, which is constrained in situ
             by the hadronic W boson mass. Using 332 lepton+jets
             candidate events and 144 dilepton candidate events, we
             measure the top quark mass to be Mtop=171.9±1.
             7(stat+JES)±1.1(othersyst)GeV/c2=171.9±2.0GeV/c2. © 2009
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.092005},
   Key = {fds309409}
}

@article{fds309412,
   Author = {Aaltonen, T and others},
   Title = {Search for the neutral current top quark decay t→Zc using
             the ratio of Z-boson+4  jets to W-boson+4  jets
             production},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {052001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.052001},
   Abstract = {We have used the Collider Detector at Fermilab (CDF-II) to
             search for the flavor-changing neutral-current (FCNC)
             top-quark decay t→Zc using a technique employing ratios of
             W and Z production, measured in pp̅ data corresponding to
             an integrated luminosity of 1.52  fb-1. The analysis
             uses a comparison of two decay chains, pp̅ →tt̅
             →WbWb→ℓνbjjb and pp̅ →tt̅ →ZcWb→ℓℓcjjb,
             to cancel systematic uncertainties in acceptance,
             efficiency, and luminosity. We validate the modeling of
             acceptance and efficiency for lepton identification over the
             multiyear data set using another ratio of W and Z
             production, in this case the observed ratio of inclusive
             production of W to Z bosons. To improve the discrimination
             against standard model backgrounds to top-quark decays, we
             calculate the top-quark mass for each event with two leptons
             and four jets assuming it is a tt̅ event with one of the
             top quarks decaying to Zc. For additional background
             discrimination we require at least one jet to be identified
             as originating from a b quark. No significant signal is
             found and we set an upper limit on the FCNC branching ratio
             Br(t→Zc) using a likelihood constructed from the
             ℓℓcjjb top-quark mass distribution and the number of
             ℓνbjjb events. Limits are set as a function of the
             helicity of the Z boson produced in the FCNC decay. For 100%
             longitudinally-polarized Z bosons we find limits of 8.3% and
             9.3% (95% C.L.) depending on the assumptions regarding the
             theoretical top-quark pair production cross
             section.},
   Doi = {10.1103/PhysRevD.80.052001},
   Key = {fds309412}
}

@article{fds309413,
   Author = {Aaltonen, T and others},
   Title = {Search for anomalous production of events with a photon,
             jet, b-quark jet, and missing transverse
             energy},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {052003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.052003},
   Abstract = {We present a signature-based search for the anomalous
             production of events containing a photon, two jets, of which
             at least one is identified as originating from a b quark,
             and missing transverse energy (E̸T). The search uses data
             corresponding to 2.0  fb-1 of integrated luminosity from
             pp̅ collisions at a center-of-mass energy of
             sqrt[s]=1.96  TeV, collected with the CDF II detector at
             the Fermilab Tevatron. From 6.697 47×106 events with a
             photon candidate with transverse energy ET&gt;25  GeV,
             we find 617 events with E̸T&gt;25  GeV and two or more
             jets with ET&gt;15  GeV, at least one identified as
             originating from a b quark, versus an expectation of 607
             &plusmn; 113 events. Increasing the requirement on E̸T to
             50 GeV, we find 28 events versus an expectation of 30
             &plusmn; 11 events. We find no indications of
             non-standard-model phenomena.},
   Doi = {10.1103/PhysRevD.80.052003},
   Key = {fds309413}
}

@article{fds309414,
   Author = {Aaltonen, T and others},
   Title = {Top quark mass measurement in the tt̅ all hadronic channel
             using a matrix element technique in pp̅ collisions at
             sqrt[s] =1.96 TeV},
   Journal = {Physical Review D},
   Volume = {79},
   Number = {7},
   Pages = {072010},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.072010},
   Abstract = {We present a measurement of the top quark mass in the all
             hadronic channel (tt̅ →bb̅ q1q̅ 2q3q̅ 4) using
             943  pb-1 of pp̅ collisions at sqrt[s]=1.96  TeV
             collected at the CDF II detector at Fermilab (CDF). We apply
             the standard model production and decay matrix element (ME)
             to tt̅ candidate events. We calculate per-event probability
             densities according to the ME calculation and construct
             template models of signal and background. The scale of the
             jet energy is calibrated using additional templates formed
             with the invariant mass of pairs of jets. These templates
             form an overall likelihood function that depends on the top
             quark mass and on the jet energy scale (JES). We estimate
             both by maximizing this function. Given 72 observed events,
             we measure a top quark mass of 171.1 &plusmn; 3.7(stat+JES)
             &plusmn; 2.1(syst)  GeV/c2. The combined uncertainty on
             the top quark mass is 4.3  GeV/c2.},
   Doi = {10.1103/PhysRevD.79.072010},
   Key = {fds309414}
}

@article{fds309415,
   Author = {Aaltonen, T and others},
   Title = {Top quark mass measurement in the lepton plus jets channel
             using a modified matrix element method},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {7},
   Pages = {072001},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.072001},
   Abstract = {We report a measurement of the top quark mass, mt, obtained
             from pp̄ collisions at s=1.96TeV at the Fermilab Tevatron
             using the CDF II detector. We analyze a sample corresponding
             to an integrated luminosity of 1.9fb-1. We select events
             with an electron or muon, large missing transverse energy,
             and exactly four high-energy jets in the central region of
             the detector, at least one of which is tagged as coming from
             a b quark. We calculate a signal likelihood using a matrix
             element integration method, where the matrix element is
             modified by using effective propagators to take into account
             assumptions on event kinematics. Our event likelihood is a
             function of mt and a parameter JES (jet energy scale) that
             determines in situ the calibration of the jet energies. We
             use a neural network discriminant to distinguish signal from
             background events. We also apply a cut on the peak value of
             each event likelihood curve to reduce the contribution of
             background and badly reconstructed events. Using the 318
             events that pass all selection criteria, we find
             mt=172.7±1.8(stat+JES) ±1.2(syst)GeV/c2. © 2009 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.79.072001},
   Key = {fds309415}
}

@article{fds309416,
   Author = {Aaltonen, T and others},
   Title = {Search for new particles decaying into dijets in
             proton-antiproton collisions at sqrt(s) = 1.96
             TeV},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112002},
   Abstract = {We present a search for new particles which produce narrow
             two-jet (dijet) resonances using proton-antiproton collision
             data corresponding to an integrated luminosity of 1.13fb-1
             collected with the CDFA II detector. The measured dijet mass
             spectrum is found to be consistent with next-to-leading-order
             perturbative QCD predictions, and no significant evidence of
             new particles is found. We set upper limits at the 95%
             confidence level on cross sections times the branching
             fraction for the production of new particles decaying into
             dijets with both jets having a rapidity magnitude |y| <1.
             These limits are used to determine the mass exclusions for
             the excited quark, axigluon, flavor-universal coloron, E6
             diquark, color-octet techni-ρ, W′, and Z′. © 2009 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.79.112002},
   Key = {fds309416}
}

@article{fds309417,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the t[overline t] production cross section in
             2 fb[sup -1] of p[overline p] collisions at sqrt(s) = 1.96
             TeV using lepton plus jets events with soft muon b
             tagging},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {5},
   Pages = {052007},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.052007},
   Abstract = {We present a measurement of the tt̄ production cross
             section in pp̄ collisions at s=1.96TeV using events
             containing a high transverse momentum electron or muon,
             three or more jets, and missing transverse energy. Events
             consistent with tt̄ decay are found by identifying jets
             containing candidate heavy-flavor semileptonic decays to
             muons. The measurement uses a CDF run II data sample
             corresponding to 2fb-1 of integrated luminosity. Based on
             248 candidate events with three or more jets and an expected
             background of 79.5±5.3 events, we measure a production
             cross section of 9.1±1.6pb. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.052007},
   Key = {fds309417}
}

@article{fds309419,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the top quark mass at CDF using the
             ``neutrino phi weighting'' template method on a lepton plus
             isolated track sample},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {7},
   Pages = {072005},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.072005},
   Abstract = {We present a measurement of the top quark mass with tt̄
             dilepton events produced in pp̄ collisions at the Fermilab
             Tevatron (s=1.96TeV) and collected by the CDF II detector. A
             sample of 328 events with a charged electron or muon and an
             isolated track, corresponding to an integrated luminosity of
             2.9fb-1, are selected as tt̄ candidates. To account for the
             unconstrained event kinematics, we scan over the phase space
             of the azimuthal angles (ν1,ν2) of neutrinos and
             reconstruct the top quark mass for each ν1, ν2 pair by
             minimizing a χ2 function in the tt̄ dilepton hypothesis.
             We assign χ2-dependent weights to the solutions in order to
             build a preferred mass for each event. Preferred mass
             distributions (templates) are built from simulated tt̄ and
             background events, and parametrized in order to provide
             continuous probability density functions. A likelihood fit
             to the mass distribution in data as a weighted sum of signal
             and background probability density functions gives a top
             quark mass of 165.5-3.3+3.4(stat)±3. 1(syst)GeV/c2. © 2009
             The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.072005},
   Key = {fds309419}
}

@article{fds309420,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the top quark mass using the invariant mass
             of lepton pairs in soft muon b-tagged events},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {5},
   Pages = {051104},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.051104},
   Abstract = {We present the first measurement of the mass of the top
             quark in a sample of tt̅ →ℓν̅ bb̅ qq̅ events (where
             ℓ=e,μ) selected by identifying jets containing a muon
             candidate from the semileptonic decay of heavy-flavor
             hadrons (soft muon b tagging). The pp̅ collision data used
             correspond to an integrated luminosity of 2  fb-1 and
             were collected by the CDF II detector at the Fermilab
             Tevatron Collider. The measurement is based on a novel
             technique exploiting the invariant mass of a subset of the
             decay particles, specifically the lepton from the W boson of
             the t→Wb decay and the muon from a semileptonic b decay.
             We fit template histograms, derived from simulation of tt̅
             events and a modeling of the background, to the mass
             distribution observed in the data and measure a top quark
             mass of 180.5 &plusmn; 12.0(stat) &plusmn;
             3.6(syst)  GeV/c2, consistent with the current world
             average value.},
   Doi = {10.1103/PhysRevD.80.051104},
   Key = {fds309420}
}

@article{fds309421,
   Author = {Aaltonen, T and others},
   Title = {Searching the inclusive ℓγE̸T+b-quark signature for
             radiative top quark decay and non-standard-model
             processes},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {1},
   Pages = {011102},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.011102},
   Abstract = {We compare the inclusive production of events containing a
             lepton (ℓ), a photon (γ), significant transverse momentum
             imbalance (E̸T), and a jet identified as containing a
             b-quark, to SM predictions. The search uses data produced in
             proton-antiproton collisions at sqrt[s]=1.96  TeV
             corresponding to 1.9  fb-1 of integrated luminosity
             taken with the CDF detector. We find 28 ℓγbE̸T events
             versus an expectation of 31.0-3.5+4.1 events. If we further
             require events to contain at least three jets and large
             total transverse energy, the largest SM source is radiative
             top-quark pair production, tt̅ +γ. In the data we observe
             16 tt̅ γ candidate events versus an expectation from SM
             sources of 11.2-2.1+2.3. Assuming the difference between the
             observed number and the predicted non-top-quark total of
             6.8-2.0+2.2 is due to SM top-quark production, we estimate
             the tt̅ γ cross section to be 0.15 &plusmn;
             0.08  pb.},
   Doi = {10.1103/PhysRevD.80.011102},
   Key = {fds309421}
}

@article{fds309422,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the b-hadron production cross section using
             decays to mu[sup -]D[sup 0]X final states in p[overline p]
             collisions at sqrt(s) = 1.96 TeV},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {9},
   Pages = {092003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.092003},
   Abstract = {We report a measurement of the production cross section for
             b hadrons in pp̄ collisions at s=1.96TeV. Using a data
             sample derived from an integrated luminosity of 83pb-1
             collected with the upgraded Collider Detector (CDF II) at
             the Fermilab Tevatron, we analyze b hadrons, Hb, partially
             reconstructed in the semileptonic decay mode Hb→μ-D0X.
             Our measurement of the inclusive production cross section
             for b hadrons with transverse momentum pT>9GeV/c and
             rapidity |y|<0.6 is σ=1.30μb±0.05μb(stat)±0.
             14μb(syst)±0.07μb(B), where the uncertainties are
             statistical, systematic, and from branching fractions,
             respectively. The differential cross sections dσ/dpT are
             found to be in good agreement with recent measurements of
             the Hb cross section and well described by fixed-order
             next-to-leading logarithm predictions. © 2009 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.79.092003},
   Key = {fds309422}
}

@article{fds309424,
   Author = {Aaltonen, T and others},
   Title = {Observation of the Ωb- baryon and measurement of the
             properties of the Ξb- and Ωb- baryons},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {7},
   Pages = {072003},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.072003},
   Abstract = {We report the observation of the bottom, doubly-strange
             baryon Ωb- through the decay chain Ωb-→J/ψΩ-, where
             J/ψ→μ+μ-, Ω-→ΛK-, and Λ→pπ-, using
             4.2  fb-1 of data from pp̅ collisions at
             sqrt[s]=1.96  TeV, and recorded with the Collider
             Detector at Fermilab. A signal is observed whose probability
             of arising from a background fluctuation is 4.0×10-8, or
             5.5 Gaussian standard deviations. The Ωb- mass is measured
             to be 6054.4 &plusmn; 6.8(stat) &plusmn;
             0.9(syst)  MeV/c2. The lifetime of the Ωb- baryon is
             measured to be 1.13-0.40+0.53(stat) &plusmn;
             0.02(syst)  ps. In addition, for the Ξb- baryon we
             measure a mass of 5790.9 &plusmn; 2.6(stat) &plusmn;
             0.8(syst)  MeV/c2 and a lifetime of 1.56-0.25+0.27(stat)
             &plusmn; 0.02(syst)  ps. Under the assumption that the
             Ξb- and Ωb- are produced with similar kinematic
             distributions to the Λb0 baryon, we find
             σ(Ξb-)B(Ξb-→J/ψΞ-) / σ(Λb0)B(Λb0→J/ψΛ)=0.167-0.025+0.037(stat)
             &plusmn; 0.012(syst) and σ(Ωb-)B(Ωb-→J/ψΩ-) /
             σ(Λb0)B(Λb0→J/ψΛ)=0.045-0.012+0.017(stat) &plusmn;
             0.004(syst) for baryons produced with transverse momentum in
             the range of 6--20  GeV/c.},
   Doi = {10.1103/PhysRevD.80.072003},
   Key = {fds309424}
}

@article{fds309425,
   Author = {Aaltonen, T and others},
   Title = {Production of ψ(2S) mesons in pp̅ collisions at 1.96
             TeV},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {3},
   Pages = {031103},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.031103},
   Abstract = {We have measured the differential cross section for the
             inclusive production of ψ(2S) mesons decaying to μ+μ-
             that were produced in prompt or B-decay processes from pp̅
             collisions at 1.96 TeV. These measurements have been made
             using a data set from an integrated luminosity of
             1.1  fb-1 collected by the CDF II detector at Fermilab.
             For events with transverse momentum pT(ψ(2S))&gt;2  GeV/c
             and rapidity |y(ψ(2S))|&lt;0.6 we measure the integrated
             inclusive cross section σ(pp̅ →ψ(2S)X)·Br(ψ(2S)→μ+μ-)
             to be 3.29 &plusmn; 0.04(stat) &plusmn; 0.32(syst)  nb.},
   Doi = {10.1103/PhysRevD.80.031103},
   Key = {fds309425}
}

@article{fds309426,
   Author = {Aaltonen, T and others},
   Title = {Measurement of the tt̅ cross section in pp̅ collisions at
             sqrt[s] =1.96 TeV using dilepton events with a lepton plus
             track selection},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112007},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112007},
   Abstract = {This paper reports a measurement of the cross section for
             the pair production of top quarks in pp̅ collisions at
             sqrt[s]=1.96  TeV at the Fermilab Tevatron. The data
             were collected from the CDF run II detector in a set of runs
             with a total integrated luminosity of 1.1  fb-1. The
             cross section is measured in the dilepton channel, the
             subset of tt̅ events in which both top quarks decay through
             t→Wb→ℓνb, where ℓ=e, μ, or τ. The lepton pair is
             reconstructed as one identified electron or muon and one
             isolated track. The use of an isolated track to identify the
             second lepton increases the tt̅ acceptance, particularly
             for the case in which one W decays as W→τν. The purity
             of the sample may be further improved at the cost of a
             reduction in the number of signal events, by requiring an
             identified b jet. We present the results of measurements
             performed with and without the request of an identified b
             jet. The former is the first published CDF result for which
             a b-jet requirement is added to the dilepton selection. In
             the CDF data there are 129 pretag lepton+track candidate
             events, of which 69 are tagged. With the tagging
             information, the sample is divided into tagged and untagged
             subsamples, and a combined cross section is calculated by
             maximizing a likelihood. The result is σtt̅ =9.6 &plusmn;
             1.2(stat)-0.5+0.6(sys) &plusmn; 0.6(lum)  pb, assuming a
             branching ratio of BR(W→ℓν)=10.8% and a top mass of
             mt=175  GeV/c2.},
   Doi = {10.1103/PhysRevD.79.112007},
   Key = {fds309426}
}

@article{fds309427,
   Author = {Aaltonen, T and others},
   Title = {Search for the Higgs boson produced in association with
             Z→ℓ+ℓ- using the matrix element method at CDF
             II},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {7},
   Pages = {071101},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.071101},
   Abstract = {We present a search for associated production of the
             standard model Higgs boson and a Z boson where the Z boson
             decays to two leptons and the Higgs decays to a pair of b
             quarks in pp̅ collisions at the Fermilab Tevatron. We use
             event probabilities based on standard model matrix elements
             to construct a likelihood function of the Higgs content of
             the data sample. In a CDF data sample corresponding to an
             integrated luminosity of 2.7  fb-1 we see no evidence of
             a Higgs boson with a mass between 100  GeV/c2 and
             150  GeV/c2. We set 95% confidence level upper limits on
             the cross section for ZH production as a function of the
             Higgs boson mass mH; the limit is 8.2 times the standard
             model prediction at mH=115  GeV/c2.},
   Doi = {10.1103/PhysRevD.80.071101},
   Key = {fds309427}
}

@article{fds309428,
   Author = {Aaltonen, T and others},
   Title = {Measurement of particle production and inclusive
             differential cross sections in pp̅ collisions at sqrt[s]
             =1.96 TeV},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112005},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112005},
   Abstract = {We report a set of measurements of particle production in
             inelastic pp̅ collisions collected with a minimum-bias
             trigger at the Tevatron Collider with the CDF II experiment.
             The inclusive charged particle transverse momentum
             differential cross section is measured, with improved
             precision, over a range about ten times wider than in
             previous measurements. The former modeling of the spectrum
             appears to be incompatible with the high particle momenta
             observed. The dependence of the charged particle transverse
             momentum on the event particle multiplicity is analyzed to
             study the various components of hadron interactions. This is
             one of the observable variables most poorly reproduced by
             the available Monte Carlo generators. A first measurement of
             the event transverse energy sum differential cross section
             is also reported. A comparison with a pythia prediction at
             the hadron level is performed. The inclusive
             charged-particle differential production cross section is
             fairly well reproduced only in the transverse momentum range
             available from previous measurements. At higher momentum the
             agreement is poor. The transverse energy sum is poorly
             reproduced over the whole spectrum. The dependence of the
             charged particle transverse momentum on the particle
             multiplicity needs the introduction of more sophisticated
             particle production mechanisms, such as multiple parton
             interactions, in order to be better explained.},
   Doi = {10.1103/PhysRevD.79.112005},
   Key = {fds309428}
}

@article{fds309429,
   Author = {Aaltonen, T and others},
   Title = {Evidence for a Narrow Near-Threshold Structure in the J/ψϕ
             Mass Spectrum in B+→J/ψϕK+ Decays},
   Journal = {Phys. Rev. Lett.},
   Volume = {102},
   Number = {24},
   Pages = {242002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/physrevlett.102.242002},
   Abstract = {Evidence is reported for a narrow structure near the J/ψϕ
             threshold in exclusive B+→J/ψϕK+ decays produced in p̅
             p collisions at sqrt[s]=1.96  TeV. A signal of 14
             &plusmn; 5 events, with statistical significance in excess
             of 3.8 standard deviations, is observed in a data sample
             corresponding to an integrated luminosity of 2.7  fb-1,
             collected by the CDF II detector. The mass and natural width
             of the structure are measured to be 4143.0 &plusmn;
             2.9(stat) &plusmn; 1.2(syst)  MeV/c2 and
             11.7-5.0+8.3(stat) &plusmn; 3.7(syst)  MeV/c2.},
   Doi = {10.1103/physrevlett.102.242002},
   Key = {fds309429}
}

@article{fds309430,
   Author = {Aaltonen, T and others},
   Title = {Search for WW and WZ production in lepton plus jets final
             state at CDF},
   Journal = {Phys. Rev. D},
   Volume = {79},
   Number = {11},
   Pages = {112011},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112011},
   Abstract = {We present a search for WW and WZ production in final states
             that contain a charged lepton (electron or muon) and at
             least two jets, produced in sqrt[s]=1.96  TeV pp̅
             collisions at the Fermilab Tevatron, using data
             corresponding to 1.2  fb-1 of integrated luminosity
             collected with the CDF II detector. Diboson production in
             this decay channel has yet to be observed at hadron
             colliders due to the large single W plus jets background. An
             artificial neural network has been developed to increase
             signal sensitivity, as compared with an event selection
             based on conventional cuts. We set a 95% confidence level
             upper limit of σWW×BR(W→ℓνℓ,W→jets)+σWZ×BR(W→ℓνℓ,Z→jets)&lt;2.88  pb,
             which is consistent with the standard model
             next-to-leading-order cross section calculation for this
             decay channel of 2.09 &plusmn; 0.12  pb.},
   Doi = {10.1103/PhysRevD.79.112011},
   Key = {fds309430}
}

@article{fds309432,
   Author = {Aaltonen, T and others},
   Title = {Search for standard model Higgs boson production in
             association with a W boson using a neural network
             discriminant at CDF},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {1},
   Pages = {012002},
   Publisher = {APS},
   Year = {2009},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.012002},
   Abstract = {We present a search for standard model Higgs boson
             production in association with a W boson in
             proton-antiproton collisions (pp̅ →W &plusmn;
             H→ℓνbb̅ ) at a center of mass energy of 1.96 TeV. The
             search employs data collected with the CDF II detector that
             correspond to an integrated luminosity of approximately
             1.9  fb-1. We select events consistent with a signature
             of a single charged lepton (e &plusmn; /μ &plusmn; ),
             missing transverse energy, and two jets. Jets corresponding
             to bottom quarks are identified with a secondary vertex
             tagging method, a jet probability tagging method, and a
             neural network filter. We use kinematic information in an
             artificial neural network to improve discrimination between
             signal and background compared to previous analyses. The
             observed number of events and the neural network output
             distributions are consistent with the standard model
             background expectations, and we set 95% confidence level
             upper limits on the production cross section times branching
             fraction ranging from 1.2 to 1.1 pb or 7.5 to 102 times the
             standard model expectation for Higgs boson masses from 110
             to 150  GeV/c2, respectively.},
   Doi = {10.1103/PhysRevD.80.012002},
   Key = {fds309432}
}

@article{fds168217,
   Author = {T. Aaltonen and others},
   Title = {Measurement of the fraction of ttbar production via
             gluon-gluon fusion in ppbar collisions at 1.96
             TeV},
   Journal = {PRD},
   Volume = {79},
   Number = {3},
   Pages = {031101},
   Year = {2009},
   Key = {fds168217}
}

@article{fds168258,
   Author = {T. Aaltonen and others},
   Title = {Search for High-Mass e+e- Resonances in ppbar Collisions at
             1.96 TeV},
   Journal = {PRL},
   Volume = {102},
   Number = {3},
   Year = {2009},
   Key = {fds168258}
}

@article{fds309395,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
             T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
             F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bar-Shalom, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Behari, S and Bellettini, G and Bellinger,
             J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry,
             T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso,
             M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent,
             PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia,
             JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
             A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
             SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
             Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
             YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
             B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
             S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen,
             D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
             P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
             F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla
             Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rajaraman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
             PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A and Sinervo, P and Sisakyan, A},
   Title = {Search for maximal flavor violating scalars in same-charge
             lepton pairs in pp collisions at sqrt[s]=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {4},
   Pages = {041801},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.102.041801},
   Abstract = {Models of maximal flavor violation (MxFV) in elementary
             particle physics may contain at least one new scalar SU(2)
             doublet field Phi(FV)=(eta(0),eta(+)) that couples the first
             and third generation quarks (q_(1), q_(3)) via a Lagrangian
             term L(FV)=xi(13)Phi(FV)q(1)q(3). These models have a
             distinctive signature of same-charge top-quark pairs and
             evade flavor-changing limits from meson mixing measurements.
             Data corresponding to 2 fb(-1) collected by the Collider
             Dectector at Fermilab II detector in pp[over ] collisions at
             sqrt[s]=1.96 TeV are analyzed for evidence of the MxFV
             signature. For a neutral scalar eta(0) with m_(eta;(0))=200
             GeV/c(2) and coupling xi(13)=1, approximately 11 signal
             events are expected over a background of 2.1+/-1.8 events.
             Three events are observed in the data, consistent with
             background expectations, and limits are set on the coupling
             xi(13) for m(eta(0)=180-300 GeV/c(2).},
   Doi = {10.1103/physrevlett.102.041801},
   Key = {fds309395}
}

@article{fds309396,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Beecher, D and Behari, S and Bellettini,
             G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
             GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
             R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper,
             S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
             J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
             CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
             A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
             T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
             K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert,
             B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi,
             F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers,
             E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
             I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
             B},
   Title = {Direct bound on the total decay width of the top quark in pp
             collisions at sqrt[s]=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {4},
   Pages = {042001},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.102.042001},
   Abstract = {We present the first direct experimental bound on the total
             decay width of the top quark, Gamma(t), using 955 pb(-1) of
             the Tevatron's pp collisions recorded by the Collider
             Detector at Fermilab. We identify 253 top-antitop pair
             candidate events. The distribution of reconstructed top
             quark mass from these events is fitted to templates
             representing different values of the top quark width. Using
             a confidence interval based on likelihood-ratio ordering, we
             extract an upper limit at 95% C.L. of Gamma(t)<13.1 GeV for
             an assumed top quark mass of 175 GeV/c(2).},
   Doi = {10.1103/physrevlett.102.042001},
   Key = {fds309396}
}

@article{fds309398,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
             P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
             D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
             KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
             PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
             AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
             J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
             K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman,
             M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
             G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó,
             O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
             A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker,
             GL},
   Title = {Search for a Higgs boson decaying to two W bosons at
             CDF.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {2},
   Pages = {021802},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.102.021802},
   Abstract = {We present a search for a Higgs boson decaying to two W
             bosons in pp[over ] collisions at sqrt[s]=1.96 TeV
             center-of-mass energy. The data sample corresponds to an
             integrated luminosity of 3.0 fb;(-1) collected with the CDF
             II detector. We find no evidence for production of a Higgs
             boson with mass between 110 and 200 GeV/c;(2), and determine
             upper limits on the production cross section. For the mass
             of 160 GeV/c;(2), where the analysis is most sensitive, the
             observed (expected) limit is 0.7 pb (0.9 pb) at 95% Bayesian
             credibility level which is 1.7 (2.2) times the standard
             model cross section.},
   Doi = {10.1103/physrevlett.102.021802},
   Key = {fds309398}
}

@article{fds309404,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
             M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
   Title = {Search for the rare decays B+→μ+μ-K+, B0→μ+μ-
             K*(892)0, and Bs0→μ+μ- at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.011104},
   Abstract = {We search for b→sμ+μ- transitions in B meson (B+, B0, or
             Bs0) decays with 924pb-1 of pp̄ collisions at s=1.96TeV
             collected with the CDF II detector at the Fermilab Tevatron.
             We find excesses with significances of 4.5, 2.9, and 2.4
             standard deviations in the B+→μ+μ-K+,
             B0→μ+μ-K*(892)0, and Bs0→μ+μ- decay modes,
             respectively. Using B→J/ψh (h=K+, K*(892)0,) decays as
             normalization channels, we report branching fractions for
             the previously observed B+ and B0 decays,
             B(B+→μ+μ-K+)=(0.59±0.15±0. 04)×10-6, and
             B(B0→μ+μ-K*(892)0)=(0.81±0. 30±0.10)×10-6, where the
             first uncertainty is statistical, and the second is
             systematic. We set an upper limit on the relative branching
             fraction B(Bs0→μ+μ-)/B(Bs0→J/ψ)<2.6(2.3)×10-3 at the
             95(90)% confidence level, which is the most stringent to
             date. © 2009 The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.011104},
   Key = {fds309404}
}

@article{fds309411,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Aurisano, A and Azfar, F and Azzurri, P and Badgett,
             W and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung,
             K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci,
             MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
             J},
   Title = {Global search for new physics with 2.0fb-1 at
             CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.011101},
   Abstract = {Data collected in run II of the Fermilab Tevatron are
             searched for indications of new electroweak-scale physics.
             Rather than focusing on particular new physics scenarios,
             CDF data are analyzed for discrepancies with the standard
             model prediction. A model-independent approach (Vista)
             considers gross features of the data, and is sensitive to
             new large cross-section physics. Further sensitivity to new
             physics is provided by two additional algorithms: a Bump
             Hunter searches invariant mass distributions for "bumps"
             that could indicate resonant production of new particles,
             and the Sleuth procedure scans for data excesses at large
             summed transverse momentum. This combined global search for
             new physics in 2.0fb-1 of pp̄ collisions at s=1.96TeV
             reveals no indication of physics beyond the standard model.
             © 2009 The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.011101},
   Key = {fds309411}
}

@article{fds309408,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
             M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
             M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A},
   Title = {Erratum: Search for high-mass e+e- Resonances in pp̄
             collisions at s=1.96TeV (Physical Review Letters (2009) 102
             (031801))},
   Journal = {Physical Review Letters},
   Volume = {102},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevLett.102.059901},
   Doi = {10.1103/PhysRevLett.102.059901},
   Key = {fds309408}
}

@article{fds309392,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
             D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher,
             A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi,
             C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
             P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and da Costa, JG and Gunay-Unalan, Z and Haber, C and Hahn,
             K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher,
             F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris,
             RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
             A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
             BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
             AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone,
             S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
             CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso,
             SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
             G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
             K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder,
             N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
             A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
             MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
             FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
             J},
   Title = {Inclusive search for squark and gluino production in pp[over
             ] collisions at sqrt[s]=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {12},
   Pages = {121801},
   Year = {2009},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.102.121801},
   Abstract = {We report on a search for inclusive production of squarks
             and gluinos in pp[over ] collisions at sqrt[s]=1.96 TeV, in
             events with large missing transverse energy and multiple
             jets of hadrons in the final state. The study uses a CDF Run
             II data sample corresponding to 2 fb(-1) of integrated
             luminosity. The data are in good agreement with the standard
             model predictions, giving no evidence for any squark or
             gluino component. In an R-parity conserving minimal
             supergravity scenario with A(0)=0, mu<0, and tanbeta=5, 95%
             C.L. upper limits on the production cross sections in the
             range between 0.1 and 1 pb are obtained, depending on the
             squark and gluino masses considered. For gluino masses below
             280 GeV/c(2), arbitrarily large squark masses are excluded
             at the 95% C.L., while for mass degenerate gluinos and
             squarks, masses below 392 GeV/c(2) are excluded at the 95%
             C.L.},
   Doi = {10.1103/physrevlett.102.121801},
   Key = {fds309392}
}

@article{fds309433,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BAL and Amerio,
             S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Measurement of cross sections for b jet production in events
             with a Z boson in pp̄ collisions at s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.052008},
   Abstract = {A measurement of the b jet production cross section is
             presented for events containing a Z boson produced in pp̄
             collisions at s=1.96TeV, using data corresponding to an
             integrated luminosity of 2fb-1 collected by the CDF II
             detector at the Tevatron. Z bosons are selected in the
             electron and muon decay modes. Jets are considered with
             transverse energy ET>20GeV and pseudorapidity |η|<1.5 and
             are identified as b jets using a secondary vertex algorithm.
             The ratio of the integrated Z+b jet cross section to the
             inclusive Z production cross section is measured to be
             3.32±0.53(stat)±0.42(syst) ×10-3. This ratio is also
             measured differentially in jet ET, jet η, Z-boson
             transverse momentum, number of jets, and number of b jets.
             The predictions from leading-order Monte Carlo generators
             and next-to-leading-order QCD calculations are found to be
             consistent with the measurements within experimental and
             theoretical uncertainties. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.79.052008},
   Key = {fds309433}
}

@article{fds309423,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Measurement of W-boson helicity fractions in top-quark
             decays using cos θ*},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {674},
   Number = {3},
   Pages = {160-167},
   Publisher = {Elsevier BV},
   Year = {2009},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2009.02.040},
   Abstract = {Fully reconstructed t over(t, ̄) → W+ b W- over(b, ̄)
             → ℓ ν q over(q, ̄)′ b over(b, ̄) events are used to
             determine the fractions of right-handed (f+) and
             longitudinally polarized (f0) W bosons produced in top-quark
             decays. The helicity fractions are sensitive to the
             couplings and the Dirac structure of the Wtb vertex. This
             Letter reports measurements of the W-boson helicity
             fractions from two different methods using data
             corresponding to an integrated luminosity of 1.9 fb- 1 of p
             over(p, ̄) collisions at a center-of-mass energy of 1.96
             TeV collected by the CDF II detector operating at the
             Fermilab Tevatron. Combining the results from the two
             methods, we find f0 = 0.62 ± 0.10 (stat) ± 0.05 (syst)
             under the assumption that f+ = 0, and f+ = - 0.04 ± 0.04
             (stat) ± 0.03 (syst) with f0 fixed to the theoretically
             expected value of 0.70. Model-independent fits are also
             performed and simultaneously determine f0 = 0.66 ± 0.16
             (stat) ± 0.05 (syst) and f+ = - 0.03 ± 0.06 (stat) ± 0.03
             (syst). All these results are consistent with standard model
             expectations. © 2009 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2009.02.040},
   Key = {fds309423}
}

@article{fds309388,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
             GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
             R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
             M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
             M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
             C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
             RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
             J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela,
             J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
             DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
             J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
             F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto,
             WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
             A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D},
   Title = {Search for the decays B_{(s)};{0} --> e;{+} micro;{-} and
             B_{(s)};{0} --> e;{+} e;{-} in CDF run II.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {20},
   Pages = {201801},
   Year = {2009},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.102.201801},
   Abstract = {We report results from a search for the lepton flavor
             violating decays B_{s};{0} --> e;{+} micro;{-} and B;{0} -->
             e;{+} micro;{-}, and the flavor-changing neutral-current
             decays B_{s};{0} --> e;{+} e;{-} and B;{0} --> e;{+} e;{-}.
             The analysis uses data corresponding to 2 fb;{-1} of
             integrated luminosity of pp[over ] collisions at sqrt[s] =
             1.96 TeV collected with the upgraded Collider Detector (CDF
             II) at the Fermilab Tevatron. The observed number of B0 and
             B_{s};{0} candidates is consistent with background
             expectations. The resulting Bayesian upper limits on the
             branching ratios at 90% credibility level are B(B_{s};{0}
             --> e;{+} micro;{-}) < 2.0 x 10;{-7}, B(B;{0} --> e;{+}
             micro;{-}) < 6.4 x 10;{-8}, B(B_{s};{0} --> e;{+} e;{-}) <
             2.8 x 10;{-7}, and B(B;{0} --> e;{+} e;{-}) < 8.3 x 10;{-8}.
             From the limits on B(B_{(s)};{0} --> e;{+} micro;{-}), the
             following lower bounds on the Pati-Salam leptoquark masses
             are also derived: M_{LQ}(B_{s};{0} --> e;{+} micro;{-}) >
             47.8 TeV/c;{2}, and M_{LQ}(B;{0} --> e;{+} micro;{-}) > 59.3
             TeV / c;{2}, at 90% credibility level.},
   Doi = {10.1103/physrevlett.102.201801},
   Key = {fds309388}
}

@article{fds309405,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
             P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
             D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
             M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
             S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
             E and Hamilton, A and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
             BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
             AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan,
             P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
             CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
             R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla
             Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
             A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
             B},
   Title = {Observation of exclusive charmonium production and
             gammagamma --> micro;{+}micro;{-} in pp[over] collisions at
             sqrt[s] = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {24},
   Pages = {242001},
   Year = {2009},
   Month = {June},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.102.242001},
   Abstract = {In CDF we have observed the reactions p + p[over] --> p + X
             + p[over], with X being a centrally produced J/psi, psi(2S),
             or chi_{c0}, and gammagamma-->micro;{+}micro;{-} in pp[over]
             collisions at sqrt[s] = 1.96 TeV. The event signature
             requires two oppositely charged central muons, and either no
             other particles or one additional photon detected. Exclusive
             vector meson production is as expected for elastic
             photoproduction, gamma + p --> J/psi(psi(2S)) + p, observed
             here for the first time in hadron-hadron collisions. We also
             observe exclusive chi_{c0} --> J/psi + gamma. The cross
             sections dsigma/dy|_{y = 0} for J/psi, psi(2S), and chi_{c0}
             are 3.92 +/- 0.25(stat) +/- 0.52(syst) nb, 0.53 +/-
             0.09(stat) +/- 0.10(syst) nb, and 76 +/- 10(stat) +/-
             10(syst) nb, respectively, and the continuum is consistent
             with QED. We put an upper limit on the cross section for
             Odderon exchange in exclusive J/psi production.},
   Doi = {10.1103/physrevlett.102.242001},
   Key = {fds309405}
}

@article{fds309410,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi,
             F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
             M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
             M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
             S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Di Canto and A and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Garosi, P and Genser, K and Gerberich,
             H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
             da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
             D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
             JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
             S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee,
             SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
             P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
             J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
             J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
             S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sinervo,
             P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M},
   Title = {Search for exclusive Z-boson production and observation of
             high-mass pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
             ] events in pp[over ] collisions at sqrt[s]=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {102},
   Number = {22},
   Pages = {222002},
   Year = {2009},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.102.222002},
   Abstract = {This Letter presents a search for exclusive Z boson
             production in proton-antiproton collisions at sqrt[s]=1.96
             TeV, using the CDF II detector. No exclusive Z-->l;{+}l;{-}
             candidates are observed and the first upper limit on the
             exclusive Z cross section in hadron collisions is found to
             be sigma_{excl}(Z)<0.96 pb at 95% confidence level. In
             addition, eight candidate exclusive dilepton events from the
             process pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
             ] are observed, and a measurement of the cross section for
             M_{ll}>40 GeV/c;{2} and |eta_{l}|<4 is found to be
             sigma=0.24_{-0.10};{+0.13} pb, which is consistent with the
             standard model prediction.},
   Doi = {10.1103/physrevlett.102.222002},
   Key = {fds309410}
}

@article{fds309436,
   Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
             MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
             B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
             M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
             MA},
   Title = {Measurement of the ratio of branching fractions B(B±→J/
             ψπ±)/B(B±→J/ψK±)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.112003},
   Abstract = {We report a measurement of the ratio of branching fractions
             of the decays B±→J/ψπ± and B±→J/ψK± using the CDF
             II detector at the Fermilab Tevatron Collider. The signal
             from the Cabbibo-suppressed B±→J/ψπ± decay is
             separated from B±→J/ψK± using the B±→J/ψK±
             invariant mass distribution and the kinematical differences
             of the hadron track in the two decay modes. From a sample of
             220pb-1 of pp̄ collisions at s=1.96TeV, we observe 91±15
             B±→J/ψπ± events together with 1883±34 B±→J/ψK±
             events. The ratio of branching fractions is found to be
             B(B±→J/ψπ±)/ B(B±→J/ψK±)=(4.86±0.82(stat)±0.15(syst))%.
             © 2009 The American Physical Society.},
   Doi = {10.1103/PhysRevD.79.112003},
   Key = {fds309436}
}

@article{fds309403,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
             González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
             A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
             F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
             A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
             A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
             M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
   Title = {Erratum: Measurement of the inclusive jet cross section at
             the Fermilab Tevatron pp̄ collider using a cone-based jet
             algorithm (Physical Review D (2008) 78 (052006))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {79},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.79.119902},
   Doi = {10.1103/PhysRevD.79.119902},
   Key = {fds309403}
}

@article{fds309431,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Search for narrow resonances lighter than Υ
             mesons},
   Journal = {European Physical Journal C},
   Volume = {62},
   Number = {2},
   Pages = {319-326},
   Publisher = {Springer Nature},
   Year = {2009},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-009-1057-4},
   Abstract = {We report a search for narrow resonances, produced in p p̄
             collisions at √ s=1.96 TeV, that decay into muon pairs
             with invariant mass between 6.3 and 9.0 GeV/c 2. The data,
             collected with the CDF II detector at the Fermilab Tevatron
             collider, correspond to an integrated luminosity of 630 pb
             -1. We use the dimuon invariant mass distribution to set 90%
             upper credible limits of about 1% to the ratio of the
             production cross section times muonic branching fraction of
             possible narrow resonances to that of the Υ(1S) meson. ©
             2009 Springer-Verlag.},
   Doi = {10.1140/epjc/s10052-009-1057-4},
   Key = {fds309431}
}

@article{fds309435,
   Author = {Abat, E and Abdallah, JM and Addy, TN and Adragna, P and Aharrouche, M and Ahmad, A and Akesson, TPA and Aleksa, M and Alexa, C and Anderson, K and Anghinolfi, F and Antonaki, A and Arabidze, G and Arik, E and Baker, OK and Banfi, D and Baron, S and Beck, HP and Belhorma, B and Benchekroun, D and Benjamin, DP and Benslama, K and Bergeaas Kuutmann and E and Bertelsen,
             H and Binet, S and Biscarat, C and Boldea, V and Bondarenko, VG and Boonekamp, M and Bosman, M and Bourdarios, C and Burckhart Chromek,
             D and Bychkov, V and Callahan, J and Calvet, D and Canneri, M and Capeáns
             Garrido, M and Caprini, M and Cardiel Sas and L and Carli, T and Carminati,
             L and Carvalho, J and Cascella, M and Castillo, MV and Catinaccio, A and Cavalli Sforza and M and Cavalli, D and Cavasinni, V and Cetin, SA and Chen, H and Cherkaoui, R and Chevallier, F and Ciobotaru, M and Citterio, M and Cleland, B and Cogneras, E and Conde Muino and P and Consonni, M and Constantinescu, S and Cornelissen, T and Corso Radu,
             A and Costa, G and Cwetanski, P and Da Silva and D and Dam, M and Danielsson,
             HO and Dannheim, D and Davidek, T and De, K and Defay, PO and Dekhissi, B and Del Peso and J and Delmastro, M and Del Prete and T and Derue, F and Di
             Ciaccio, L and Di Girolamo and B and Dita, S and Dittus, F and Djama, F and Djobava, T and Dobson, M and Dolgoshein, BA and Dotti, A and Drake, G and Dressnandt, N and Driouchi, C and Ebenstein, WL and Eerola, P and Efthymiopoulos, I and Egorov, K and Eifert, TF and El Kacimi and M and Etienvre, AI and Fabich, A and Fakhr-Edine, AI and Fanti, M and Farbin,
             A and Farthouat, P and Fassouliotis, D},
   Title = {Study of the response of the ATLAS central calorimeter to
             pions of energies from 3 to 9 GeV},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {607},
   Number = {2},
   Pages = {372-386},
   Publisher = {Elsevier BV},
   Year = {2009},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.nima.2009.05.158},
   Abstract = {A fully instrumented slice of the ATLAS central detector was
             exposed to test beams from the SPS (Super Proton
             Synchrotron) at CERN in 2004. In this paper, the response of
             the central calorimeters to pions with energies in the range
             between 3 and 9 GeV is presented. The linearity and the
             resolution of the combined calorimetry (electromagnetic and
             hadronic calorimeters) was measured and compared to the
             prediction of a detector simulation program using the
             toolkit Geant 4. © 2009 Elsevier B.V.},
   Doi = {10.1016/j.nima.2009.05.158},
   Key = {fds309435}
}

@article{fds309401,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
             BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
             J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
             A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
             P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
   Title = {Publisher's Note: Search for hadronic decays of W and Z
             bosons in photon events in pp̄ collisions at
             s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {80},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2009},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.079901},
   Doi = {10.1103/PhysRevD.80.079901},
   Key = {fds309401}
}

@article{fds309399,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Aloisio, A and Alon, R and Alonso, A and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós,
             G and Amram, N and Anastopoulos, C and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Antonaki, A and Antonelli, M and Antonelli, S and Antunovic, B and Anulli, F and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin,
             JF and Argyropoulos, T and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai, M and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
             M},
   Title = {The ATLAS Collaboration},
   Journal = {Nuclear Physics A},
   Volume = {830},
   Number = {1-4},
   Pages = {925c-940c},
   Publisher = {Elsevier BV},
   Year = {2009},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.nuclphysa.2009.10.143},
   Doi = {10.1016/j.nuclphysa.2009.10.143},
   Key = {fds309399}
}

@article{fds309434,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the inclusive isolated prompt photon cross
             section in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
             collisions at $\sqrt{s}=1.96\,\,TeV$ using the CDF
             detector},
   Journal = {Phys. Rev. D},
   Volume = {80},
   Number = {11},
   Pages = {111106},
   Publisher = {American Physical Society},
   Year = {2009},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.111106},
   Abstract = {A measurement of the cross section for the inclusive
             production of isolated photons by the CDF experiment at the
             Fermilab Tevatron collider is presented. The measurement
             covers the pseudorapidity region $|\eta\gamma|30$  GeV
             and is based on 2.5  fb-1 of integrated luminosity. The
             sample is almost a factor of 7 larger than those used for
             recent published results and extends the $E_T^\gamma$
             coverage by 100 GeV. The result agrees with next-to-leading
             order perturbative QCD calculations within uncertainties
             over the range $50},
   Doi = {10.1103/PhysRevD.80.111106},
   Key = {fds309434}
}

@article{fds309325,
   Author = {Aaltonen, and T, and others},
   Title = {Search for the Production of Scalar Bottom Quarks in $p
             \bar{p}$ collisions at $\sqrt{s} = 1.96$
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {8},
   Pages = {081802},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.081802},
   Abstract = {http://arxiv.org/abs/1005.3600},
   Doi = {10.1103/PhysRevLett.105.081802},
   Key = {fds309325}
}

@article{fds309327,
   Author = {Aaltonen, and T, and others},
   Title = {First Measurement of the Ratio $\sigma_{(t\bar{t})} /
             \sigma_{(Z/\gamma^*\to ll)}$ and Precise Extraction of the
             $t\bar{t}$ Cross Section},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {1},
   Pages = {012001},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.012001},
   Abstract = {http://arxiv.org/abs/1004.3224},
   Doi = {10.1103/PhysRevLett.105.012001},
   Key = {fds309327}
}

@article{fds309328,
   Author = {Aaltonen, and T, and others},
   Title = {Search for Pair Production of Supersymmetric Top Quarks in
             Dilepton Events from $p\bar{p}$ Collisions at $\sqrt{s}$ =
             1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {25},
   Pages = {251801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.251801},
   Abstract = {http://arxiv.org/abs/0912.1308},
   Doi = {10.1103/PhysRevLett.104.251801},
   Key = {fds309328}
}

@article{fds309329,
   Author = {Aaltonen, and T, and others},
   Title = {Search for $WW$ and $WZ$ resonances decaying to electron,
             missing $E_T$, and two jets in $p\bar{p}$ collisions at
             $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {24},
   Pages = {241801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.241801},
   Abstract = {http://arxiv.org/abs/1004.4946},
   Doi = {10.1103/PhysRevLett.104.241801},
   Key = {fds309329}
}

@article{fds309330,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $W^+W^-$ Production Cross Section and
             Search for Anomalous $WW\gamma$ and $WWZ$ Couplings in $p
             \bar p$ Collisions at $\sqrt{s} = 1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {20},
   Pages = {201801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.201801},
   Abstract = {http://arxiv.org/abs/0912.4500},
   Doi = {10.1103/PhysRevLett.104.201801},
   Key = {fds309330}
}

@article{fds309332,
   Author = {Aaltonen, and T, and others},
   Title = {A Search for the Higgs Boson Using Neural Networks in Events
             with Missing Energy and $b$-quark Jets in $p\bar p$
             Collisions at $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {14},
   Pages = {141801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.141801},
   Abstract = {http://arxiv.org/abs/0911.3935},
   Doi = {10.1103/PhysRevLett.104.141801},
   Key = {fds309332}
}

@article{fds309333,
   Author = {Aaltonen, and T, and others},
   Title = {First Measurement of the b-jet Cross Section in Events with
             a $W$ Boson in $p \bar{p}$ Collisions at $\sqrt{s} = 1.96$
             TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {13},
   Pages = {131801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.131801},
   Abstract = {http://arxiv.org/abs/0909.1505},
   Doi = {10.1103/PhysRevLett.104.131801},
   Key = {fds309333}
}

@article{fds309334,
   Author = {Aaltonen, and T, and others},
   Title = {Search for Technicolor Particles Produced in Association
             with a $W$ Boson at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {11},
   Pages = {111802},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.111802},
   Abstract = {http://arxiv.org/abs/0912.2059},
   Doi = {10.1103/PhysRevLett.104.111802},
   Key = {fds309334}
}

@article{fds309335,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $\Lambda_b$ Lifetime in $\Lambda_b \to
             \Lambda_c^+ \pi^-$ Decays in $p\bar{p}$ Collisions at
             $\sqrt{s} = 1.96$ TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {10},
   Pages = {102002},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.102002},
   Abstract = {http://arxiv.org/abs/0912.3566},
   Doi = {10.1103/PhysRevLett.104.102002},
   Key = {fds309335}
}

@article{fds309336,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $WW+WZ$ Production Cross Section Using
             the Lepton+Jets Final State at CDF II},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {10},
   Pages = {101801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.101801},
   Abstract = {http://arxiv.org/abs/0911.4449},
   Doi = {10.1103/PhysRevLett.104.101801},
   Key = {fds309336}
}

@article{fds309337,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Bottomlike Quark Pair Decays $Q\bar{Q} \to
             (tW^\mp)(\bar{t}W^\pm)$ in Same-Charge Dilepton
             Events},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {9},
   Pages = {091801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.091801},
   Abstract = {http://arxiv.org/abs/0912.1057},
   Doi = {10.1103/PhysRevLett.104.091801},
   Key = {fds309337}
}

@article{fds309338,
   Author = {Aaltonen, and T, and others},
   Title = {Combination of Tevatron searches for the standard model
             Higgs boson in the $W^+W^-$ decay mode},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {6},
   Pages = {061802},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.061802},
   Abstract = {http://arxiv.org/abs/1001.4162},
   Doi = {10.1103/PhysRevLett.104.061802},
   Key = {fds309338}
}

@article{fds309339,
   Author = {Aaltonen, and T, and others},
   Title = {Inclusive Search for Standard Model Higgs Boson Production
             in the WW Decay Channel using the CDF II
             Detector},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {6},
   Pages = {061803},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.061803},
   Abstract = {http://arxiv.org/abs/1001.4468},
   Doi = {10.1103/PhysRevLett.104.061803},
   Key = {fds309339}
}

@article{fds309340,
   Author = {Aaltonen, and T, and others},
   Title = {Search for Supersymmetry with Gauge-Mediated Breaking in
             Diphoton Events with Missing Transverse Energy at CDF
             II},
   Journal = {Phys. Rev. Lett.},
   Volume = {104},
   Number = {1},
   Pages = {011801},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevLett.104.011801},
   Abstract = {http://arxiv.org/abs/0910.3606},
   Doi = {10.1103/PhysRevLett.104.011801},
   Key = {fds309340}
}

@article{fds309344,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $t \bar{t}$ Production Cross Section in
             $p \bar{p}$ Collisions at $\sqrt{s} = 1.96$ TeV using Soft
             Electron $b$-Tagging},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.092002},
   Abstract = {http://arxiv.org/abs/1002.3783},
   Doi = {10.1103/PhysRevD.81.092002},
   Key = {fds309344}
}

@article{fds309345,
   Author = {Aaltonen, and T, and others},
   Title = {Measurements of the top-quark mass using charged particle
             tracking},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {3},
   Pages = {032002},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.032002},
   Abstract = {http://arxiv.org/abs/0910.0969},
   Doi = {10.1103/PhysRevD.81.032002},
   Key = {fds309345}
}

@article{fds309347,
   Author = {Aaltonen, and T, and others},
   Title = {Search for single top quark production in $\bar{p} p$
             collisions at $\sqrt{s} = 1.96$ TeV in the missing
             transverse energy plus jets topology},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.072003},
   Abstract = {http://arxiv.org/abs/1001.4577},
   Doi = {10.1103/PhysRevD.81.072003},
   Key = {fds309347}
}

@article{fds309351,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the Top Quark Mass and $p \bar{p} \to t
             \bar{t}$ Cross Section in the All-Hadronic Mode with the
             CDFII Detector},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {5},
   Pages = {052011},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.052011},
   Abstract = {http://arxiv.org/abs/1002.0365},
   Doi = {10.1103/PhysRevD.81.052011},
   Key = {fds309351}
}

@article{fds309353,
   Author = {Aaltonen, and T, and others},
   Title = {Studying the Underlying Event in Drell-Yan and High
             Transverse Momentum Jet Production at the
             Tevatron},
   Journal = {Phys. Rev.},
   Volume = {D82},
   Number = {3},
   Pages = {034001},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.034001},
   Abstract = {http://arxiv.org/abs/1003.3146},
   Doi = {10.1103/PhysRevD.82.034001},
   Key = {fds309353}
}

@article{fds309354,
   Author = {Aaltonen, and T, and others},
   Title = {Top Quark Mass Measurement using $m_{T2}$ in the Dilepton
             Channel at CDF},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {3},
   Pages = {031102},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.031102},
   Abstract = {http://arxiv.org/abs/0911.2956},
   Doi = {10.1103/PhysRevD.81.031102},
   Key = {fds309354}
}

@article{fds309355,
   Author = {Aaltonen, and T, and others},
   Title = {Measurements of branching fraction ratios and CP asymmetries
             in $B^\pm \to D_{CP} K^\pm$ decays in hadron
             collisions},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {3},
   Pages = {031105},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.031105},
   Abstract = {http://arxiv.org/abs/0911.0425},
   Doi = {10.1103/PhysRevD.81.031105},
   Key = {fds309355}
}

@article{fds309357,
   Author = {Aaltonen, and T, and others},
   Title = {A study of the associated production of photons and
             $b$-quark jets in $p \bar{p}$ collisions at $\sqrt{s} =
             1.96$ TeV},
   Journal = {Phys. Rev.},
   Volume = {D81},
   Number = {5},
   Pages = {052006},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   url = {http://dx.doi.org/10.1103/PhysRevD.81.052006},
   Abstract = {http://arxiv.org/abs/0912.3453},
   Doi = {10.1103/PhysRevD.81.052006},
   Key = {fds309357}
}

@article{fds309358,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Color-Octet Vector Particle Decaying to $t
             \bar{t}$ in $p \bar{p}$ Collisions at $\sqrt{s}=1.96$
             TeV},
   Journal = {Phys. Lett.},
   Volume = {B691},
   Number = {4},
   Pages = {183-190},
   Publisher = {Elsevier BV},
   Year = {2010},
   url = {http://dx.doi.org/10.1016/j.physletb.2010.06.036},
   Abstract = {http://arxiv.org/abs/0911.3112},
   Doi = {10.1016/j.physletb.2010.06.036},
   Key = {fds309358}
}

@article{fds309359,
   Author = {Aaltonen, and T, and others},
   Title = {Study of multi-muon events produced in $p \bar{p}$
             interactions at $\sqrt{s} = 1.96$-TeV},
   Journal = {Eur. Phys. J.},
   Volume = {C68},
   Number = {1},
   Pages = {109-118},
   Publisher = {Springer Nature},
   Year = {2010},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1336-0},
   Abstract = {We report the results of a study of multi-muon events
             produced at the Fermilab Tevatron collider and acquired with
             the CDF II detector using a dedicated dimuon trigger. The
             production cross section and kinematics of events in which
             both muon candidates are produced inside the beam pipe of
             radius 1.5 cm are successfully modeled by known processes
             which include heavy flavor production. In contrast, we are
             presently unable to fully account for the number and
             properties of the remaining events, in which at least one
             muon candidate is produced outside of the beam pipe, in
             terms of the same understanding of the CDF II detector,
             trigger, and event reconstruction. © 2010 The
             Author(s).},
   Doi = {10.1140/epjc/s10052-010-1336-0},
   Key = {fds309359}
}

@article{fds309362,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco,
             SD and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
             J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
             A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
             ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
             F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shekhar, R and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini,
             N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez,
             F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
             T},
   Title = {Improved search for a Higgs boson produced in association
             with Z→l+l- in pp̄ collisions at
             √s=1.96TeV},
   Journal = {Physical Review Letters},
   Volume = {105},
   Number = {25},
   Pages = {251802},
   Year = {2010},
   url = {http://www.ncbi.nlm.nih.gov/pubmed/21231575},
   Abstract = {We search for the standard model Higgs boson produced with a
             Z boson in 4.1fb⊃-1 of integrated luminosity collected
             with the CDF II detector at the Tevatron. In events
             consistent with the decay of the Higgs boson to a
             bottom-quark pair and the Z boson to electrons or muons, we
             set 95% credibility level upper limits on the ZH production
             cross section multiplied by the H→bb̄ branching ratio.
             Improved analysis methods enhance signal sensitivity by 20%
             relative to previous searches. At a Higgs boson mass of
             115GeV/c2 we set a limit of 5.9 times the standard model
             cross section. © 2010 The American Physical
             Society.},
   Doi = {10.1103/PhysRevLett.105.251802},
   Key = {fds309362}
}

@article{fds185149,
   Author = {Aaltonen et al.},
   Title = {Search for WW and WZ Resonances Decaying to Electron,
             Missing ET, and Two Jets in Collisions at Ecm= 1.96 TeV,”
             Phys. Rev. Lett. 104, 241801},
   Year = {2010},
   Key = {fds185149}
}

@article{fds185147,
   Author = {T. Aaltonen et al.},
   Title = {Studying the Underlying Event in Drell-Yan and High
             Transverse Momentum Jet Production at the Tevatron,” Phys.
             Rev. D82, 034001 (2010).},
   Year = {2010},
   Key = {fds185147}
}

@article{fds185148,
   Author = {T. Aaltonen et al.},
   Title = {Measurement of W+W- Production Cross Section and Search for
             Anomalous WW and WWZ Couplings in Collisions at 1.96
             TeV,” Phys. Rev. Lett. 104, 201801 (2010).},
   Year = {2010},
   Key = {fds185148}
}

@article{fds185152,
   Author = {ATLAS collaboration},
   Title = {Charged-particle multiplicities in pp interactions at √s =
             900 GeV measured with the ATLAS detector at the LHC, Phys
             Lett B 688, 1, 21},
   Year = {2010},
   Key = {fds185152}
}

@article{fds185153,
   Author = {ATLAS Collaboration},
   Title = {Search for New Particles in Two-Jet Final States in 7 TeV
             Proton-Proton Collisions with the ATLAS Detector at the LHC,
             Phys. Rev. Lett. 105, 161801},
   Year = {2010},
   Key = {fds185153}
}

@article{fds185154,
   Author = {ATLAS Collaboration},
   Title = {The ATLAS Inner Detector commissioning and calibration, EPJC
             70 (2010) 787},
   Year = {2010},
   Key = {fds185154}
}

@article{fds185155,
   Author = {ATLAS Collaboration},
   Title = {Performance of the ATLAS Detector using First Collision
             Data, JHEP 1009:056,2010},
   Year = {2010},
   Key = {fds185155}
}

@article{fds309320,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adorisio, C and Adragna,
             P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli,
             G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas,
             A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Ambrosio, G and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR},
   Title = {Measurement of the W → ℓν and Z/γ* →
             ℓℓ production cross sections in proton-proton collisions
             at √ s = 7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2010},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP12(2010)060},
   Abstract = {First measurements of the W → ℓν and Z/γ * → ℓℓ
             (ℓ = e, μ) production cross sections in proton-proton
             collisions at √ s = 7TeV are presented using data recorded
             by the ATLAS experiment at the LHC. The results are based on
             2250 W → ℓν and 179 Z/γ* → ℓℓ candidate events
             selected from a data set corresponding to an integrated
             luminosity of approximately 320 nb-1. The measured total W
             and Z/ γ*-boson production cross sections times the
             respective leptonic branching ratios for the combined
             electron and muon channels are σtotW · BR(W → ℓν) =
             9.96 ± 0.23(stat) ± 0.50(syst) ± 1.10(lumi) nb and
             σtotZ/γ* · BR(Z/ γ* → ℓℓ) = 0.82 ± 0.06 (stat) ±
             0.05 (syst) ± 0.09 (lumi) nb (within the invariant mass
             window 66 < mℓℓ < 116 GeV). The W/Z cross-section ratio
             is measured to be 11.7 ± 0.9(stat) ± 0.4(syst). In
             addition, measurements of the W+ and W- production cross
             sections and of the lepton charge asymmetry are reported.
             Theoretical predictions based on NNLO QCD calculations are
             found to agree with the measurements.},
   Doi = {10.1007/JHEP12(2010)060},
   Key = {fds309320}
}

@article{fds309371,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acharya, BS and Adams, DL and Addy,
             TN and Adelman, J and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alviggi, MG and Amako, K and Amelung, C and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai, M and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A},
   Title = {The ATLAS Simulation Infrastructure},
   Journal = {European Physical Journal C},
   Volume = {70},
   Number = {3},
   Pages = {823-874},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1429-9},
   Abstract = {The simulation software for the ATLAS Experiment at the
             Large Hadron Collider is being used for large-scale
             production of events on the LHC Computing Grid. This
             simulation requires many components, from the generators
             that simulate particle collisions, through packages
             simulating the response of the various detectors and
             triggers. All of these components come together under the
             ATLAS simulation infrastructure. In this paper, that
             infrastructure is discussed, including that supporting the
             detector description, interfacing the event generation, and
             combining the GEANT4 simulation of the response of the
             individual detectors. Also described are the tools allowing
             the software validation, performance testing, and the
             validation of the simulated output against known physics
             processes. © 2010 CERN for the benefit of the ATLAS
             collaboration.},
   Doi = {10.1140/epjc/s10052-010-1429-9},
   Key = {fds309371}
}

@article{fds309331,
   Author = {Aad, G and Abat, E and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli,
             G and Akdogan, T and Åkesson, PF and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Ambrosini, G and Ambrosio, G and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, E and Arik,
             M and Armbruster, AJ},
   Title = {Charged-particle multiplicities in pp interactions at √ s
             = 900 GeV measured with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {688},
   Number = {1},
   Pages = {21-42},
   Publisher = {Elsevier BV},
   Year = {2010},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2010.03.064},
   Abstract = {The first measurements from proton-proton collisions
             recorded with the ATLAS detector at the LHC are presented.
             Data were collected in December 2009 using a minimum-bias
             trigger during collisions at a centre-of-mass energy of 900
             GeV. The charged-particle multiplicity, its dependence on
             transverse momentum and pseudorapidity, and the relationship
             between mean transverse momentum and chargedparticle
             multiplicity are measured for events with at least one
             charged particle in the kinematic range |η| < 2.5 and pT >
             500 MeV. The measurements are compared to Monte Carlo models
             of proton-proton collisions and to results from other
             experiments at the same centre-of-mass energy. The
             charged-particle multiplicity per event and unit of
             pseudorapidity at η = 0 is measured to be 1.333 ±
             0.003(stat.) ± 0.040(syst.), which is 5-15% higher than the
             Monte Carlo models predict.},
   Doi = {10.1016/j.physletb.2010.03.064},
   Key = {fds309331}
}

@article{fds309367,
   Author = {Abat, E and Abdallah, JM and Addy, TN and Adragna, P and Aharrouche, M and Ahmad, A and Akesson, TPA and Aleksa, M and Alexa, C and Anderson, K and Anghinolfi, F and Antonaki, A and Arabidze, G and Arik, E and Baker, OK and Banfi, D and Baron, S and Beck, HP and Belhorma, B and Benchekroun, D and Benjamin, DP and Benslama, K and Bergeaas Kuutmann and E and Bertelsen,
             H and Binet, S and Biscarat, C and Boldea, V and Bondarenko, VG and Boonekamp, M and Bosman, M and Bourdarios, C and Burckhart Chromek,
             D and Bychkov, V and Callahan, J and Calvet, D and Canneri, M and Capeáns
             Garrido, M and Caprini, M and Cardiel Sas and L and Carli, T and Carminati,
             L and Carvalho, J and Cascella, M and Castillo, MV and Catinaccio, A and Cavalli Sforza and M and Cavalli, D and Cavasinni, V and Cetin, SA and Chen, H and Cherkaoui, R and Chevallier, F and Ciobotaru, M and Citterio, M and Cleland, B and Cogneras, E and Conde Muino and P and Consonni, M and Constantinescu, S and Cornelissen, T and Corso Radu,
             A and Costa, G and Cwetanski, P and Da Silva and D and Dam, M and Danielsson,
             HO and Dannheim, D and Davidek, T and De, K and Defay, PO and Dekhissi, B and Del Peso and J and Delmastro, M and Del Prete and T and Derue, F and Di
             Ciaccio, L and Di Girolamo and B and Dita, S and Dittus, F and Djama, F and Djobava, T and Dobson, M and Dolgoshein, BA and Dotti, A and Drake, G and Dressnandt, N and Driouchi, C and Ebenstein, WL and Eerola, P and Efthymiopoulos, I and Egorov, K and Eifert, TF and El Kacimi and M and Etienvre, AI and Fabich, A and Fakhr-Edine, AI and Fanti, M and Farbin,
             A and Farthouat, P and Fassouliotis, D},
   Title = {Study of energy response and resolution of the ATLAS barrel
             calorimeter to hadrons of energies from 20 to 350
             GeV},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {621},
   Number = {1-3},
   Pages = {134-150},
   Publisher = {Elsevier BV},
   Year = {2010},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.nima.2010.04.054},
   Abstract = {A fully instrumented slice of the ATLAS detector was exposed
             to test beams from the SPS (Super Proton Synchrotron) at
             CERN in 2004. In this paper, the results of the measurements
             of the response of the barrel calorimeter to hadrons with
             energies in the range 20350 GeV and beam impact points and
             angles corresponding to pseudo-rapidity values in the range
             0.20.65 are reported. The results are compared to the
             predictions of a simulation program using the Geant 4
             toolkit. © 2010 Published by Elsevier B.V.},
   Doi = {10.1016/j.nima.2010.04.054},
   Key = {fds309367}
}

@article{fds309368,
   Author = {Bethke, S and Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Antos, J and Apollinari,
             G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Azzurri, P and Badgett, W and Barnett, BA and Bartsch, V and Beecher, D and Behari, S and Bellettini, G and Benjamin, D and Bisello, D and Bizjak,
             I and Blocker, C and Blumenfeld, B and Bocci, A and Boisvert, V and Bolla,
             G and Bortoletto, D and Boudreau, J and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Canelli, F and Carls,
             B and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli,
             D and Chou, JP and Chung, K and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and Dell'Orso, M and Demortier,
             L and Deng, J and Deninno, M and di Giovanni, GP and Di Ruzza and B and Dittmann, JR and Donati, S and Donini, J and Dorigo, T and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fedorko,
             WT},
   Title = {Comments and Reply on: "Study of multi-muon events produced
             in pp̄ interactions at √s = 1.96 TeV"; T. Aaltonen et al.
             (The CDF collaboration)},
   Journal = {European Physical Journal C},
   Volume = {68},
   Number = {1},
   Pages = {119-123},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1337-z},
   Abstract = {The European Physical Journal C-Particles and
             Fields-publishes scientific manuscripts of relevance to the
             scientific community following careful and strict peer
             reviewing and, whenever appropriate and necessary, through
             discussion with the authors, so as to optimise scientific
             content and style of presentation prior to publication. In
             some cases significant disagreement between authors and
             referees (and/or editors) of the journal cannot be resolved
             despite all efforts and best of intentions. While the
             journal-notwithstanding any appeals-retains the right to
             reject such manuscripts, the editors of this journal may
             decide, in cases deemed of exceptional interest and
             potential significance for the field, to accept the
             manuscript for publication, to amend it by "comments" of the
             editor(s) in charge and, if appropriate, by a "reply" of the
             authors of the commented manuscript. The present comment is
             on "Study of multi-muon events produced in pp̄ interactions
             at √ = 1.96 TeV"; T. Aaltonen et al. (The CDF
             Collaboration, Eur. Phys. J. C, 2010, doi:10.1140/epjc/s10052-010-1336-0.
             © 2010 The Author(s).},
   Doi = {10.1140/epjc/s10052-010-1337-z},
   Key = {fds309368}
}

@article{fds309326,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of W-Boson Polarization in Top-Quark Decay in
             ppbar Collisions at sqrt{s}=1.96 TeV},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {4},
   Pages = {042002},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.042002},
   Abstract = {We report measurements of the polarization of W bosons from
             top-quark decays using 2.7 fb{-1} of pp collisions collected
             by the CDF II detector. Assuming a top-quark mass of
             175  GeV/c{2}, three measurements are performed. A
             simultaneous measurement of the fraction of longitudinal
             (f{0}) and right-handed (f{+}) W bosons yields the
             model-independent results f{0}=0.88±0.11(stat)±0.06(syst)
             and f{+}=-0.15±0.07(stat)±0.06(syst) with a correlation
             coefficient of -0.59. A measurement of f{0} [f{+}]
             constraining f{+} [f{0}] to its standard model value of 0.0
             [0.7] yields f{0}=0.70±0.07(stat)±0.04(syst)
             [f{+}=-0.01±0.02(stat)±0.05(syst)]. All these results are
             consistent with standard model expectations. We achieve the
             single most precise measurements of f{0} for both the
             model-independent and model-dependent determinations.},
   Doi = {10.1103/PhysRevLett.105.042002},
   Key = {fds309326}
}

@article{fds309343,
   Author = {Aaltonen, and T, and others},
   Title = {Combined Tevatron upper limit on $gg\rightarrow{}H\rightarrow{}W^{+}W^{-}$
             and constraints on the Higgs boson mass in fourth-generation
             fermion models},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {1},
   Pages = {011102},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.011102},
   Abstract = {We combine results from searches by the CDF and D0
             collaborations for a standard model Higgs boson (H) in the
             process gg→H→W+W - in pp̄ collisions at the Fermilab
             Tevatron Collider at √s=1.96TeV. With 4.8fb-1 of
             integrated luminosity analyzed at CDF and 5.4fb-1 at D0, the
             95% confidence level upper limit on σ(gg→H)×B(H→W+W-)
             is 1.75 pb at mH=120GeV, 0.38 pb at mH=165GeV, and 0.83 pb
             at mH=200GeV. Assuming the presence of a fourth sequential
             generation of fermions with large masses, we exclude at the
             95% confidence level a standard-model-like Higgs boson with
             a mass between 131 and 204 GeV. © 2010 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.82.011102},
   Key = {fds309343}
}

@article{fds309348,
   Author = {Aaltonen, T and Adelman, J and Álvarez Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M},
   Title = {Erratum: Measurement of the W+W-
             production cross section and search for anomalous WWγ and
             WWZ couplings in pp̄ collisions at √s=1.96 TeV (Phys.
             Rev. Lett. (2010) 104 (201801))},
   Journal = {Physical Review Letters},
   Volume = {105},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.019905},
   Doi = {10.1103/PhysRevLett.105.019905},
   Key = {fds309348}
}

@article{fds309324,
   Author = {Aaltonen, and T, and others},
   Title = {Exclusion of an Exotic Top Quark with -4/3 Electric Charge
             Using Soft Lepton Tagging},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {10},
   Pages = {101801},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.101801},
   Abstract = {We present a measurement of the electric charge of the top
             quark using pp collisions corresponding to an integrated
             luminosity of 2.7 fb(-1) at the CDF II detector. We
             reconstruct tt events in the lepton + jets final state. We
             use soft lepton taggers to determine the flavor of the b
             jets, which we use to reconstruct the top quark's electric
             charge and exclude an exotic top quark with -4/3 charge at
             95% confidence level. This is the strongest exclusion of the
             exotic charge scenario and the first to use soft leptons for
             this purpose.},
   Doi = {10.1103/PhysRevLett.105.101801},
   Key = {fds309324}
}

@article{fds309349,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of $Z\gamma{}$ production in $pp[over
             \ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
             $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {3},
   Pages = {031103},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.031103},
   Abstract = {The production rate and kinematics of photons produced in
             association with Z bosons are studied using 2fb-1 of pp̄
             collision data collected at the Collider Detector at
             Fermilab. The cross section for pp̄→"+-γ+X (where the
             leptons " are either muons or electrons with dilepton mass
             M>40GeV/c2, and where the photon has transverse energy
             ETγ>7GeV and is well separated from the leptons) is
             4.6±0.2(stat)±0.3(syst)±0.3(lum)pb, which is consistent
             with standard model expectations. We use the photon ET
             distribution from Zγ events where the Z has decayed to
             μ+μ -, e+e-, or νν̄ to set limits on anomalous (non
             standard model) trilinear couplings between photons and Z
             bosons. © 2010 The American Physical Society.},
   Doi = {10.1103/PhysRevD.82.031103},
   Key = {fds309349}
}

@article{fds309323,
   Author = {Aaltonen, and T, and others},
   Title = {Search for New Physics with a Dijet Plus Missing $E_{T}$
             Signature in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
             Collisions at $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {13},
   Pages = {131801},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.131801},
   Abstract = {We present results of a signature-based search for new
             physics using a dijet plus missing transverse energy (E(T))
             data sample collected in 2  fb⁻¹ of pp collisions at
             √s=1.96  TeV with the CDF II detector at the Fermilab
             Tevatron. We observe no significant event excess with
             respect to the standard model prediction and extract a 95%
             C.L. upper limit on the cross section times acceptance for a
             potential contribution from a nonstandard model process. The
             search is made by using novel, data-driven techniques for
             estimating backgrounds that are applicable to first searches
             at the LHC.},
   Doi = {10.1103/PhysRevLett.105.131801},
   Key = {fds309323}
}

@article{fds309352,
   Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, J and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
             A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
             J},
   Title = {Measurement of dσ/dy of Drell-Yan e+e-
             pairs in the Z mass region from pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {692},
   Number = {4},
   Pages = {232-239},
   Publisher = {Elsevier BV},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2010.06.043},
   Abstract = {We report on a CDF measurement of the total cross section
             and rapidity distribution, dσ/dy, for γ*Z→e+e- events in
             the Z boson mass region (66<Mee<116 GeV/c2) produced in pp-
             collisions at s=1.96 TeV with 2.1 fb-1 of integrated
             luminosity. The measured cross section of 257±16 pb and
             dσ/dy distribution are compared with Next-to-Leading-Order
             (NLO) and Next-to-Next-to-Leading-Order (NNLO) QCD theory
             predictions with CTEQ and MRST/MSTW parton distribution
             functions (PDFs). There is good agreement between the
             experimental total cross section and dσ/dy measurements
             with theoretical calculations with the most recent NNLO
             PDFs. © 2010 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2010.06.043},
   Key = {fds309352}
}

@article{fds309356,
   Author = {Aaltonen, and T, and others},
   Title = {Search for anomalous production of events with two photons
             and additional energetic objects at CDF},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {5},
   Pages = {052005},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.052005},
   Abstract = {We present results of a search for anomalous production of
             two photons together with an electron, muon, τ lepton,
             missing transverse energy, or jets using pp̄ collision data
             from 1.1-2.0fb-1 of integrated luminosity collected by the
             Collider Detector at Fermilab (CDF). The event yields and
             kinematic distributions are examined for signs of new
             physics without favoring a specific model of new physics.
             The results are consistent with the standard model
             expectations. The search employs several new analysis
             techniques that significantly reduce instrumental
             backgrounds in channels with an electron and missing
             transverse energy. © 2010 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.82.052005},
   Key = {fds309356}
}

@article{fds309361,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the top pair production cross section in the
             dilepton decay channel in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
             collisions at $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {5},
   Pages = {052002},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.052002},
   Abstract = {A measurement of the tt̄ production cross section in pp̄
             collisions at √s=1.96TeV using events with two leptons,
             missing transverse energy, and jets is reported. The data
             were collected with the CDF II detector. The result in a
             data sample corresponding to an integrated luminosity
             2.8fb-1 is σtt̄=6.27±0.73(stat) ±0.63(syst)±0.39(lum)pb.
             for an assumed top mass of 175GeV/c2. © 2010 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.82.052002},
   Key = {fds309361}
}

@article{fds309322,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adorisio, C and Adragna,
             P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli,
             G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Aktas,
             A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Ambrosio, G and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Argyropoulos,
             T and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong,
             SR and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai,
             M and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain,
             T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos
             Santos Pedrosa and F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Baranov, SP and Baranov, S and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, M and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Bartsch, D and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Bazalova,
             M and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, GA and Beck, HP and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bednyakov, VA and Bee, C and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Belhorma, B and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, G and Bellomo, M and Belloni, A and Belotskiy,
             K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benedict, BH and Benekos, N and Benhammou,
             Y and Benincasa, GP and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertin, A and Bertinelli, F and Bertolucci, F and Bertolucci, S and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Biesiada, J and Biglietti, M and Bilokon, H and Binder, M and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat,
             C and Bischof, R and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blocker, C and Blocki, J and Blondel, A and Blum,
             W and Blumenschein, U and Boaretto, C and Bobbink, GJ and Bocci, A and Bocian, D and Bock, R and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Booth, P and Booth, JRA and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Boveia,
             A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Braccini, S and Bracinik, J and Braem, A and Brambilla, E and Branchini,
             P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Brett, ND and Bright-Thomas, PG and Britton, D and Brochu, FM and Brock, I and Brock,
             R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brubaker, E and Bruckman
             de Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Buis, EJ and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Byatt, T and Caballero, J and Cabrera
             Urbán, S and Caccia, M and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Camard, A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Caprio, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino,
             G and Carminati, L and Caron, B and Caron, S and Carpentieri, C and Carrillo Montoya and GD and Carron Montero and S and Carter, AA and Carter,
             JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso,
             C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavallari, A and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Cazzato, A and Ceradini, F and Cerna, C and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cervetto, M and Cetin,
             SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, H and Chen, L and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Tcherniatine, V and Chesneanu, D and Cheu, E and Cheung, SL and Chevalier, L and Chevallier, F and Chiarella, V and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R},
   Title = {Search for new particles in two-jet final states in 7 TeV
             proton-proton collisions with the ATLAS detector at the
             LHC.},
   Journal = {Physical review letters},
   Volume = {105},
   Number = {16},
   Pages = {161801},
   Year = {2010},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.105.161801},
   Abstract = {A search for new heavy particles manifested as resonances in
             two-jet final states is presented. The data were produced in
             7 TeV proton-proton collisions by the LHC and correspond to
             an integrated luminosity of 315  nb⁻¹ collected by
             the ATLAS detector. No resonances were observed. Upper
             limits were set on the product of cross section and signal
             acceptance for excited-quark (q*) production as a function
             of q* mass. These exclude at the 95% C.L. the q* mass
             interval 0.30<m(q*)<1.26  TeV, extending the reach of
             previous experiments.},
   Doi = {10.1103/physrevlett.105.161801},
   Key = {fds309322}
}

@article{fds309321,
   Author = {Aaltonen, and T, and others},
   Title = {Search for $R$-Parity Violating Decays of Sneutrinos to
             $e\mu{}$, $\mu{}\tau{}$, and $e\tau{}$ Pairs in $pp[over
             \ifmmode\bar\else\textasciimacron\fi{}]$ Collisions at
             $\sqrt{s}=1.96\,\,TeV$},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {19},
   Pages = {191801},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.191801},
   Abstract = {We present a search for supersymmetric neutrino ν
             production using the Tevatron pp collision data collected
             with the CDF II detector and corresponding to an integrated
             luminosity of 1 fb-1. We focus on the scenarios predicted by
             the R-parity violating (RPV) supersymmetric models in which
             sneutrinos decay to two charged leptons of different flavor.
             With the data consistent with the standard model
             expectations, we set upper limits on σ(pp→ν)×BR(ν→eμ,μτ,eτ)
             and use these results to constrain the RPV couplings as a
             function of the sneutrino mass.},
   Doi = {10.1103/PhysRevLett.105.191801},
   Key = {fds309321}
}

@article{fds309363,
   Author = {Aaltonen, and T, and others},
   Title = {Updated search for the flavor-changing neutral-current decay
             $D^{0}\rightarrow{}\mu{}^{+}\mu{}^{-}$ in $pp[over
             \ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
             $\sqrt{s}=1.96$ TeV},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {9},
   Pages = {091105},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.091105},
   Abstract = {We report on a search for the flavor-changing
             neutral-current decay D0→μ⊃+μ⊃- in pp̄ collisions
             at √s=1.96TeV using 360pb⊃-1 of integrated luminosity
             collected by the CDF II detector at the Fermilab Tevatron
             collider. A displaced vertex trigger selects long-lived D0
             candidates in the μ⊃+μ⊃-, π⊃+π⊃-, and
             K⊃-π⊃+ decay modes. We use the Cabibbo-favored
             D0→K⊃- π⊃+ channel to optimize the selection criteria
             in an unbiased manner, and the kinematically similar
             D0→π⊃+π⊃- channel for normalization. We set an upper
             limit on the branching fraction B(D0→μ⊃+μ⊃-)<2.1×10⊃-7(3.0×10⊃-7)
             at the 90% (95%) confidence level. © 2010 The American
             Physical Society.},
   Doi = {10.1103/PhysRevD.82.091105},
   Key = {fds309363}
}

@article{fds309366,
   Author = {Abat, E and Abdallah, JM and Addy, TN and Adragna, P and Aharrouche, M and Ahmad, A and Akesson, TPA and Aleksa, M and Alexa, C and Anderson, K and Andreazza, A and Anghinolfi, F and Antonaki, A and Arabidze, G and Arik,
             E and Atkinson, T and Baines, J and Baker, OK and Banfi, D and Baron, S and Barr, AJ and Beccherie, R and Beck, HP and Belhorma, B and Bell, PJ and Benchekroun, D and Benjamin, DP and Benslama, K and Kuutmann, EB and Bernabeu, J and Bertelsen, H and Binet, S and Biscarat, C and Boldea, V and Bondarenko, VG and Boonekamp, M and Bosman, M and Bourdarios, C and Broklova, Z and Chromek, DB and Bychkov, V and Callahan, J and Calvet,
             D and Canneri, M and Garrido, MC and Caprini, M and Sas, LC and Carli, T and Carminati, L and Carvalho, J and Cascella, M and Castillo, MV and Catinaccio, A and Cauz, D and Cavalli, D and Sforza, MC and Cavasinni,
             V and Cetin, SA and Chen, H and Cherkaoui, R and Chevalier, L and Chevallier, F and Chouridou, S and Ciobotaru, M and Citterio, M and Clark, A and Cleland, B and Cobal, M and Cogneras, E and Muino, PC and Consonni, M and Constantinescu, S and Cornelissen, T and Correard, S and Radu, AC and Costa, G and Costa, MJ and Costanzo, D and Cuneo, S and Cwetanski, P and Da Silva and D and Dam, M and Dameri, M and Danielsson,
             HO and Dannheim, D and Darbo, G and Davidek, T and De, K and Defay, PO and Dekhissi, B and Del Peso and J and Del Prete and T and Delmastro, M and Derue,
             F and Di Ciaccio and L and Di Girolamo and B and Dita, S and Dittus, F and Djama,
             F and Djobava, T},
   Title = {Combined performance studies for electrons at the 2004 ATLAS
             combined test-beam},
   Journal = {Journal of Instrumentation},
   Volume = {5},
   Number = {11},
   Pages = {P11006-P11006},
   Publisher = {IOP Publishing},
   Year = {2010},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1748-0221/5/11/P11006},
   Abstract = {In 2004 at the ATLAS (A Toroidal LHC ApparatuS) combined
             test beam, one slice of the ATLAS barrel detector (including
             an Inner Detector set-up and the Liquid Argon calorimeter)
             was exposed to particles from the H8 SPS beam line at CERN.
             It was the first occasion to test the combined electron
             performance of ATLAS. This paper presents results obtained
             for the momentum measurement p with the Inner Detector and
             for the performance of the electron measurement with the LAr
             calorimeter (energy E linearity and resolution) in the
             presence of a magnetic field in the Inner Detector for
             momenta ranging from 20 GeV/c to 100 GeV/c. Furthermore the
             particle identification capabilities of the Transition
             Radiation Tracker, Bremsstrahlungs-recovery algorithms
             relying on the LAr calorimeter and results obtained for the
             E/p ratio and a way how to extract scale parameters will be
             discussed. © 2010 IOP Publishing Ltd and
             SISSA.},
   Doi = {10.1088/1748-0221/5/11/P11006},
   Key = {fds309366}
}

@article{fds309317,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Silva, J and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge,
             E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen,
             D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Pedrosa, FBDS and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, C and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, G and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benedict,
             BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocci, A and Bock, R and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov,
             A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boonekamp, M and Boorman, G and Booth, CN and Booth, P and Booth, JRA and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Brambilla, E and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Brett, ND and Bright-Thomas, PG and Britton, D and Brochu, FM and Brock, I and Brock,
             R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brubaker, E and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Buis, EJ and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Urbán,
             SC and Caccia, M and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camard, A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino,
             G and Carminati, L and Caron, B and Caron, S and Carpentieri, C and Montoya, GDC and Montero, SC and Carter, AA and Carter, JR and Carvalho,
             J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
             AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
             G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavallari, A and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Cazzato, A and Ceradini, F and Cerna, C and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty,
             D and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre,
             E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, H and Chen, L and Chen, S and Chen,
             T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and El
             Moursli, RC and Tcherniatine, V and Cheu, E and Cheung, SL and Chevalier, L and Chevallier, F and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {Observation of a centrality-dependent dijet asymmetry in
             lead-lead collisions at sqrt[S(NN)] =2.76 TeV with the ATLAS
             detector at the LHC.},
   Journal = {Physical review letters},
   Volume = {105},
   Number = {25},
   Pages = {252303},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.105.252303},
   Abstract = {By using the ATLAS detector, observations have been made of
             a centrality-dependent dijet asymmetry in the collisions of
             lead ions at the Large Hadron Collider. In a sample of
             lead-lead events with a per-nucleon center of mass energy of
             2.76 TeV, selected with a minimum bias trigger, jets are
             reconstructed in fine-grained, longitudinally segmented
             electromagnetic and hadronic calorimeters. The transverse
             energies of dijets in opposite hemispheres are observed to
             become systematically more unbalanced with increasing event
             centrality leading to a large number of events which contain
             highly asymmetric dijets. This is the first observation of
             an enhancement of events with such large dijet asymmetries,
             not observed in proton-proton collisions, which may point to
             an interpretation in terms of strong jet energy loss in a
             hot, dense medium.},
   Doi = {10.1103/physrevlett.105.252303},
   Key = {fds309317}
}

@article{fds309318,
   Author = {Aaltonen, and T, and others},
   Title = {Top Quark Mass Measurement in the $lepton+jets$ Channel
             Using a Matrix Element Method and in situ Jet Energy
             Calibration},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {25},
   Pages = {252001},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.252001},
   Abstract = {A precision measurement of the top quark mass m(t) is
             obtained using a sample of tt events from pp collisions at
             the Fermilab Tevatron with the CDF II detector. Selected
             events require an electron or muon, large missing transverse
             energy, and exactly four high-energy jets, at least one of
             which is tagged as coming from a b quark. A likelihood is
             calculated using a matrix element method with quasi-Monte
             Carlo integration taking into account finite detector
             resolution and jet mass effects. The event likelihood is a
             function of m(t) and a parameter Δ(JES) used to calibrate
             the jet energy scale in situ. Using a total of 1087 events
             in 5.6 fb(-1) of integrated luminosity, a value of
             m(t)=173.0 ± 1.2 GeV/c(2) is measured.},
   Doi = {10.1103/PhysRevLett.105.252001},
   Key = {fds309318}
}

@article{fds309319,
   Author = {Aaltonen, and T, and others},
   Title = {Direct Top-Quark Width Measurement at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {105},
   Number = {23},
   Pages = {232003},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevLett.105.232003},
   Abstract = {We present a measurement of the top-quark width in the
             lepton+jets decay channel of tt events produced in p p
             collisions at Fermilab's Tevatron collider and collected by
             the CDF II detector. From a data sample corresponding to 4.3
             fb(-1) of integrated luminosity, we identify 756 candidate
             events. The top-quark mass and the mass of the hadronically
             decaying W boson that comes from the top-quark decay are
             reconstructed for each event and compared with templates of
             different top-quark widths (Γ(t)) and deviations from
             nominal jet energy scale (Δ(JES)) to perform a simultaneous
             fit for both parameters, where Δ(JES) is used for the in
             situ calibration of the jet energy scale. By applying a
             Feldman-Cousins approach, we establish an upper limit at 95%
             confidence level (CL) of Γ(t) <7.6 GeV and a two-sided 68%
             CL interval of 0.3 GeV <Γ(t) <4.4  GeV for a top-quark
             mass of 172.5 GeV/c(2), which are consistent with the
             standard model prediction.},
   Doi = {10.1103/PhysRevLett.105.232003},
   Key = {fds309319}
}

@article{fds309342,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Adorisio, C and Adragn, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Aktas, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimontia, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amelung, C and Amorima, A and Amorós, G and Amram, N and Anastopoulos,
             C and Andeen, T and Anders, CF and Anderson, KJ and Andreazzaa, A and Andreia, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjosa,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonellia, S and Antos, J and Antunovic, B and Anullia, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arika, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai, M and Asai, S and Asfandiyarov, R and Ask, S and Åsmana, B and Asner, D and Asquith, L and Assamagan, K and Astvatsatourov, A and Atoian, G and Auerbach, B and Augsten, K},
   Title = {Readiness of the ATLAS Tile Calorimeter for LHC
             collisions},
   Journal = {European Physical Journal C},
   Volume = {70},
   Number = {4},
   Pages = {1193-1236},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1508-y},
   Abstract = {The Tile hadronic calorimeter of the ATLAS detector has
             undergone extensive testing in the experimental hall since
             its installation in late 2005. The readout, control and
             calibration systems have been fully operational since 2007
             and the detector has successfully collected data from the
             LHC single beams in 2008 and first collisions in 2009. This
             paper gives an overview of the Tile Calorimeter performance
             as measured using random triggers, calibration data, data
             from cosmic ray muons and single beam data. The detector
             operation status, noise characteristics and performance of
             the calibration systems are presented, as well as the
             validation of the timing and energy calibration carried out
             with minimum ionising cosmic ray muons data. The calibration
             systems' precision is well below the design value of 1%. The
             determination of the global energy scale was performed with
             an uncertainty of 4%. © 2010 CERN for the benefit of the
             ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-010-1508-y},
   Key = {fds309342}
}

@article{fds309350,
   Author = {Aaltonen, and T, and others},
   Title = {Observation of single top quark production and measurement
             of |$V_{tb}|$ with CDF},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {11},
   Pages = {112005},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.112005},
   Abstract = {We report the observation of electroweak single top quark
             production in 3.2fb⊃-1 of pp̄ collision data collected by
             the Collider Detector at Fermilab at √s=1.96TeV. Candidate
             events in the W+jets topology with a leptonically decaying W
             boson are classified as signal-like by four parallel
             analyses based on likelihood functions, matrix elements,
             neural networks, and boosted decision trees. These results
             are combined using a super discriminant analysis based on
             genetically evolved neural networks in order to improve the
             sensitivity. This combined result is further combined with
             that of a search for a single top quark signal in an
             orthogonal sample of events with missing transverse energy
             plus jets and no charged lepton. We observe a signal
             consistent with the standard model prediction but
             inconsistent with the background-only model by 5.0 standard
             deviations, with a median expected sensitivity in excess of
             5.9 standard deviations. We measure a production cross
             section of 2.3-0.5+0.6(stat+sys)pb, extract the value of the
             Cabibbo-Kobayashi-Maskawa matrix element |Vtb|=0.91-0.11+0.
             11(stat+sys)±0.07(theory), and set a lower limit |Vtb|>0.71
             at the 95%C.L., assuming mt=175GeV/c2.},
   Doi = {10.1103/PhysRevD.82.112005},
   Key = {fds309350}
}

@article{fds309360,
   Author = {Aaltonen, and T, and others},
   Title = {Diffractive $W$ and $Z$ production at the Fermilab
             Tevatron},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {11},
   Pages = {112004},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.112004},
   Abstract = {We report on a measurement of the fraction of events with a
             W or Z boson which are produced diffractively in p̄p
             collisions at √s=1.96TeV, using data from 0.6fb⊃-1 of
             integrated luminosity collected with the CDFII detector
             equipped with a Roman-pot spectrometer that detects the p̄
             from p̄+p→p̄+[X+W/Z]. We find that (1.00±0.11)% of Ws
             and (0.88±0.22)% of Zs are produced diffractively in a
             region of antiproton or proton fractional momentum loss ξ
             of 0.03<ξ<0.10 and 4-momentum transferred squared t of
             -1<t<0(GeV/c)2, where we account for the events in which the
             proton scatters diffractively while the antiproton
             dissociates, p̄+p→[X+W/Z]+p, by doubling the measured
             proton dissociation fraction. We also report on searches for
             W and Z production in double Pomeron exchange,
             p+p̄→p+[X+W/Z]+p̄, and on exclusive Z production,
             p̄+p→p̄+Z+p. No signal is seen above background for
             these processes, and comparisons are made with expectations.
             © 2010 The American Physical Society.},
   Doi = {10.1103/PhysRevD.82.112004},
   Key = {fds309360}
}

@article{fds309364,
   Author = {Aaltonen, and T, and others},
   Title = {Measurement of the $WW+WZ$ production cross section using a
             matrix element technique in $lepton+jets$
             events},
   Journal = {Phys. Rev. D},
   Volume = {82},
   Number = {11},
   Pages = {112001},
   Publisher = {American Physical Society},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.112001},
   Abstract = {We present a measurement of the WW+WZ production cross
             section observed in a final state consisting of an
             identified electron or muon, two jets, and missing
             transverse energy. The measurement is carried out in a data
             sample corresponding to up to 4.6fb⊃-1 of integrated
             luminosity at √s=1.96TeV collected by the CDF II detector.
             Matrix element calculations are used to separate the diboson
             signal from the large backgrounds. The WW+WZ cross section
             is measured to be 17.4±3.3pb in agreement with standard
             model predictions. A fit to the dijet invariant mass
             spectrum yields a compatible cross section measurement. ©
             2010 The American Physical Society.},
   Doi = {10.1103/PhysRevD.82.112001},
   Key = {fds309364}
}

@article{fds309369,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acharya, BS and Adams, DL and Addy,
             TN and Adelman, J and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, E and Arik,
             M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai, M and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L},
   Title = {Drift Time Measurement in the ATLAS Liquid Argon
             Electromagnetic Calorimeter using Cosmic
             Muons},
   Journal = {European Physical Journal C},
   Volume = {70},
   Number = {3},
   Pages = {755-785},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1403-6},
   Abstract = {The ionization signals in the liquid argon of the ATLAS
             electromagnetic calorimeter are studied in detail using
             cosmic muons. In particular, the drift time of the
             ionization electrons is measured and used to assess the
             intrinsic uniformity of the calorimeter gaps and estimate
             its impact on the constant term of the energy resolution.
             The drift times of electrons in the cells of the second
             layer of the calorimeter are uniform at the level of 1.3% in
             the barrel and 2.8% in the endcaps. This leads to an
             estimated contribution to the constant term of
             (0.290.040.05)% in the barrel and (0.540.040.06)% in the
             endcaps. The same data are used to measure the drift
             velocity of ionization electrons in liquid argon, which is
             found to be 4.61±0.07 mm/μs at 88.5 K and 1 kV/mm. © 2010
             CERN for the benefit of the ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-010-1403-6},
   Key = {fds309369}
}

@article{fds309370,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acharya, BS and Adams, DL and Addy,
             TN and Adelman, J and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Antonaki, A and Antonelli, M and Antonelli, S and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai,
             M and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K},
   Title = {Readiness of the ATLAS liquid argon calorimeter for LHC
             collisions},
   Journal = {European Physical Journal C},
   Volume = {70},
   Number = {3},
   Pages = {723-753},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1354-y},
   Abstract = {The ATLAS liquid argon calorimeter has been operating
             continuously since August 2006. At this time, only part of
             the calorimeter was readout, but since the beginning of
             2008, all calorimeter cells have been connected to the ATLAS
             readout system in preparation for LHC collisions. This paper
             gives an overview of the liquid argon calorimeter
             performance measured in situ with random triggers,
             calibration data, cosmic muons, and LHC beam splash events.
             Results on the detector operation, timing performance,
             electronics noise, and gain stability are presented. High
             energy deposits from radiative cosmic muons and beam splash
             events allow to check the intrinsic constant term of the
             energy resolution. The uniformity of the electromagnetic
             barrel calorimeter response along η (averaged over Φ) is
             measured at the percent level using minimum ionizing cosmic
             muons. Finally, studies of electromagnetic showers from
             radiative muons have been used to cross-check the Monte
             Carlo simulation. The performance results obtained using the
             ATLAS readout, data acquisition, and reconstruction software
             indicate that the liquid argon calorimeter is well-prepared
             for collisions at the dawn of the LHC era. © 2010 CERN for
             the benefit of the ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-010-1354-y},
   Key = {fds309370}
}

@article{fds309372,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acharya, BS and Adams, DL and Addy,
             TN and Adelman, J and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alviggi, MG and Amako, K and Amelung, C and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai, M and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A},
   Title = {Commissioning of the ATLAS Muon Spectrometer with cosmic
             rays},
   Journal = {European Physical Journal C},
   Volume = {70},
   Number = {3},
   Pages = {875-916},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1415-2},
   Abstract = {The ATLAS detector at the Large Hadron Collider has
             collected several hundred million cosmic ray events during
             2008 and 2009. These data were used to commission the Muon
             Spectrometer and to study the performance of the trigger and
             tracking chambers, their alignment, the detector control
             system, the data acquisition and the analysis programs. We
             present the performance in the relevant parameters that
             determine the quality of the muon measurement. We discuss
             the single element efficiency, resolution and noise rates,
             the calibration method of the detector response and of the
             alignment system, the track reconstruction efficiency and
             the momentum measurement. The results show that the detector
             is close to the design performance and that the Muon
             Spectrometer is ready to detect muons produced in high
             energy proton-proton collisions. © 2010 CERN for the
             benefit of the ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-010-1415-2},
   Key = {fds309372}
}

@article{fds309373,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acharya, BS and Adams, DL and Addy,
             TN and Adelman, J and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander,
             G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alviggi, MG and Amako, K and Amelung, C and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai, M and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astvatsatourov, A and Atoian, G and Auerbach, B},
   Title = {The ATLAS Inner Detector commissioning and
             calibration},
   Journal = {European Physical Journal C},
   Volume = {70},
   Number = {3},
   Pages = {787-821},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1366-7},
   Abstract = {The ATLAS Inner Detector is a composite tracking system
             consisting of silicon pixels, silicon strips and straw tubes
             in a 2 T magnetic field. Its installation was completed in
             August 2008 and the detector took part in data-taking with
             single LHC beams and cosmic rays. The initial detector
             operation, hardware commissioning and in-situ calibrations
             are described. Tracking performance has been measured with
             7. 6 million cosmic-ray events, collected using a tracking
             trigger and reconstructed with modular pattern-recognition
             and fitting software. The intrinsic hit efficiency and
             tracking trigger efficiencies are close to 100%. Lorentz
             angle measurements for both electrons and holes, specific
             energy-loss calibration and transition radiation turn-on
             measurements have been performed. Different alignment
             techniques have been used to reconstruct the detector
             geometry. After the initial alignment, a transverse impact
             parameter resolution of 22. 1±0. 9 μm and a relative
             momentum resolution σp/p=(4. 83±0. 16)×10-4 GeV-1×pT
             have been measured for high momentum tracks. © 2010 CERN
             for the benefit of the ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-010-1366-7},
   Key = {fds309373}
}

@article{fds309341,
   Author = {Aad, G and Abat, E and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adorisio, C and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, PF and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Aktas, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Ambrosini, G and Ambrosio, G and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, E and Arik,
             M},
   Title = {Performance of the ATLAS detector using first collision
             data},
   Journal = {Journal of High Energy Physics},
   Volume = {2010},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP09(2010)056},
   Abstract = {More than half a million minimum-bias events of LHC
             collision data were collected by the ATLAS experiment in
             December 2009 at centre-of-mass energies of 0.9 TeV and 2.36
             TeV. This paper reports on studies of the initial
             performance of the ATLAS detector from these data.
             Comparisons between data and Monte Carlo predictions are
             shown for distributions of several track-and
             calorimeter-based quantities. The good performance of the
             ATLAS detector in these first data gives confidence for
             successful running at higher energies.},
   Doi = {10.1007/JHEP09(2010)056},
   Key = {fds309341}
}

@article{fds309346,
   Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
             D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
             C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
             D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
             WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
             A and Clark, D},
   Title = {Erratum: Measurement of particle production and inclusive
             differential cross sections in pp̄ collisions at
             √s=1.96TeV (Physical Review D - Particles, Fields,
             Gravitation and Cosmology)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {82},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2010},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.82.119903},
   Doi = {10.1103/PhysRevD.82.119903},
   Key = {fds309346}
}

@article{fds337204,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
             J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
             A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
             ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
             F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Tipton, P and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
             J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
             J},
   Title = {Evidence for tt̄γ production and measurement of
             σtt̄γtt̄},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {3},
   Year = {2011},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.031104},
   Abstract = {Using data corresponding to 6.0fb-1 of pp̄ collisions at
             √s=1.96TeV collected by the CDF II detector, we present a
             cross section measurement of top-quark pair production with
             an additional radiated photon in the central region with 10
             GeV or more of transverse energy tt̄γ. The events are
             selected by looking for a lepton (ℓ or μ), a photon (γ),
             significant transverse momentum imbalance (ET), large total
             transverse energy, and three or more jets, with at least one
             identified as containing a b quark (b). Using an event
             selection optimized for the tt̄γ candidate sample, we also
             measure the cross section of tt̄ (σtt̄). We measure the
             tt̄γ cross section (σtt̄γ) to be 0.18±0.08pb, and the
             ratio of σtt̄γ to σtt̄ to be 0.024±0.009. We observe a
             probability of 0.0015 (3.0 standard deviations) of the
             background (non-tt̄γ events alone producing 30 events or
             more. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.031104},
   Key = {fds337204}
}

@article{fds313358,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
   Title = {Search for Bs0→μ+μ- and
             B0→μ+μ- decays with CDF
             II},
   Journal = {Physical Review Letters},
   Volume = {107},
   Number = {19},
   Pages = {191801},
   Year = {2011},
   url = {http://www.ncbi.nlm.nih.gov/pubmed/22181596},
   Abstract = {A search has been performed for Bs0→μ+μ- and B0→μ+μ-
             decays using 7fb-1 of integrated luminosity collected by the
             CDF II detector at the Fermilab Tevatron collider. The
             observed number of B0 candidates is consistent with
             background-only expectations and yields an upper limit on
             the branching fraction of B(B0→μ+μ-)&lt;6.0×10-9 at 95%
             confidence level. We observe an excess of Bs0 candidates.
             The probability that the background processes alone could
             produce such an excess or larger is 0.27%. The probability
             that the combination of background and the expected standard
             model rate of Bs0→μ+μ- could produce such an excess or
             larger is 1.9%. These data are used to determine
             B(Bs0→μ+μ-)=(1.8-0.9+1.1)×10 -8 and provide an upper
             limit of B(Bs0→μ+μ -)&lt;4.0×10-8 at 95% confidence
             level. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevLett.107.191801},
   Key = {fds313358}
}

@article{fds313350,
   Author = {Aaltonen, T and González, BÃ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
             WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
             YC},
   Title = {Measurements of the properties of Λc(2595),
             Λc(2625), Σc(2455), and Σ
             c(2520) baryons},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {1},
   Year = {2011},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.012003},
   Abstract = {We report measurements of the resonance properties of Λ
             c(2595)+ and Λc(2625)+ baryons in their decays to
             Λc+π+π- as well as Σc(2455)++,0 and Σ c(2520)++,0
             baryons in their decays to Λc+π± final states. These
             measurements are performed using data corresponding to
             5.2fb-1 of integrated luminosity from pp̄ collisions at
             √s=1.96TeV, collected with the CDF II detector at the
             Fermilab Tevatron. Exploiting the largest available charmed
             baryon sample, we measure masses and decay widths with
             uncertainties comparable to the world averages for Σc
             states, and significantly smaller uncertainties than the
             world averages for excited Λc+ states. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.84.012003},
   Key = {fds313350}
}

@article{fds329532,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
             C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
             M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
             S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
             JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
             MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
   Title = {Erratum: Search for Bs0→μ+μ- and
             B0→μ+μ- decays with CDF II
             (Physical Review Letters (2011) 107 (191801))},
   Journal = {Physical Review Letters},
   Volume = {107},
   Number = {23},
   Year = {2011},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.239903},
   Doi = {10.1103/PhysRevLett.107.239903},
   Key = {fds329532}
}

@article{fds325319,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, A and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoros, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antosb, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchou, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Boeser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
             JM and Buttinger, W and Byatt, T and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Measurement of the inclusive and dijet cross-sections of
             b-jets in pp collisions at √s=7 TeV
             with the ATLAS detector},
   Journal = {EUROPEAN PHYSICAL JOURNAL C},
   Volume = {71},
   Number = {12},
   Publisher = {Springer New York LLC},
   Year = {2011},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1846-4},
   Abstract = {The inclusive and dijet production cross-sections have been
             measured for jets containing b-hadrons (b-jets) in
             proton-proton collisions at a centre-of-mass energy of +fs =
             7 TeV, using the ATLAS detector at the LHC. The measurements
             use data corresponding to an integrated luminosity of 34
             pb_1. The b-jets are identified using either a
             lifetime-based method, where secondary decay vertices of
             b-hadrons in jets are reconstructed using information from
             the tracking detectors, or a muon-based method where the
             presence of a muon is used to identify semileptonic decays
             of b-hadrons inside jets. The inclusive b-jet cross-section
             is measured as a function of transverse momentum in the
             range 20 < pT < 400 GeV and rapidity in the range \y\ < 2.1.
             The bb-dijet cross-section is measured as a function of the
             dijet invariant mass in the range 110 < mjj < 760 GeV, the
             azimuthal angle difference between the two jets and the
             angular variable χ in two dijet mass regions. The results
             are compared with next-to-leading-order QCD predictions.
             Good agreement is observed between the measured
             cross-sections and the predictions obtained using POWHEG +
             Pythia. MC@NLO + Herwig shows good agreement with the
             measured bb-dijet cross-section. However, it does not
             reproduce the measured inclusive cross-section well,
             particularly for central b-jets with large transverse
             momenta.},
   Doi = {10.1140/epjc/s10052-011-1846-4},
   Key = {fds325319}
}

@article{fds325320,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TP and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoros, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimaraes da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Boeser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
             JM and Buttinger, W and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
             M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall,
             J},
   Title = {Search for massive colored scalars in four-jet final states
             in √s=7 TeV proton-proton collisions with the ATLAS
             detector},
   Journal = {EUROPEAN PHYSICAL JOURNAL C},
   Volume = {71},
   Number = {12},
   Publisher = {Springer New York LLC},
   Year = {2011},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1828-6},
   Abstract = {A search for pair-produced scalar particles decaying to a
             four-jet final state is presented. The analysis is performed
             using an integrated luminosity of 34 pb-1 recorded by the
             ATLAS detector in 2010. No deviation from the Standard Model
             is observed. For a scalar mass of 100 GeV (190 GeV) the
             limit on the scalar gluon pair production cross section at
             95% confidence level is 1 nb (0.28 nb). When these results
             are interpreted as mass limits, scalar-gluons (hyperpions)
             with masses of 100 to 185 GeV (100 to 155 GeV) are excluded
             at 95% confidence level with the exception of a mass window
             of width about 5 GeV (15 GeV) around 140
             GeV.},
   Doi = {10.1140/epjc/s10052-011-1828-6},
   Key = {fds325320}
}

@article{fds199959,
   Author = {ATLAS collaboration},
   Title = {Search for high-mass states with one lepton plus missing
             transverse momentum in proton-proton collisions at Ecm = 7
             TeV with the ATLAS detecto},
   Journal = {Phys. Lett. B701(2011) 50},
   Year = {2011},
   Key = {fds199959}
}

@article{fds199960,
   Author = {ATLAS Collaboration},
   Title = {Search for a heavy particle decaying into an electron and a
             muon with the ATLAS detector in Ecm = 7 TeV pp collisions at
             the LHC},
   Journal = {Phys. Rev. Lett. 106, 251801 (2011)},
   Year = {2011},
   Key = {fds199960}
}

@article{fds199961,
   Author = {ATLAS Collaboration},
   Title = {Measurement of the WW cross section in Ecm = 7 TeV pp
             collisions with ATLAS},
   Journal = {Phys. Rev. Lett. 107, 041802 (2011)},
   Year = {2011},
   Key = {fds199961}
}

@article{fds199968,
   Author = {CDF Collaboration},
   Title = {Search for New Heavy Gauge Boson W' with Event Signature
             Electron+Missing Transverse Energy in p anti-p Collisions at
             Ecm=1.96 TeV},
   Journal = {Phys. Rev. D83, 031102 (2011)},
   Year = {2011},
   Key = {fds199968}
}

@article{fds199969,
   Author = {CDF collaboration},
   Title = {Search for New Heavy Gauge Boson W' with Event Signature
             Electron+Missing Transverse Energy in p anti-p Collisions at
             Ecm= 1.96 TeV},
   Journal = {Phys. Rev. D83, 112008 (2011)},
   Year = {2011},
   Key = {fds199969}
}

@article{fds321641,
   Author = {Liang, Z and Martin, B and Meyer, J and Tanaka, S and Thompson, PD and Wang, J and Yang, Y and Yu, J and Zimmermann, S and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi,
             B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov,
             VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonelli,
             S and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui,
             S and Arguin, JF and Arik, E and Arik, M},
   Title = {Measurements of underlying-event properties using neutral
             and charged particles in pp collisions at √s = 900 GeV and
             √s = 7 TeV with the ATLAS detector at the
             LHC},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1636-z},
   Abstract = {We present first measurements of charged and neutral
             particle-flow correlations in pp collisions using the ATLAS
             calorimeters.Data were collected in 2009 and 2010 at
             centre-of-mass energies of 900 GeV and 7 TeV.Events were
             selected using a minimum-bias trigger which required a
             charged particle in scintillation counters on either side of
             the interaction point.Particle flows, sensitive to the
             underlying event, are measured using clusters of energy in
             the ATLAS calorimeters, taking advantage of their fine
             granularity.No Monte Carlo generator used in this analysis
             can accurately describe the measurements.The results are
             independent of those based on charged particles measured by
             the ATLAS tracking systems and can be used to constrain the
             parameters of Monte Carlo generators.},
   Doi = {10.1140/epjc/s10052-011-1636-z},
   Key = {fds321641}
}

@article{fds321642,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Measurement of the top quark-pair production cross section
             with ATLAS in pp collisions at √s = 7 TeV},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1577-6},
   Abstract = {A measurement of the production cross-section for top quark
             pairs (tt̅) in pp collisions at √s =7 TeVis presented
             using data recorded with the ATLAS detector at the Large
             Hadron Collider. Events are selected in two different
             topologies: single lepton (electron e or muon μ) with large
             missing transverse energy and at least four jets, and
             dilepton (ee, μμ or eμ) with large missing transverse
             energy and at least two jets. In a data sample of 2.9
             pb–1, 37 candidate events are observed in the
             single-lepton topology and 9 events in the dilepton
             topology. The corresponding expected backgrounds from
             non-tt̅ Standard Model processes are estimated using
             data-driven methods and determined to be 12.2 ± 3.9 events
             and 2.5± 0.6 events, respectively. The kinematic properties
             of the selected events are consistent with SM tt̅
             production. The inclusive top quark pair production
             cross-section is measured to be The measurement agrees with
             perturbative QCD calculations.},
   Doi = {10.1140/epjc/s10052-011-1577-6},
   Key = {fds321642}
}

@article{fds321643,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adorisio, C and Adragna,
             P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli,
             G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas,
             A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Ambrosio, G and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Argyropoulos,
             T and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong,
             SR and Arnaez, O},
   Title = {Measurement of inclusive jet and dijet cross sections in
             proton-proton collisions at 7 TeV centre-of-mass energy with
             the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {2},
   Pages = {1-59},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-010-1512-2},
   Abstract = {Jet cross sections have been measured for the first time in
             proton-proton collisions at a centre-of-mass energy of 7 TeV
             using the ATLAS detector. The measurement uses an integrated
             luminosity of 17 nb−1 recorded at the Large Hadron
             Collider. The anti-kt algorithm is used to identify jets,
             with two jet resolution parameters, R = 0.4 and 0.6. The
             dominant uncertainty comes from the jet energy scale, which
             is determined to within 7% for central jets above 60 GeV
             transverse momentum. Inclusive single-jet differential cross
             sections are presented as functions of jet transverse
             momentum and rapidity. Dijet cross sections are presented as
             functions of dijet mass and the angular variable χ. The
             results are compared to expectations based on
             next-toleading- order QCD, which agree with the data,
             providing a validation of the theory in a new kinematic
             regime.},
   Doi = {10.1140/epjc/s10052-010-1512-2},
   Key = {fds321643}
}

@article{fds320780,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for new phenomena in final states with large jet
             multiplicities and missing transverse momentum using √s =
             7 TeV pp collisions with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2011)099},
   Abstract = {Results are presented of a search for any particle(s)
             decaying to six or more jets in association with missing
             transverse momentum. The search is performed using
             1.34fb−1 of √s = 7 TeV proton-proton collisions recorded
             by the ATLAS detector during 2011. Data-driven techniques
             are used to determine the backgrounds in kinematic regions
             that require at least six, seven or eight jets, well beyond
             the multiplicities required in previous analyses. No
             evidence is found for physics beyond the Standard Model. The
             results are interpreted in the context of a supersymmetry
             model (MSUGRA/CMSSM) where they extend previous
             constraints.},
   Doi = {10.1007/JHEP11(2011)099},
   Key = {fds320780}
}

@article{fds309237,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for diphoton events with large missing transverse
             energy with 36 pb-1 of 7 TeV proton-proton
             collision data with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1744-9},
   Abstract = {Making use of 36 pb-1 of proton-proton collision data at
             √s = 7 TeV, the ATLAS Collaboration has performed a search
             for diphoton events with large missing transverse energy.
             Observing no excess of events above the Standard Model
             prediction, a 95% Confidence Level (CL) upper limit is set
             on the cross section for new physics of σ < 0.38-0.65 pb in
             the context of a generalised model of gauge-mediated
             supersymmetry breaking (GGM) with a bino-like lightest
             neutralino, and of σ < 0.18-0.23 pb in the context of a
             specific model with one universal extra dimension (UED). A
             95% CL lower limit of 560 GeV, for bino masses above 50 GeV,
             is set on the GGM gluino mass, while a lower limit of 1/R >
             961 GeV is set on the UED compactification radius R. These
             limits provide the most stringent tests of these models to
             date.},
   Doi = {10.1140/epjc/s10052-011-1744-9},
   Key = {fds309237}
}

@article{fds309241,
   Author = {Aaltonen, T and ÁlvarezGonzález, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan,
             A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg,
             C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd,
             S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha,
             C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
             YC and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De Cecco and S},
   Title = {Improved determination of the sample composition of dimuon
             events produced in pp̄ collisions at √s=1.96
             TeV},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {8},
   Pages = {1-14},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1720-4},
   Abstract = {We use a new method to estimate with 5% accuracy the
             contribution of pion and kaon in-flight-decays to the dimuon
             data set acquired with the CDF detector. Based on this
             improved estimate, we show that the total number and the
             properties of the collected dimuon events are not yet
             accounted for by ordinary sources of dimuons which also
             include the contributions, as measured in the data, of heavy
             flavor, Υ{hooked}, and Drell-Yan production in addition to
             muons mimicked by hadronic punchthrough. The number of
             unaccounted events corresponds to (12.8±3.2)% of the bb̄
             production. We find that (23±6)% of the unaccounted events
             contain additional muon candidates. For comparison, this
             fraction is (6.9±0.4)% for events due to bb̄ production.
             © 2011 The Author(s).},
   Doi = {10.1140/epjc/s10052-011-1720-4},
   Key = {fds309241}
}

@article{fds309260,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Aktas, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood- Spiers and SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amelung, C and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Arutinov, D and Asai, M and Asai, S and Silva, J and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astvatsatourov, A and Atoian, G and Auerbach, B},
   Title = {Studies of the performance of the ATLAS detector using
             cosmic-ray muons},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {3},
   Pages = {1-36},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1593-6},
   Abstract = {Muons from cosmic-ray interactions in the atmosphere provide
             a high-statistics source of particles that can be used to
             study the performance and calibration of the ATLAS detector.
             Cosmic-ray muons can penetrate to the cavern and deposit
             energy in all detector subsystems. Such events have played
             an important role in the commissioning of the detector since
             the start of the installation phase in 2005 and were
             particularly important for understanding the detector
             performance in the time prior to the arrival of the first
             LHC beams. Global cosmic-ray runs were undertaken in both
             2008 and 2009 and these data have been used through to the
             early phases of collision data-taking as a tool for
             calibration, alignment and detector monitoring. These large
             datasets have also been used for detector performance
             studies, including investigations that rely on the combined
             performance of different subsystems. This paper presents the
             results of performance studies related to combined tracking,
             lepton identification and the reconstruction of jets and
             missing transverse energy. Results are compared to
             expectations based on a cosmic-ray event generator and a
             full simulation of the detector response.},
   Doi = {10.1140/epjc/s10052-011-1593-6},
   Key = {fds309260}
}

@article{fds309265,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Charged-particle multiplicities in ppinteractions measured
             with the ATLAS detector at the LHC},
   Journal = {New Journal of Physics},
   Volume = {13},
   Number = {5},
   Pages = {053033-053033},
   Publisher = {IOP Publishing},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1367-2630/13/5/053033},
   Abstract = {Measurements are presented from proton-proton collisions at
             centre-of-mass energies of s = 0.9, 2.36 and 7 TeV recorded
             with the ATLAS detector at the LHC. Events were collected
             using a single-arm minimumbias trigger. The charged-particle
             multiplicity, its dependence on transverse momentum and
             pseudorapidity and the relationship between the mean
             transverse momentum and charged-particle multiplicity are
             measured. Measurements in different regions of phase space
             are shown, providing diffraction-reduced measurements as
             well as more inclusive ones. The observed distributions are
             corrected to well-defined phase-space regions, using
             model-independent corrections. The results are compared to
             each other and to various Monte Carlo (MC) models, including
             a new AMBT1 pythia6 tune. In all the kinematic regions
             considered, the particle multiplicities are higher than
             predicted by the MC models. The central charged-particle
             multiplicity per event and unit of pseudorapidity, for
             tracks with pT < 100 MeV, is measured to be 3.483±0.009
             (stat)±0.106 (syst) at s = 0.9 TeV and 5.630±0.003
             (stat)±0.169 (syst) at s = 7 TeV. © 2011 CERN for the
             benefit of the ATLAS Collaboration, published under licence
             by IOP Publishing Ltd for the Institute of Physics and
             Deutsche Physikalische Gesellschaft.},
   Doi = {10.1088/1367-2630/13/5/053033},
   Key = {fds309265}
}

@article{fds309276,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for neutral MSSM Higgs bosons decaying to
             τ+τ- pairs in proton-proton
             collisions at s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {3},
   Pages = {174-192},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.001},
   Abstract = {A search for neutral Higgs bosons decaying to pairs of τ
             leptons with the ATLAS detector at the LHC is presented. The
             analysis is based on proton-proton collisions at a
             center-of-mass energy of 7 TeV, recorded in 2010 and
             corresponding to an integrated luminosity of 36 pb-1. After
             signal selection, 276 events are observed in this data
             sample. The observed number of events is consistent with the
             total expected background of 269±36 events. Exclusion
             limits at the 95% confidence level are derived for the
             production cross section of a generic Higgs boson φ as a
             function of the Higgs boson mass and for A/H/h production in
             the Minimal Supersymmetric Standard Model (MSSM) as a
             function of the parameters mA and tanβ. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.10.001},
   Key = {fds309276}
}

@article{fds309278,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R},
   Title = {A search for new physics in dijet mass and angular
             distributions in ppcollisions at √s=7 TeV measured with
             the ATLAS detector},
   Journal = {New Journal of Physics},
   Volume = {13},
   Number = {5},
   Pages = {053044-053044},
   Publisher = {IOP Publishing},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1367-2630/13/5/053044},
   Abstract = {A search for new interactions and resonances produced in LHC
             proton-proton (pp) collisions at a centre-of-mass energy
             √s = 7 TeV was performed with the ATLAS detector. Using a
             dataset with an integrated luminosity of 36 pb -1, dijet
             mass and angular distributions were measured up to dijet
             masses of ∼3.5TeV and were found to be in good agreement
             with Standard Model predictions. This analysis sets limits
             at 95% CL on various models for new physics: an excited
             quark is excluded for mass between 0.60 and 2.64 TeV, an
             axigluon hypothesis is excluded for axigluon masses between
             0.60 and 2.10 TeV and quantum black holes are excluded in
             models with six extra space-time dimensions for quantum
             gravity scales between 0.75 and 3.67 TeV. Production cross
             section limits as a function of dijet mass are set using a
             simplified Gaussian signal model to facilitate comparisons
             with other hypotheses. Analysis of the dijet angular
             distribution using a novel technique simultaneously
             employing the dijet mass excludes quark contact interactions
             with a compositeness scale A below 9.5 TeV. © 2011 CERN for
             the benefit of the ATLAS Collaboration.},
   Doi = {10.1088/1367-2630/13/5/053044},
   Key = {fds309278}
}

@article{fds309279,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the differential cross-sections of inclusive,
             prompt and non-prompt J/Ψ production in proton-proton
             collisions at √s=7 TeV},
   Journal = {Nuclear Physics B},
   Volume = {850},
   Number = {3},
   Pages = {387-444},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2011.05.015},
   Abstract = {The inclusive J/Ψ production cross-section and fraction of
             J/Ψ mesons produced in B-hadron decays are measured in
             proton-proton collisions at √s=7 TeV with the ATLAS
             detector at the LHC, as a function of the transverse
             momentum and rapidity of the J/Ψ, using 2.3 pb-1 of
             integrated luminosity. The cross-section is measured from a
             minimum pT of 1 GeV to a maximum of 70 GeV and for
             rapidities within |y|<2.4 giving the widest reach of any
             measurement of J/Ψ production to date. The differential
             production cross-sections of prompt and non-prompt J/Ψ are
             separately determined and are compared to Colour Singlet
             NNLO*, Colour Evaporation Model, and FONLL predictions. ©
             2011 CERN.},
   Doi = {10.1016/j.nuclphysb.2011.05.015},
   Key = {fds309279}
}

@article{fds309280,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S},
   Title = {Measurement of the Υ(1S) production cross-section in pp
             collisions at s=7 TeV in ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {1-2},
   Pages = {9-27},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.09.092},
   Abstract = {A measurement of the cross-section for Υ(1S)→μ+μ-
             production in proton-proton collisions at centre of mass
             energy of 7 TeV is presented. The cross-section is measured
             as a function of the Υ(1S) transverse momentum in two bins
             of rapidity, |yΥ(1S)|<1.2 and 1.2<|yΥ(1S)|<2.4. The
             measurement requires that both muons have transverse
             momentum pTμ>4 GeV and pseudorapidity |ημ|<2.5 in order
             to reduce theoretical uncertainties on the acceptance, which
             depend on the poorly known polarisation. The results are
             based on an integrated luminosity of 1.13 pb-1, collected
             with the ATLAS detector at the Large Hadron Collider. The
             cross-section measurement is compared to theoretical
             predictions: it agrees to within a factor of two with a
             prediction based on the NRQCD model including colour-singlet
             and colour-octet matrix elements as implemented in Pythia
             while it disagrees by up to a factor of ten with the
             next-to-leading order prediction based on the colour-singlet
             model. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.09.092},
   Key = {fds309280}
}

@article{fds309281,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S},
   Title = {Search for heavy long-lived charged particles with the ATLAS
             detector in pp collisions at √s=7 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {703},
   Number = {4},
   Pages = {428-446},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.08.042},
   Abstract = {A search for long-lived charged particles reaching the muon
             spectrometer is performed using a data sample of 37 pb-1
             from pp collisions at √s=7 TeV collected by the ATLAS
             detector at the LHC in 2010. No excess is observed above the
             estimated background. Stable τ̃ sleptons are excluded at
             95% CL up to a mass of 136 GeV, in GMSB models with N5=3,
             mmessenger=250 TeV, sign(μ)=1 and tanβ=5. Electroweak
             production of sleptons is excluded up to a mass of 110 GeV.
             Gluino R-hadrons in a generic interaction model are excluded
             up to masses of 530 GeV to 544 GeV depending on the fraction
             of R-hadrons produced as g̃-balls. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.08.042},
   Key = {fds309281}
}

@article{fds309284,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Search for supersymmetry in pp collisions at √s=7 TeV in
             final states with missing transverse momentum and
             b-jets},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {701},
   Number = {4},
   Pages = {398-416},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.06.015},
   Abstract = {Results are presented of a search for supersymmetric
             particles in events with large missing transverse momentum
             and at least one heavy flavour jet candidate in √s=7 TeV
             proton-proton collisions. In a data sample corresponding to
             an integrated luminosity of 35 pb-1 recorded by the ATLAS
             experiment at the Large Hadron Collider, no significant
             excess is observed with respect to the prediction for
             Standard Model processes. For R-parity conserving models in
             which sbottoms (stops) are the only squarks to appear in the
             gluino decay cascade, gluino masses below 590 GeV (520 GeV)
             are excluded at the 95% C.L. The results are also
             interpreted in an MSUGRA/CMSSM supersymmetry breaking
             scenario with tanβ=40 and in an SO(10) model framework. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.06.015},
   Key = {fds309284}
}

@article{fds309286,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S and Åsman, B},
   Title = {Search for squarks and gluinos using final states with jets
             and missing transverse momentum with the ATLAS detector in
             √s=7 TeV proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {701},
   Number = {2},
   Pages = {186-203},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.05.061},
   Abstract = {A search for squarks and gluinos in final states containing
             jets, missing transverse momentum and no electrons or muons
             is presented. The data were recorded by the ATLAS experiment
             in √s=7 TeV proton-proton collisions at the Large Hadron
             Collider. No excess above the Standard Model background
             expectation was observed in 35 pb-1 of analysed data. Gluino
             masses below 500 GeV are excluded at the 95% confidence
             level in simplified models containing only squarks of the
             first two generations, a gluino octet and a massless
             neutralino. The exclusion increases to 870 GeV for equal
             mass squarks and gluinos. In MSUGRA/CMSSM models with
             tanβ=3, A0=0 and μ>0, squarks and gluinos of equal mass
             are excluded below 775 GeV. These are the most stringent
             limits to date. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.05.061},
   Key = {fds309286}
}

@article{fds309299,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for {Randall-Sundrum} gravitons in the diphoton
             channel at {CDF}},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {1},
   Pages = {011102},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.011102},
   Abstract = {We report on a search for new particles in the diphoton
             channel using a data sample of pp̄ collisions at
             √s=1.96TeV collected by the CDF II detector at the
             Fermilab Tevatron, with an integrated luminosity of
             5.4fb⊃-1. The diphoton invariant mass spectrum of the data
             agrees well with the standard model expectation. We set
             upper limits on the production cross section times branching
             ratio for the Randall-Sundrum graviton, as a function of
             diphoton mass. We subsequently derive lower limits on the
             graviton mass of 459GeV/c2 and 963GeV/c2, at the 95%
             confidence level, for coupling parameters (k/M̄Pl) of 0.01
             and 0.1, respectively. © 2011 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.83.011102},
   Key = {fds309299}
}

@article{fds309311,
   Author = {Abat, E and Abdallah, JM and Addy, TN and Adragna, P and Aharrouche, M and Ahmad, A and Akesson, TPA and Aleksa, M and Alexa, C and Anderson, K and Andreazza, A and Anghinolfi, F and Antonaki, A and Arabidze, G and Arik,
             E and Atkinson, T and Baines, J and Baker, OK and Banfi, D and Baron, S and Barr, AJ and Beccherle, R and Beck, HP and Belhorma, B and Bell, PJ and Benchekroun, D and Benjamin, DP and Benslama, K and Bergeaas
             Kuutmann, E and Bernabeu, J and Bertelsen, H and Binet, S and Biscarat,
             C and Boldea, V and Bondarenko, VG and Boonekamp, M and Bosman, M and Bourdarios, C and Broklova, Z and Burckhart Chromek and D and Bychkov,
             V and Callahan, J and Calvet, D and Canneri, M and Capéans Garrido and M and Caprini, M and Cardiel Sas and L and Carli, T and Carminati, L and Carvalho, J and Cascella, M and Castillo, MV and Catinaccio, A and Cauz,
             D and Cavalli, D and Cavalli Sforza and M and Cavasinni, V and Cetin, SA and Chen, H and Cherkaoui, R and Chevalier, L and Chevallier, F and Chouridou, S and Ciobotaru, M and Citterio, M and Clark, A and Cleland,
             B and Cobal, M and Cogneras, E and Conde Muino and P and Consonni, M and Constantinescu, S and Cornelissen, T and Correard, S and Corso Radu,
             A and Costa, G and Costa, MJ and Costanzo, D and Cuneo, S and Cwetanski, P and Da Silva and D and Dam, M and Dameri, M and Danielsson, HO and Dannheim, D and Darbo, G and Davidek, T and De, K and Defay, PO and Dekhissi, B and Del
             Peso, J and Del Prete and T and Delmastro, M and Derue, F and Di Ciaccio,
             L and Di Girolamo and B and Dita, S and Dittus, F and Djama, F and Djobava,
             T},
   Title = {A layer correlation technique for pion energy calibration at
             the 2004 ATLAS Combined Beam Test},
   Journal = {Journal of Instrumentation},
   Volume = {6},
   Number = {6},
   Pages = {P06001-P06001},
   Publisher = {IOP Publishing},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/6/06/P06001},
   Abstract = {A new method for calibrating the hadron response of a
             segmented calorimeter is developed and successfully applied
             to beam test data. It is based on a principal component
             analysis of energy deposits in the calorimeter layers,
             exploiting longitudinal shower development information to
             improve the measured energy resolution. Corrections for
             invisible hadronic energy and energy lost in dead material
             in front of and between the calorimeters of the ATLAS
             experiment were calculated with simulated Geant4 Monte Carlo
             events and used to reconstruct the energy of pions impinging
             on the calorimeters during the 2004 Barrel Combined Beam
             Test at the CERN H8 area. For pion beams with energies
             between 20GeV and 180GeV, the particle energy is
             reconstructed within 3% and the energy resolution is
             improved by between 11% and 25% compared to the resolution
             at the electromagnetic scale. © 2011 CERN for the benefit
             of the ATLAS collaboration, published under license by IOP
             Publishing Ltd and SISSA.},
   Doi = {10.1088/1748-0221/6/06/P06001},
   Key = {fds309311}
}

@article{fds309312,
   Author = {Abat, E and Abdallah, M and Addy, N and Adragna, P and Aharrouche, M and Ahmad, A and Akesson, A and Aleksa, M and Alexa, C and Anderson, K and Andreazza, A and Anghinolfi, F and Antonaki, A and Arabidze, G and Arik,
             E and Atkinson, T and Baines, J and Baker, K and Banfi, D and Baron, S and Barr, J and Beccherle, R and Beck, P and Belhorma, B and Bell, J and Benchekroun, D and Benjamin, P and Benslama, K and Bergeaas Kuutmann,
             E and Bernabeu, J and Bertelsen, H and Binet, S and Biscarat, C and Boldea,
             V and Bondarenko, G and Boonekamp, M and Bosman, M and Bourdarios, C and Broklova, Z and Burckhart Chromek and D and Bychkov, V and Callahan, J and Calvet, D and Canneri, M and Capens Garrido and M and Caprini, M and Cardiel Sas and L and Carli, T and Carminati, L and Carvalho, J and Cascella, M and Castillo, MV and Catinaccio, A and Cauz, D and Cavalli,
             D and Cavalli Sforza and M and Cavasinni, V and Cetin, SA and Chen, H and Cherkaoui, R and Chevalier, L and Chevallier, F and Chouridou, S and Ciobotaru, M and Citterio, M and Clark, A and Cleland, B and Cobal, M and Cogneras, E and Conde Muino and P and Consonni, M and Constantinescu, S and Cornelissen, T and Correard, S and Corso Radu and A and Costa, G and Costa,
             MJ and Costanzo, D and Cuneo, S and Cwetanski, P and Da Silva and D and Dam,
             M and Dameri, M and Danielsson, HO and Dannheim, D and Darbo, G and Davidek, T and De, K and Defay, PO and Dekhissi, B and Del Peso and J and Del
             Prete, T and Delmastro, M and Derue, F and Di Ciaccio and L and Di
             Girolamo, B and Dita, S and Dittus, F and Djama, F and Djobava,
             T},
   Title = {Photon reconstruction in the ATLAS inner detector and liquid
             argon barrel calorimeter at the 2004 combined test
             beam},
   Journal = {Journal of Instrumentation},
   Volume = {6},
   Number = {4},
   Pages = {P04001-P04001},
   Publisher = {IOP Publishing},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/6/04/P04001},
   Abstract = {The reconstruction of photons in the ATLAS detector is
             studied with data taken during the 2004 Combined Test Beam,
             where a full slice of the ATLAS detector was exposed to
             beams of particles of known energy at the CERN SPS. The
             results presented show significant differences in the
             longitudinal development of the electromagnetic shower
             between converted and unconverted photons as well as in the
             total measured energy. The potential to use the
             reconstructed converted photons as a means to precisely map
             the material of the tracker in front of the electromagnetic
             calorimeter is also considered. All results obtained are
             compared with a detailed Monte-Carlo simulation of the
             test-beam setup which is based on the same simulation and
             reconstruction tools as those used for the ATLAS detector
             itself. © 2011 CERN for the benefit of the ATLAS
             collaboration, published under license by IOP Publishing Ltd
             and SISSA.},
   Doi = {10.1088/1748-0221/6/04/P04001},
   Key = {fds309312}
}

@article{fds309313,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams,
             DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna,
             P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M and Anduaga,
             XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R},
   Title = {Limits on the production of the standard model Higgs boson
             in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {9},
   Pages = {1-30},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1728-9},
   Abstract = {A search for the Standard Model Higgs boson at the Large
             Hadron Collider (LHC) running at a centre-of-mass energy of
             7 TeV is reported, based on a total integrated luminosity of
             up to 40 pb-1 collected by the ATLAS detector in 2010.
             Several Higgs boson decay channels: H→γγ,
             H→ZZ(*)→ℓℓℓℓ, H→ZZ→ℓℓνν,
             H→ZZ→ℓℓqq, H→WW(*)→ℓνℓν and
             H→WW→ℓνqq (ℓ is e, μ) are combined in a mass range
             from 110 GeV to 600 GeV. The highest sensitivity is achieved
             in the mass range between 160 GeV and 170 GeV, where the
             expected 95% CL exclusion sensitivity is at Higgs boson
             production cross sections 2. 3 times the Standard Model
             prediction. Upper limits on the cross section for its
             production are determined. Models with a fourth generation
             of heavy leptons and quarks with Standard Model-like
             couplings to the Higgs boson are also investigated and are
             excluded at 95% CL for a Higgs boson mass in the range from
             140 GeV to 185 GeV. © 2011 CERN for the benefit of the
             ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-011-1728-9},
   Key = {fds309313}
}

@article{fds321637,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of dijet production with a veto on additional
             central jet activity in pp collisions at √s = 7TeV using
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {9},
   Pages = {1-36},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2011)053},
   Abstract = {A measurement of jet activity in the rapidity interval
             bounded by a dijet system is presented. Events are vetoed if
             a jet with transverse momentum greater than 20GeV is found
             between the two boundary jets. The fraction of dijet events
             that survive the jet veto is presented for boundary jets
             that are separated by up to six units of rapidity and with
             mean transverse momentum 50 < pT < 500GeV. The mean
             multiplicity of jets above the veto scale in the rapidity
             interval bounded by the dijet system is also presented as an
             alternative method for quantifying perturbative QCD
             emission. The data are compared to a next-to-leading order
             plus parton shower prediction from the powheg-box, an
             all-order resummation using the hej calculation and the
             pythia, herwig++ and alpgen event generators. The
             measurement was performed using pp collisions at √s = 7TeV
             using data recorded by the ATLAS detector in
             2010.},
   Doi = {10.1007/JHEP09(2011)053},
   Key = {fds321637}
}

@article{fds325781,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of multi-jet cross sections in proton–proton
             collisions at a 7 TeV center-of-mass energy},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {11},
   Pages = {1-27},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1763-6},
   Abstract = {Inclusive multi-jet production is studied in proton–proton
             collisions at a center-of-mass energy of 7 TeV, using the
             ATLAS detector. The data sample corresponds to an integrated
             luminosity of 2.4 pb-1. Results on multi-jet cross sections
             are presented and compared to both leading-order plus
             parton-shower Monte Carlo predictions and to
             next-to-leading-order QCD calculations.},
   Doi = {10.1140/epjc/s10052-011-1763-6},
   Key = {fds325781}
}

@article{fds325782,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai,
             S},
   Title = {Measurement of Wγ and Zγ production in proton-proton
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2011)072},
   Abstract = {We present studies of W and Z bosons with associated high
             energy photons produced in pp collisions at √s = 7TeV. The
             analysis uses 35 pb γ + X) event candidates are selected.
             The kinematic distributions of the leptons and photons and
             the production cross sections are measured. The data are
             found to agree with Standard Model predictions that include
             next-to-leading-order O(ααs) contributions. © SISSA
             2011.},
   Doi = {10.1007/JHEP09(2011)072},
   Key = {fds325782}
}

@article{fds309261,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adorisio, C and Adragna,
             P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli,
             G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Aktas,
             A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Ambrosio, G and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR},
   Title = {Search for quark contact interactions in dijet angular
             distributions in pp collisions at s=7 TeV measured with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {694},
   Number = {4-5},
   Pages = {327-345},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2010.10.021},
   Abstract = {Dijet angular distributions from the first LHC pp collisions
             at center-of-mass energy s=7 TeV have been measured with the
             ATLAS detector. The dataset used for this analysis
             represents an integrated luminosity of 3.1 pb-1. Dijet Χ
             distributions and centrality ratios have been measured up to
             dijet masses of 2.8 TeV, and found to be in good agreement
             with Standard Model predictions. Analysis of the λ
             distributions excludes quark contact interactions with a
             compositeness scale Χ below 3.4 TeV, at 95% confidence
             level, significantly exceeding previous limits. © 2010
             CERN.},
   Doi = {10.1016/j.physletb.2010.10.021},
   Key = {fds309261}
}

@article{fds309287,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the ${B}^{-}$ lifetime using a simulation
             free approach for trigger bias correction},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {3},
   Pages = {032008},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.032008},
   Abstract = {The collection of a large number of B-hadron decays to
             hadronic final states at the CDF II Detector is possible due
             to the presence of a trigger that selects events based on
             track impact parameters. However, the nature of the
             selection requirements of the trigger introduces a large
             bias in the observed proper-decay-time distribution. A
             lifetime measurement must correct for this bias, and the
             conventional approach has been to use a Monte Carlo
             simulation. The leading sources of systematic uncertainty in
             the conventional approach are due to differences between the
             data and the Monte Carlo simulation. In this paper, we
             present an analytic method for bias correction without using
             simulation, thereby removing any uncertainty due to the
             differences between data and simulation. This method is
             presented in the form of a measurement of the lifetime of
             the B- using the mode B-→D0π -. The B- lifetime is
             measured as τB -=1.663±0.023±0.015ps, where the first
             uncertainty is statistical and the second systematic. This
             new method results in a smaller systematic uncertainty in
             comparison to methods that use simulation to correct for the
             trigger bias. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.83.032008},
   Key = {fds309287}
}

@article{fds309296,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of $t\overline{t}$ spin correlation in
             $p\overline{p}$ collisions using the CDF II detector at the
             Tevatron},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {3},
   Pages = {031104},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.031104},
   Abstract = {The tt̄ spin correlation at production is a fundamental
             prediction of QCD and a potentially incisive test of new
             physics coupled to top quarks. We measure the tt̄ spin
             state in pp̄ collisions at √s=1.96TeV using 1001
             candidate events in the lepton plus jets decay channel
             reconstructed in the CDF II detector. In the helicity basis,
             for a top-quark mass of 172.5GeV/c2, we find a spin
             correlation coefficient κ=0.60±0.50(stat)±0. 16(syst),
             consistent with the QCD prediction, κ 0.40. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.031104},
   Key = {fds309296}
}

@article{fds309301,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for a new heavy gauge boson ${W}^{$'${}}$ with event
             signature $\mathrm{\text{electron}}+\mathrm{\text{missing}}$
             transverse energy in $p\overline{p}$ collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {3},
   Pages = {031102},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.031102},
   Abstract = {We present a search for a new heavy charged vector boson
             W′ decaying to an electron-neutrino pair in pp̄
             collisions at a center-of-mass energy of 1.96 TeV. The data
             were collected with the CDF II detector and correspond to an
             integrated luminosity of 5.3fb-1. No significant excess
             above the standard model expectation is observed and we set
             upper limits on σ•B(W′→eν). Assuming standard model
             couplings to fermions and the neutrino from the W′ boson
             decay to be light, we exclude a W′ boson with mass less
             than 1.12TeV/c2 at the 95% confidence level. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.031102},
   Key = {fds309301}
}

@article{fds309257,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Baltasar Dos
             Santos Pedrosa and F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa,
             HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, C and Begel, M and Behar Harpaz,
             S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             G and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Ben
             Ami, S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci,
             F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black,
             KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocci, A and Bock, R and Boddy, CR and Boehler,
             M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bona, M and Boonekamp, M and Boorman, G and Booth, CN and Booth, P and Booth, JRA and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Brambilla, E and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton,
             D and Brett, ND and Bright-Thomas, PG and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brubaker,
             E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci,
             F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Buis, EJ and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera Urbán and S and Caccia, M and Caforio, D and Cakir,
             O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camard, A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carpentieri, C and Carrillo Montoya and GD and Carron Montero and S and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cavallari, A and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Cazzato, A and Ceradini, F and Cerna, C and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty,
             D and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre,
             E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, H and Chen, L and Chen, S and Chen,
             T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui
             El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chevallier, F and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {Search for diphoton events with large missing transverse
             energy in 7 TeV proton-proton collisions with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {106},
   Number = {12},
   Pages = {121803},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.106.121803},
   Abstract = {A search for diphoton events with large missing transverse
             energy is presented. The data were collected with the ATLAS
             detector in proton-proton collisions at √s=7 TeV at the
             CERN Large Hadron Collider and correspond to an integrated
             luminosity of 3.1 pb⁻¹. No excess of such events is
             observed above the standard model background prediction. In
             the context of a specific model with one universal extra
             dimension with compactification radius R and gravity-induced
             decays, values of 1/R<729 GeV are excluded at 95% C. L.,
             providing the most sensitive limit on this model to
             date.},
   Doi = {10.1103/physrevlett.106.121803},
   Key = {fds309257}
}

@article{fds309258,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for High Mass Resonances Decaying to Muon Pairs in
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
             $p\overline{p}$ Collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {12},
   Pages = {121801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.121801},
   Abstract = {We present a search for a new narrow, spin-1, high mass
             resonance decaying to μ(+)μ⁻+X, using a
             matrix-element-based likelihood and a simultaneous
             measurement of the resonance mass and production rate. In
             data with 4.6 fb⁻¹ of integrated luminosity collected by
             the CDF detector in pp collisions at √s=1960 GeV, the most
             likely signal cross section is consistent with zero at 16%
             confidence level. We therefore do not observe evidence for a
             high mass resonance and place limits on models predicting
             spin-1 resonances, including M>1071 GeV/c² at 95%
             confidence level for a Z' boson with the same couplings to
             fermions as the Z boson.},
   Doi = {10.1103/PhysRevLett.106.121801},
   Key = {fds309258}
}

@article{fds309259,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of ${b}$ Hadron Lifetimes in Exclusive Decays
             Containing a ${J}/\psi$ in $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {12},
   Pages = {121804},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.121804},
   Abstract = {We report on a measurement of b-hadron lifetimes in the
             fully reconstructed decay modes B(+)→J/ψK(+),
             B⁰→J/ψK*(892)⁰, B⁰→J/ψK(s)⁰, and
             Λ(b)⁰→J/ψΛ⁰ using data corresponding to an
             integrated luminosity of 4.3 fb⁻¹, collected by the CDF
             II detector at the Fermilab Tevatron. The measured lifetimes
             are τ(B(+))=[1.639±0.009(stat)±0.009(syst)] ps,
             τ(B⁰)=[1.507±0.010(stat)±0.008(syst)] ps, and
             τ(Λ(b)⁰)=[1.537±0.045(stat)±0.014(syst)] ps. The
             lifetime ratios are τ(B(+))/τ(B⁰)=[1.088±0.009(stat)±0.004(syst)]
             and τ(Λ(b)⁰)/τ(B⁰)=[1.020±0.030(stat)±0.008(syst)].
             These are the most precise determinations of these
             quantities from a single experiment.},
   Doi = {10.1103/PhysRevLett.106.121804},
   Key = {fds309259}
}

@article{fds309295,
   Author = {Aaltonen, and T, and al, E},
   Title = {Observation of ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}^{*}(892{)}^{0}$
             and ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}_{S}^{0}$
             decays},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {5},
   Pages = {052012},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.052012},
   Abstract = {We report the first observation of two Cabibbo-suppressed
             decay modes of the Bs0 meson. Using a sample of pp̄
             collisions at √s=1.96TeV corresponding to 5.9fb-1 of
             integrated luminosity collected with the CDF II, the
             collider detector at the Fermilab Tevatron, we search for
             new Bs0 decay modes in a sample of events containing
             J/ψ→μ+μ - decays. We reconstruct a Bs0→J/ψK*(892)0
             signal with K*(892)0→K+π-, observing a yield of 151±25
             events with a statistical significance of 8.0σ. We also
             reconstruct a Bs0→J/ψKS0 signal with KS0→π+π-,
             observing a yield of 64±14 events with a statistical
             significance of 7.2σ. From these yields, we extract the
             branching ratios B(Bs0→J/ψK*(892)0)=(8. 3±3.8)×10-5 and
             B(Bs0→J/ψK0)=(3.5±0.8) ×10-5, where statistical,
             systematic, and fragmentation- fraction uncertainties are
             included in the combined uncertainty. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.83.052012},
   Key = {fds309295}
}

@article{fds309267,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Study of jet shapes in inclusive jet production in pp
             collisions at √s=7TeV using the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {83},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.052003},
   Abstract = {Jet shapes have been measured in inclusive jet production in
             proton-proton collisions at √s=7TeV using 3pb-1 of data
             recorded by the ATLAS experiment at the LHC. Jets are
             reconstructed using the anti-kt algorithm with transverse
             momentum 30GeV<pT<600GeV and rapidity in the region |y|<2.8.
             The data are corrected for detector effects and compared to
             several leading-order QCD matrix elements plus parton shower
             Monte Carlo predictions, including different sets of
             parameters tuned to model fragmentation processes and
             underlying event contributions in the final state. The
             measured jets become narrower with increasing jet transverse
             momentum and the jet shapes present a moderate jet rapidity
             dependence. Within QCD, the data test a variety of
             perturbative and nonperturbative effects. In particular, the
             data show sensitivity to the details of the parton shower,
             fragmentation, and underlying event models in the Monte
             Carlo generators. For an appropriate choice of the
             parameters used in these models, the data are well
             described. © 2011 CERN, for the ATLAS Collaboration.},
   Doi = {10.1103/PhysRevD.83.052003},
   Key = {fds309267}
}

@article{fds309272,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoroś, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for a heavy gauge boson decaying to a charged lepton
             and a neutrino in 1 fb-1 of pp collisions at √s
             = 7 TeV using the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {1-2},
   Pages = {28-46},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.09.093},
   Abstract = {The ATLAS detector at the LHC is used to search for
             high-mass states, such as heavy charged gauge bosons (W'),
             decaying to a charged lepton (electron or muon) and a
             neutrino. Results are presented based on the analysis of pp
             collisions at a center-of-mass energy of 7 TeV corresponding
             to an integrated luminosity of 1.04 fb-1. No excess above
             Standard Model expectations is observed. A W' with
             Sequential Standard Model couplings is excluded at the 95%
             confidence level for masses up to 2.15 TeV.},
   Doi = {10.1016/j.physletb.2011.09.093},
   Key = {fds309272}
}

@article{fds309264,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Measurement of the centrality dependence of J/Ψ yields and
             observation of Z production in lead-lead collisions with the
             ATLAS detector at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {697},
   Number = {4},
   Pages = {294-312},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.02.006},
   Abstract = {Using the ATLAS detector, a centrality-dependent suppression
             has been observed in the yield of J/Ψ mesons produced in
             the collisions of lead ions at the Large Hadron Collider. In
             a sample of minimum-bias lead-lead collisions at a
             nucleon-nucleon centre of mass energy sNN=2.76 TeV,
             corresponding to an integrated luminosity of about 6.7
             μb-1, J/Ψ mesons are reconstructed via their decays to
             μ+μ- pairs. The measured J/Ψ yield, normalized to the
             number of binary nucleon-nucleon collisions, is found to
             significantly decrease from peripheral to central
             collisions. The centrality dependence is found to be
             qualitatively similar to the trends observed at previous,
             lower energy experiments. The same sample is used to
             reconstruct Z bosons in the μ+μ- final state, and a total
             of 38 candidates are selected in the mass window of 66 to
             116 GeV. The relative Z yields as a function of centrality
             are also presented, although no conclusion can be inferred
             about their scaling with the number of binary collisions,
             because of limited statistics. This analysis provides the
             first results on J/Ψ and Z production in lead-lead
             collisions at the LHC. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.02.006},
   Key = {fds309264}
}

@article{fds309263,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonelli, S and Antos,
             J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui,
             S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Measurement of the inclusive isolated prompt photon cross
             section in pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {83},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.052005},
   Abstract = {A measurement of the cross section for the inclusive
             production of isolated prompt photons in pp collisions at a
             center-of-mass energy √s=7TeV is presented. The
             measurement covers the pseudorapidity ranges |ηγ|<1. 37
             and 1.52≤|ηγ|<1.81 in the transverse energy range
             15≤ETγ<100GeV. The results are based on an integrated
             luminosity of 880nb-1, collected with the ATLAS detector at
             the Large Hadron Collider. Photon candidates are identified
             by combining information from the calorimeters and from the
             inner tracker. Residual background in the selected sample is
             estimated from data based on the observed distribution of
             the transverse isolation energy in a narrow cone around the
             photon candidate. The results are compared to predictions
             from next-to-leading-order perturbative QCD calculations. ©
             2011 CERN, for the ATLAS Collaboration.},
   Doi = {10.1103/PhysRevD.83.052005},
   Key = {fds309263}
}

@article{fds309251,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos Santos Pedrosa,
             F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, G and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci,
             F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Biesiada, J and Biglietti,
             M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blocker, C and Blocki, J and Blondel, A and Blum,
             W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bona, M and Bondarenko, VG and Boonekamp, M and Boorman, G and Booth, CN and Booth, P and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni,
             S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik,
             J and Braem, A and Brambilla, E and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Brett, ND and Bright-Thomas, PG and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brubaker, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Buira-Clark, D and Buis, EJ and Bulekov,
             O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera Urbán and S and Caccia, M and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camard, A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carpentieri,
             C and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho,
             J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavallari,
             A and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Cazzato, A and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, H and Chen, L and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chevallier, F and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou,
             Y},
   Title = {Measurement of dijet azimuthal decorrelations in pp
             collisions at sqrt(s)=7  TeV.},
   Journal = {Physical review letters},
   Volume = {106},
   Number = {17},
   Pages = {172002},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.106.172002},
   Abstract = {Azimuthal decorrelations between the two central jets with
             the largest transverse momenta are sensitive to the dynamics
             of events with multiple jets. We present a measurement of
             the normalized differential cross section based on the full
             data set (∫Ldt=36  pb(-1)) acquired by the ATLAS
             detector during the 2010 sqrt(s)=7  TeV proton-proton
             run of the LHC. The measured distributions include jets with
             transverse momenta up to 1.3 TeV, probing perturbative QCD
             in a high-energy regime.},
   Doi = {10.1103/physrevlett.106.172002},
   Key = {fds309251}
}

@article{fds309252,
   Author = {Aaltonen, and T, and al, E},
   Title = {Invariant Mass Distribution of Jet Pairs Produced in
             Association with a ${W}$ Boson in $p\overline{p}$ Collisions
             at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {17},
   Pages = {171801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.171801},
   Abstract = {We report a study of the invariant mass distribution of jet
             pairs produced in association with a W boson using data
             collected with the CDF detector which correspond to an
             integrated luminosity of 4.3  fb(-1). The observed
             distribution has an excess in the 120-160  GeV/c(2) mass
             range which is not described by current theoretical
             predictions within the statistical and systematic
             uncertainties. In this Letter, we report studies of the
             properties of this excess.},
   Doi = {10.1103/PhysRevLett.106.171801},
   Key = {fds309252}
}

@article{fds309253,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the Mass Difference between $t$ and
             $\overline{t}$ Quarks},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {15},
   Pages = {152001},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.152001},
   Abstract = {We present a direct measurement of the mass difference
             between t and t quarks using tt candidate events in the
             lepton+jets channel, collected with the CDF II detector at
             Fermilab's 1.96 TeV Tevatron pp Collider. We make an event
             by event estimate of the mass difference to construct
             templates for top quark pair signal events and background
             events. The resulting mass difference distribution of data
             is compared to templates of signals and background using a
             maximum likelihood fit. From a sample corresponding to an
             integrated luminosity of 5.6  fb(-1), we measure a mass
             difference, ΔM(top) = M(t) - M(t) = -3.3 ± 1.4(stat) ±
             1.0(syst)  GeV/c2, approximately 2 standard deviations
             away from the CPT hypothesis of zero mass
             difference.},
   Doi = {10.1103/PhysRevLett.106.152001},
   Key = {fds309253}
}

@article{fds309254,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for Heavy Bottomlike Quarks Decaying to an Electron
             or Muon and Jets in $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {14},
   Pages = {141803},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.141803},
   Abstract = {We report the most sensitive direct search for pair
             production of fourth-generation bottomlike chiral quarks
             (b') each decaying promptly to tW. We search for an excess
             of events with an electron or muon, at least five jets (one
             identified as due to a b or c quark), and an imbalance of
             transverse momentum by using data from pp collisions
             collected by the CDF II detector at Fermilab with an
             integrated luminosity of 4.8  fb(-1). We observe events
             consistent with background expectation, calculate upper
             limits on the b' pair-production cross section (σ(bb'))
             ≲30  fb for m(b') > 375  GeV/c2), and exclude
             m(b') < 372  GeV/c2 at 95% confidence level assuming a
             100% branching ratio of b' to tW.},
   Doi = {10.1103/PhysRevLett.106.141803},
   Key = {fds309254}
}

@article{fds309255,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos Santos Pedrosa,
             F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, G and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci,
             F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Biesiada, J and Biglietti,
             M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blocker, C and Blocki, J and Blondel, A and Blum,
             W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bona, M and Bondarenko, VG and Boonekamp, M and Boorman, G and Booth, CN and Booth, P and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni,
             S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik,
             J and Braem, A and Brambilla, E and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Brett, ND and Bright-Thomas, PG and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brubaker, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Buira-Clark, D and Buis, EJ and Bulekov,
             O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera Urbán and S and Caccia, M and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camard, A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carpentieri,
             C and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho,
             J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavallari,
             A and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Cazzato, A and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, H and Chen, L and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chevallier, F and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou,
             Y},
   Title = {Search for supersymmetry using final states with one lepton,
             jets, and missing transverse momentum with the ATLAS
             detector in √s=7 TeV pp collisions.},
   Journal = {Physical review letters},
   Volume = {106},
   Number = {13},
   Pages = {131802},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.106.131802},
   Abstract = {This Letter presents the first search for supersymmetry in
             final states containing one isolated electron or muon, jets,
             and missing transverse momentum from √s=7  TeV
             proton-proton collisions at the LHC. The data were recorded
             by the ATLAS experiment during 2010 and correspond to a
             total integrated luminosity of 35  pb(-1). No excess
             above the standard model background expectation is observed.
             Limits are set on the parameters of the minimal supergravity
             framework, extending previous limits. Within this framework,
             for A(0)=0 GeV, tanβ=3, and μ>0 and for equal squark and
             gluino masses, gluino masses below 700 GeV are excluded at
             95% confidence level.},
   Doi = {10.1103/physrevlett.106.131802},
   Key = {fds309255}
}

@article{fds309256,
   Author = {Aad, D and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, N and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoros, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Luminosity determination in pp collisions at √s = 7 TeV
             using the ATLAS detector at the LHC},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {4},
   Pages = {1-37},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1630-5},
   Abstract = {Measurements of luminosity obtained using the ATLAS detector
             during early running of the Large Hadron Collider (LHC) at
             √s = 7 TeV are presented. The luminosity is independently
             determined using several detectors and multiple algorithms,
             each having different acceptances, systematic uncertainties
             and sensitivity to background. The ratios of the
             luminosities obtained from these methods are monitored as a
             function of time and of μ, the average number of inelastic
             interactions per bunch crossing. Residual time- and
             μ-dependence between the methods is less than 2% for 0 < μ
             < 2.5. Absolute luminosity calibrations, performed using
             beam separation scans, have a common systematic uncertainty
             of ±11%, dominated by the measurement of the LHC beam
             currents. After calibration, the luminosities obtained from
             the different methods differ by at most ±2%. The visible
             cross sections measured using the beam scans are compared to
             predictions obtained with the PYTHIA and PHOJET event
             generators and the ATLAS detector simulation. © CERN for
             the benefit of the ATLAS collaboration 2011.},
   Doi = {10.1140/epjc/s10052-011-1630-5},
   Key = {fds309256}
}

@article{fds309292,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the Forward-Backward Asymmetry in the
             ${B}\rightarrow{K}^{(*)}\mu^{+}\mu^{-}$ Decay and First
             Observation of the ${B}_{s}^{0}$\rightarrow${}$\phi${}{$\mu${}}^{+}{$\mu${}}^{-}$
             Decay},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {16},
   Pages = {161801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.161801},
   Abstract = {We reconstruct the rare decays B(+)→K(+)μ(+0μ(-0,
             B90)→K*(892)(0)μ(+)μ(-), and B(s)(0)→ϕ(1020)μ(+)μ(-)
             in a data sample corresponding to 4.4  fb(-1) collected
             in pp collisions at √[s]=1.96  TeV by the CDF II
             detector at the Tevatron Collider. Using 121±16
             B(+)→K(+)μ(+)μ(-) and 101±12 B(0)→K(*0)μ(+)μ(-)
             decays we report the branching ratios. In addition, we
             report the differential branching ratio and the muon
             forward-backward asymmetry in the B(+) and B(0) decay modes,
             and the K(*0) longitudinal polarization fraction in the B(0)
             decay mode with respect to the squared dimuon mass. These
             are consistent with the predictions, and most recent
             determinations from other experiments and of comparable
             accuracy. We also report the first observation of the
             B(s)(0)→ϕμ(+)μ(-) decay and measure its branching ratio
             BR(B(s)(0)→ϕμ(+)μ(-))=[1.44±0.33±0.46]×10(-6) using
             27±6 signal events. This is currently the most rare B(s)(0)
             decay observed.},
   Doi = {10.1103/PhysRevLett.106.161801},
   Key = {fds309292}
}

@article{fds309293,
   Author = {Aaltonen, and and, T and al, E},
   Title = {Measurement of the $t\overline{t}$ production cross section
             with an \textit{in~situ} calibration of $b$-jet
             identification efficiency},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {7},
   Pages = {071102},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.071102},
   Abstract = {A measurement of the top-quark pair-production cross section
             in pp̄ collisions at √s=1.96TeV using data corresponding
             to an integrated luminosity of 1.12fb-1 collected with the
             Collider Detector at Fermilab is presented. Decays of
             top-quark pairs into the final states eν+ jets and μν+
             jets are selected, and the cross section and the b-jet
             identification efficiency are determined using a new
             measurement technique which requires agreement between the
             measured cross sections with exactly one and with multiple
             identified b quarks from the top-quark decays. Assuming a
             top-quark mass of 175GeV/c2, a cross section of
             8.5±0.6(stat)±0. 7(syst)pb is measured. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.83.071102},
   Key = {fds309293}
}

@article{fds309266,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Measurement of the production cross section for W-bosons in
             association with jets in pp collisions at √s=7 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {698},
   Number = {5},
   Pages = {325-345},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.03.012},
   Abstract = {This Letter reports on a first measurement of the inclusive
             W+jets cross section in proton-proton collisions at a
             centre-of-mass energy of 7 TeV at the LHC, with the ATLAS
             detector. Cross sections, in both the electron and muon
             decay modes of the W-boson, are presented as a function of
             jet multiplicity and of the transverse momentum of the
             leading and next-to-leading jets in the event. Measurements
             are also presented of the ratio of cross sections
             σ(W+≥n)/σ(W+≥n-1) for inclusive jet multiplicities
             n=1-4. The results, based on an integrated luminosity of 1.3
             pb-1, have been corrected for all known detector effects and
             are quoted in a limited and well-defined range of jet and
             lepton kinematics. The measured cross sections are compared
             to particle-level predictions based on perturbative QCD.
             Next-to-leading order calculations, studied here for n≤2,
             are found in good agreement with the data. Leading-order
             multiparton event generators, normalized to the NNLO total
             cross section, describe the data well for all measured jet
             multiplicities. © 2011 CERN Elsevier B.V.},
   Doi = {10.1016/j.physletb.2011.03.012},
   Key = {fds309266}
}

@article{fds309285,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Search for massive long-lived highly ionising particles with
             the ATLAS detector at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {698},
   Number = {5},
   Pages = {353-370},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.03.033},
   Abstract = {A search is made for massive highly ionising particles with
             lifetimes in excess of 100 ns, with the ATLAS experiment at
             the Large Hadron Collider, using 3.1 pb-1 of pp collision
             data taken at √s=7 TeV. The signature of energy loss in
             the ATLAS inner detector and electromagnetic calorimeter is
             used. No such particles are found and limits on the
             production cross section for electric charges 6e≤|q|≤17e
             and masses 200 GeV≤m≤1000 GeV are set in the range 1-12
             pb for different hypotheses on the production mechanism. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.03.033},
   Key = {fds309285}
}

@article{fds309304,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
   Title = {Measurement of the top quark mass in the lepton+jets channel
             using the lepton transverse momentum},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {698},
   Number = {5},
   Pages = {371-379},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.03.041},
   Abstract = {This Letter reports a measurement of the top quark mass,
             Mtop, in data from pp- collisions at s=1.96 TeV
             corresponding to 2.7 fb-1 of integrated luminosity at the
             Fermilab Tevatron using the CDF II detector. Events with the
             lepton+jets topology are selected. An unbinned likelihood is
             constructed based on the dependence of the lepton transverse
             momentum, PT, on Mtop. A maximum likelihood fit to the data
             yields a measured mass Mtop=176.9±8.0stat±2.7syst GeV/c2.
             In this measurement, the contribution by the jet energy
             scale uncertainty to the systematic error is negligible. The
             result provides an important consistency test for other Mtop
             measurements where explicit use of the jet energy is made
             for deriving the top quark mass. © 2011 Elsevier
             B.V.},
   Doi = {10.1016/j.physletb.2011.03.041},
   Key = {fds309304}
}

@article{fds309249,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for Production of Heavy Particles Decaying to Top
             Quarks and Invisible Particles in $p\overline{p}$ Collisions
             at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {19},
   Pages = {191801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.191801},
   Abstract = {We present a search for a new particle T' decaying to top
             quark via T' → t + X, where X is an invisible particle. In
             a data sample with 4.8  fb(-1) of integrated luminosity
             collected by the CDF II detector at Fermilab in pp
             collisions with √s = 1.96  TeV, we search for pair
             production of T' in the lepton + jets channel, pp → tt + X
             + X → ℓνbqq'b + X + X. We interpret our results
             primarily in terms of a model where T' are exotic fourth
             generation quarks and X are dark matter particles. Current
             direct and indirect bounds on such exotic quarks restrict
             their masses to be between 300 and 600  GeV/c2, the dark
             matter particle mass being anywhere below m(T'). The data
             are consistent with standard model expectations, and we set
             95% confidence level limits on the generic production of
             T'T' → tt + X + X. For the dark matter model we exclude T'
             at 95% confidence level up to m(T') = 360  GeV/c2 for
             m(X) ≤ 100  GeV/c2.},
   Doi = {10.1103/PhysRevLett.106.191801},
   Key = {fds309249}
}

@article{fds309250,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurements of Direct ${CP}$ Violating Asymmetries in
             Charmless Decays of Strange Bottom Mesons and Bottom
             Baryons},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {18},
   Pages = {181802},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.181802},
   Abstract = {We report measurements of direct CP-violating asymmetries in
             charmless decays of neutral bottom hadrons to pairs of
             charged hadrons with the upgraded Collider Detector at the
             Fermilab Tevatron. Using a data sample corresponding to 1
             fb(-1) of integrated luminosity, we obtain the first
             measurements of direct CP violation in bottom strange
             mesons, A(CP)(B(s)(0)→K(-)π(+))=+0.39±0.15(stat)±0.08(syst),
             and bottom baryons, A(CP)(Λ(b)(0)→pπ(-))=+0.03±0.17(stat)±0.05(syst)
             and A(CP)(Λ(b)(0)→pK(-))=+0.37±0.17(stat)±0.03(syst).
             In addition, we measure CP violation in B(0)→K(+)π(-)
             decays with 3.5σ significance, A(CP)(B(0)→K(+)π(-))=-0.086±0.023(stat)±0.009(syst),
             in agreement with the current world average. Measurements of
             branching fractions of B(s)(0)→K(+)K(-) and
             B(0)→π(+)π(-) decays are also updated.},
   Doi = {10.1103/PhysRevLett.106.181802},
   Key = {fds309250}
}

@article{fds309262,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Ackers, M and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahmed, H and Ahsan, M and Aielli, G and Akdogan,
             T and Ákesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, J and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antos, J and Antunovic, B and Anulli, F and Aoun, S and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Argyropoulos, T and Arik, E and Arik, M and Armbruster,
             AJ and Arms, KE and Armstrong, SR and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Measurement of underlying event characteristics using
             charged particles in pp collisions at √s=900GeV and 7 TeV
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {83},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112001},
   Abstract = {Measurements of charged particle distributions, sensitive to
             the underlying event, have been performed with the ATLAS
             detector at the LHC. The measurements are based on data
             collected using a minimum-bias trigger to select
             proton-proton collisions at center-of-mass energies of 900
             GeV and 7 TeV. The "underlying event" is defined as those
             aspects of a hadronic interaction attributed not to the hard
             scattering process, but rather to the accompanying
             interactions of the rest of the proton. Three regions are
             defined in azimuthal angle with respect to the highest
             transverse momentum charged particle in the event, such that
             the region transverse to the dominant momentum-flow is most
             sensitive to the underlying event. In each of these regions,
             distributions of the charged particle multiplicity,
             transverse momentum density, and average pT are measured.
             The data show generally higher underlying event activity
             than that predicted by Monte Carlo models tuned to pre-LHC
             data. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.83.112001},
   Key = {fds309262}
}

@article{fds309247,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos Santos Pedrosa,
             F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci,
             F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Biesiada, J and Biglietti,
             M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blocker, C and Blocki, J and Blondel, A and Blum,
             W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Bona, M and Bondarenko, VG and Boonekamp, M and Boorman, G and Booth, CN and Booth, P and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni,
             S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik,
             J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton,
             D and Brett, ND and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brubaker, E and Bruckman de Renstrom,
             PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni,
             G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan,
             NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark,
             D and Buis, EJ and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camard, A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carpentieri,
             C and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho,
             J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavallari,
             A and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Cazzato, A and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, L and Chen, S and Chen, T and Chen, X and Cheng,
             S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal,
             M},
   Title = {Search for a heavy particle decaying into an electron and a
             muon with the ATLAS detector in sqrt[s] = 7 TeV pp
             collisions at the LHC.},
   Journal = {Physical review letters},
   Volume = {106},
   Number = {25},
   Pages = {251801},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.106.251801},
   Abstract = {This Letter presents the first search for a heavy particle
             decaying into an e ± μ(-/+) final state in sqrt[s] = 7 TeV
             pp collisions at the LHC. The data were recorded by the
             ATLAS detector during 2010 and correspond to a total
             integrated luminosity of 35 pb(-1). No excess above the
             standard model background expectation is observed.
             Exclusions at 95% confidence level are placed on two
             representative models. In an R-parity violating
             supersymmetric model, tau sneutrinos with a mass below 0.75
             TeV are excluded, assuming all R-parity violating couplings
             are zero except λ(311)' = 0.11 and λ312 = 0.07. In a
             lepton flavor violating model, a Z'-like vector boson with
             masses of 0.70-1.00 TeV and corresponding cross sections
             times branching ratios of 0.175-0.183 pb is excluded. These
             results extend to higher mass R-parity violating sneutrinos
             and lepton flavor violating Z's than previous constraints
             from the Tevatron.},
   Doi = {10.1103/physrevlett.106.251801},
   Key = {fds309247}
}

@article{fds309248,
   Author = {Aaltonen, and T, and al, E},
   Title = {First Measurement of the Angular Coefficients of {Drell-Yan}
             ${e}^{+}{e}^{-}$ Pairs in the ${Z}$ Mass Region from
             $p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {106},
   Number = {24},
   Pages = {241801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevLett.106.241801},
   Abstract = {We report on the first measurement of the angular
             distributions of final state electrons in pp¯ → γ*/Z →
             e(+)e(-) + X events produced in the Z boson mass region at
             √s1.96 TeV. The data sample collected by the CDF II
             detector for this result corresponds to 2.1  fb(-1) of
             integrated luminosity. The angular distributions are studied
             as a function of the transverse momentum of the
             electron-positron pair and show good agreement with the
             Lam-Tung relation, consistent with a spin-1 description of
             the gluon, and demonstrate that, at high values of the
             transverse momentum, Z bosons are produced via
             quark-antiquark annihilation and quark-gluon Compton
             processes.},
   Doi = {10.1103/PhysRevLett.106.241801},
   Key = {fds309248}
}

@article{fds309283,
   Author = {Collaboration, AVKWGAEAATLAS},
   Title = {Search for high mass dilepton resonances in pp collisions at
             7 TeV with the ATLAS experiment},
   Journal = {Physics Letters B},
   Volume = {700},
   Number = {3-4},
   Pages = {163-180},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.04.044},
   Abstract = {This Letter presents a search for high mass e+e- or μ+μ-
             resonances in pp collisions at √s=7 TeV at the LHC. The
             data were recorded by the ATLAS experiment during 2010 and
             correspond to a total integrated luminosity of ~40 pb-1. No
             statistically significant excess above the Standard Model
             expectation is observed in the search region of dilepton
             invariant mass above 110 GeV. Upper limits at the 95%
             confidence level are set on the cross section times
             branching ratio of Z' resonances decaying to dielectrons and
             dimuons as a function of the resonance mass. A lower mass
             limit of 1.048 TeV on the Sequential Standard Model Z' boson
             is derived, as well as mass limits on Z* and E6-motivated Z'
             models. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.04.044},
   Key = {fds309283}
}

@article{fds309288,
   Author = {Aaltonen, and T, and al, E},
   Title = {Top quark mass measurement using the template method at
             {CDF}},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {111101},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.111101},
   Abstract = {We present a measurement of the top quark mass in the
             lepton+jets and dilepton channels of tt̄ decays using the
             data sample corresponding to an integrated luminosity of
             5.6fb-1 of pp̄ collisions at Tevatron with √s=1.96TeV,
             collected with the CDF II detector. We construct templates
             of two reconstructed top quark masses from different
             jets-to-quarks combinations and the invariant mass of two
             jets from the W decays in the lepton+jets channel, and a
             reconstructed top quark mass and mT2, a variable related to
             the transverse mass in events with two missing particles, in
             the dilepton channel. The simultaneous fit of the templates
             from signal and background events in the lepton+jets and
             dilepton channels to the data yields a measured top quark
             mass of Mtop=172.1±1.1(stat)±0. 9(syst)GeV/c2. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.111101},
   Key = {fds309288}
}

@article{fds309297,
   Author = {Aaltonen, and T, and al, E},
   Title = {Evidence for a mass dependent forward-backward asymmetry in
             top quark pair production},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {112003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112003},
   Abstract = {We present a new measurement of the inclusive
             forward-backward tt̄ production asymmetry and its rapidity
             and mass dependence. The measurements are performed with
             data corresponding to an integrated luminosity of 5.3fb -1
             of pp̄ collisions at √s=1.96TeV, recorded with the CDF-II
             Detector at the Fermilab Tevatron. Significant inclusive
             asymmetries are observed in both the laboratory frame and
             the tt̄ rest frame, and in both cases are found to be
             consistent with CP conservation under interchange of t and
             t̄. In the tt̄ rest frame, the asymmetry is observed to
             increase with the tt̄ rapidity difference, Δy, and with
             the invariant mass M tt̄ of the tt̄ system. Fully
             corrected parton-level asymmetries are derived in two
             regions of each variable, and the asymmetry is found to be
             most significant at large Δy and Mtt̄. For
             Mtt̄?450GeV/c2, the parton-level asymmetry in the tt̄ rest
             frame is Att̄=0.475±0.114 compared to a next-to-leading
             order QCD prediction of 0.088±0.013. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.83.112003},
   Key = {fds309297}
}

@article{fds309302,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of event shapes in $p\overline{p}$ collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {112007},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112007},
   Abstract = {A study of event-shape observables in proton-antiproton
             collisions at √s=1.96TeV is presented. The data for this
             analysis were recorded by the CDF II Detector at the
             Tevatron Collider. The variables studied are the transverse
             thrust and thrust minor, both defined in the plane
             perpendicular to the beam direction. The observables are
             measured using energies from unclustered calorimeter cells.
             In addition to studies of the differential distributions, we
             present the dependence of event-shape mean values on the
             leading-jet transverse energy. Data are compared with pythia
             Tune A and to resummed parton-level predictions that were
             matched to fixed-order results at next-to-leading-order
             (NLO) accuracy (NLO+NLL). Predictions from pythia Tune A
             agree fairly well with the data. However, the underlying
             event contributes significantly to these observables, making
             it difficult to make direct comparisons to the NLO+NLL
             predictions, which do not account for the underlying event.
             To overcome this difficulty, we introduce a new observable,
             a weighted difference of the mean values of the thrust and
             thrust minor, which is less sensitive to the underlying
             event, allowing for a comparison with NLO+NLL. Both pythia
             Tune A and the NLO+NLL calculations agree well within the
             20% theoretical uncertainty with the data for this
             observable, indicating that perturbative QCD successfully
             describes shapes of the hadronic final states. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.112007},
   Key = {fds309302}
}

@article{fds309303,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for new heavy particles decaying to ${ZZ}\rightarrow
             llll$, $lljj$ in $p\overline{p}$ collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Number = {11},
   Pages = {112008},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112008},
   Abstract = {We report on a search for anomalous production of Z boson
             pairs through a massive resonance decay in data
             corresponding to 2.5-2.9fb-1 of integrated luminosity in
             pp̄ collisions at √s=1.96TeV using the CDF II detector at
             the Fermilab Tevatron. This analysis, with more data and
             channels where the Z bosons decay to muons or jets,
             supersedes the 1.1fb-1 four-electron channel result
             previously published by CDF. In order to maintain high
             efficiency for muons, we use a new forward tracking
             algorithm and muon identification requirements optimized for
             these high signal-to-background channels. Predicting the
             dominant backgrounds in each channel entirely from sideband
             data samples, we observe four-body invariant mass spectra
             above 300GeV/c2 that are consistent with background. We set
             limits using the acceptance for a massive graviton resonance
             that are 7-20 times stronger than the previously published
             direct limits on resonant ZZ diboson production. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.83.112008},
   Key = {fds309303}
}

@article{fds309316,
   Author = {Oh, SH and Ebenstein, WL and Wang, CW},
   Title = {Multi-anode wire straw tube tracker},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {640},
   Number = {1},
   Pages = {160-163},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.nima.2011.02.105},
   Abstract = {We report on a test of a straw tube detector design having
             several anode (sense) wires inside a straw tube. The anode
             wires form a circle inside the tube and are read out
             independently. This design could solve several shortcomings
             of the traditional single wire straw tube design such as
             double hit capability and stereo configuration. © 2011
             Elsevier B.V. All rights reserved.},
   Doi = {10.1016/j.nima.2011.02.105},
   Key = {fds309316}
}

@article{fds309269,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Ákesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Search for pair production of first or second generation
             leptoquarks in proton-proton collisions at √s=7TeV using
             the ATLAS detector at the LHC},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {83},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.112006},
   Abstract = {This paper describes searches for the pair production of
             first or second generation scalar leptoquarks using 35pb-1
             of proton-proton collision data recorded by the ATLAS
             detector at √s=7TeV. Leptoquarks are searched in events
             with two oppositely-charged muons or electrons and at least
             two jets, and in events with one muon or electron, missing
             transverse momentum and at least two jets. After event
             selection, the observed yields are consistent with the
             predicted backgrounds. Leptoquark production is excluded at
             the 95 CL for masses MLQ<376 (319) GeV and MLQ<422 (362) GeV
             for first and second generation scalar leptoquarks,
             respectively, when assuming the branching fraction of a
             leptoquark to a charged lepton is equal to 1.0 (0.5). ©
             2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.83.112006},
   Key = {fds309269}
}

@article{fds321638,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Measurement of the W charge asymmetry in the W→μν decay
             mode in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {701},
   Number = {1},
   Pages = {31-49},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.05.024},
   Abstract = {This Letter reports a measurement of the muon charge
             asymmetry from W bosons produced in proton–proton
             collisions at a centre-of-mass energy of 7 TeV with the
             ATLAS experiment at the LHC. The asymmetry is measured in
             the W→μν decay mode as a function of the muon
             pseudorapidity using a data sample corresponding to a total
             integrated luminosity of 31 pb−1. The results are compared
             to predictions based on next-to-leading order calculations
             with various parton distribution functions. This measurement
             provides information on the u and d quark momentum fractions
             in the proton.},
   Doi = {10.1016/j.physletb.2011.05.024},
   Key = {fds321638}
}

@article{fds321639,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Ali, S and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S},
   Title = {Search for high-mass states with one lepton plus missing
             transverse momentum in proton–proton collisions at s=7 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {701},
   Number = {1},
   Pages = {50-69},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.05.043},
   Abstract = {The ATLAS detector is used to search for high-mass states,
             such as heavy charged gauge bosons (W′,W⁎), decaying to
             a charged lepton (electron or muon) and a neutrino. Results
             are presented based on the analysis of pp collisions at a
             center-of-mass energy of 7 TeV corresponding to an
             integrated luminosity of 36 pb−1. No excess beyond
             standard model expectations is observed. A W′ with
             sequential standard model couplings is excluded at 95%
             confidence level for masses below 1.49 TeV, and a W⁎
             (charged chiral boson) for masses below 1.35
             TeV.},
   Doi = {10.1016/j.physletb.2011.05.043},
   Key = {fds321639}
}

@article{fds321640,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TP and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B},
   Title = {Search for stable hadronising squarks and gluinos with the
             ATLAS experiment at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {701},
   Number = {1},
   Pages = {1-19},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.05.010},
   Abstract = {Hitherto unobserved long-lived massive particles with
             electric and/or colour charge are predicted by a range of
             theories which extend the Standard Model. In this Letter a
             search is performed at the ATLAS experiment for slow-moving
             charged particles produced in proton–proton collisions at
             7 TeV centre-of-mass energy at the LHC, using a data-set
             corresponding to an integrated luminosity of 34 pb−1. No
             deviations from Standard Model expectations are found. This
             result is interpreted in a framework of supersymmetry models
             in which coloured sparticles can hadronise into long-lived
             bound hadronic states, termed R-hadrons, and 95% CL limits
             are set on the production cross-sections of squarks and
             gluinos. The influence of R-hadron interactions in matter
             was studied using a number of different models, and lower
             mass limits for stable sbottoms and stops are found to be
             294 and 309 GeV respectively. The lower mass limit for a
             stable gluino lies in the range from 562 to 586 GeV
             depending on the model assumed. Each of these constraints is
             the most stringent to date.},
   Doi = {10.1016/j.physletb.2011.05.010},
   Key = {fds321640}
}

@article{fds309242,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for New Dielectron Resonances and {Randall-Sundrum}
             Gravitons at the {Collider Detector at Fermilab}},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {5},
   Pages = {051801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.051801},
   Abstract = {A search for new dielectron-mass resonances using data
             recorded by the CDF II detector and corresponding to an
             integrated luminosity of 5.7  fb(-1) is presented. No
             significant excess over the expected standard model
             prediction is observed. In this data set, an event with the
             highest dielectron mass ever observed (960  GeV/c(2))
             was recorded. The results are interpreted in the
             Randall-Sundrum (RS) model. Combined with the
             5.4  fb(-1) diphoton analysis, the RS-graviton
             lower-mass limit for the coupling k/M¯(Pl)=0.1 is
             1058  GeV/c(2), making it the strongest limit to
             date.},
   Doi = {10.1103/PhysRevLett.107.051801},
   Key = {fds309242}
}

@article{fds309243,
   Author = {Aaltonen, and T, and al, E},
   Title = {Limits on Anomalous Trilinear Gauge Couplings in ${Z}\gamma$
             Events from $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {5},
   Pages = {051802},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.051802},
   Abstract = {Using Zγ candidate events collected by the CDF detector at
             the Tevatron Collider, we search for potential anomalous
             (non-standard-model) couplings between the Z boson and the
             photon. Zγ couplings vanish at tree level and are heavily
             suppressed at higher orders; hence any evidence of couplings
             indicates new physics. Measurements are performed using data
             corresponding to an integrated luminosity of 4.9  fb(-1)
             in the Z→νν¯ decay channel and 5.1  fb(-1) in the
             Z→l(+)l(-) (l=μ, e) decay channels. The combination of
             these measurements provides the most stringent limits to
             date on Zγ trilinear gauge couplings. Using an energy scale
             of Λ=1.5  TeV to allow for a direct comparison with
             previous measurements, we find limits on the CP-conserving
             parameters that describe Zγ couplings to be
             |h(3)(γ,Z)|<0.022 and |h(4)(γ,Z)|<0.0009. These results
             are consistent with standard model predictions.},
   Doi = {10.1103/PhysRevLett.107.051802},
   Key = {fds309243}
}

@article{fds309244,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos Santos Pedrosa,
             F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci,
             F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Biesiada, J and Biglietti,
             M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
             A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Boonekamp, M and Boorman,
             G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Brubaker, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse,
             M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camard,
             A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Cazzato, A and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, L and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov,
             A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
             M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of the W+ W- cross section in sqrt(s) =
             7  TeV pp collisions with ATLAS.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {4},
   Pages = {041802},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.107.041802},
   Abstract = {This Letter presents a measurement of the W+ W- production
             cross section in sqrt(s) = 7  TeV pp collisions by the
             ATLAS experiment, using 34  pb(-1) of integrated
             luminosity produced by the Large Hadron Collider at CERN.
             Selecting events with two isolated leptons, each either an
             electron or a muon, 8 candidate events are observed with an
             expected background of 1.7 ± 0.6 events. The measured cross
             section is 41(-16)(+20)(stat) ± 5(syst)±1(lumi)  pb,
             which is consistent with the standard model prediction of 44
             ± 3  pb calculated at next-to-leading order in
             QCD.},
   Doi = {10.1103/physrevlett.107.041802},
   Key = {fds309244}
}

@article{fds309245,
   Author = {Aaltonen, and T, and al, E},
   Title = {First Search for Multijet Resonances in $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
             $p\overline{p}$ Collisions},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {4},
   Pages = {042001},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.042001},
   Abstract = {We present the first model independent search for three-jet
             hadronic resonances within multijet events in sqrt(s) =
             1.96  TeV pp collisions at the Fermilab Tevatron using
             the CDF II detector. Pair production of supersymmetric
             gluinos and squarks with hadronic R-parity violating decays
             is employed as an example of a new physics benchmark for
             this signature. Selection criteria based on the kinematic
             properties of an ensemble of jet combinations within each
             event help to extract signal from copious QCD background. No
             significant excess outside the top quark mass window is
             observed in data with an integrated luminosity of
             3.2  fb(-1). We place 95% confidence level limits on the
             production cross section σ(pp → XX')×BR(gg →
             3  jet + 3  jet) where X, X' = g, q, or q, with q, q
             → g + jet, as a function of gluino mass, in the range of
             77  GeV/c2 to 240  GeV/c2.},
   Doi = {10.1103/PhysRevLett.107.042001},
   Key = {fds309245}
}

@article{fds309246,
   Author = {Aaltonen, and T, and al, E},
   Title = {Search for a Very Light ${CP}$-Odd {H}iggs Boson in Top
             Quark Decays from $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {3},
   Pages = {031801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.031801},
   Abstract = {We present the results of a search for a very light CP-odd
             Higgs boson a(1)(0) originating from top quark decays t →
             H(±)b → W(±(*)) a(1)(0)b, and subsequently decaying into
             τ+ τ-. Using a data sample corresponding to an integrated
             luminosity of 2.7  fb(-1) collected by the CDF II
             detector in pp collisions at 1.96 TeV, we perform a search
             for events containing a lepton, three or more jets, and an
             additional isolated track with transverse momentum in the
             range 3 to 20  GeV/c. Observed events are consistent
             with background sources, and 95% C.L. limits are set on the
             branching ratio of t → H(±)b for various masses of H(±)
             and a(1)(0).},
   Doi = {10.1103/PhysRevLett.107.031801},
   Key = {fds309246}
}

@article{fds309282,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Search for contact interactions in dimuon events from pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.011101},
   Abstract = {A search for contact interactions has been performed using
             dimuon events recorded with the ATLAS detector in
             proton-proton collisions at √s=7TeV. The data sample
             corresponds to an integrated luminosity of 42pb-1. No
             significant deviation from the standard model is observed in
             the dimuon mass spectrum, allowing the following 95% C.L.
             limits to be set on the energy scale of contact
             interactions: Λ>4.9TeV (4.5 TeV) for constructive
             (destructive) interference in the left-left isoscalar
             compositeness model. These limits are the most stringent to
             date for μμqq contact interactions. 2011 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.84.011101},
   Key = {fds309282}
}

@article{fds309314,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for supersymmetric particles in events with lepton
             pairs and large missing transverse momentum in √s = 7 TeV
             proton-proton collisions with the ATLAS experiment},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {7},
   Pages = {18-19},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1682-6},
   Abstract = {Results are presented of searches for the production of
             supersymmetric particles decaying into final states with
             missing transverse momentum and exactly two isolated leptons
             in √s = 7 TeV proton-proton collisions at the Large Hadron
             Collider. Search strategies requiring lepton pairs with
             identical-sign or opposite-sign electric charges are
             described. In a data sample corresponding to an integrated
             luminosity of 35 pb-1 collected with the ATLAS detector, no
             significant excesses are observed. Based on specific
             benchmark models, limits are placed on the squark mass
             between 450 and 690 GeV for squarks approximately degenerate
             in mass with gluinos, depending on the supersymmetric mass
             hierarchy considered. © 2011 CERN for the benefit of the
             ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-011-1682-6},
   Key = {fds309314}
}

@article{fds309315,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for an excess of events with an identical flavour
             lepton pair and significant missing transverse momentum in
             √s = TeV proton-proton collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {7},
   Pages = {1-18},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {July},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1647-9},
   Abstract = {Results are presented of a search for particles decaying
             into final states with significant missing transverse
             momentum and exactly two identical flavour leptons (e, μ)
             of opposite charge in √s = TeV collisions at the Large
             Hadron Collider. This channel is particularly sensitive to
             supersymmetric particle cascade decays producing flavour
             correlated lepton pairs. Flavour uncorrelated backgrounds
             are subtracted using a sample of opposite flavour lepton
             pair events. Observation of an excess beyond Standard Model
             expectations following this subtraction procedure would
             offer one of the best routes to measuring the masses of
             supersymmetric particles. In a data sample corresponding to
             an integrated luminosity of 35 pb-1 no such excess is
             observed. Model-independent limits are set on the
             contribution to these final states from supersymmetry and
             are used to exclude regions of a phenomenological
             supersymmetric parameter space. © 2011 CERN for the benefit
             of the ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-011-1647-9},
   Key = {fds309315}
}

@article{fds309240,
   Author = {Aaltonen, and T, and al, E},
   Title = {Observation of the $\Xi_{b}^{0}$ Baryon},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {10},
   Pages = {102001},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.102001},
   Abstract = {The observation of the bottom, strange baryon Ξ(b)(0)
             through the decay chain Ξ(b)(0)→Ξ(c)(+)π-, where
             ΞΞ(c)(+)→Ξ- π+ π+, Ξ-→Λπ-, and Λ→pπ-, is
             reported by using data corresponding to an integrated
             luminosity of 4.2  fb(-1) from pp collisions at square
             root(s)=1.96  TeV recorded with the Collider Detector at
             Fermilab. A signal of 25.3(-5.4)(+5.6) candidates is
             observed whose probability of arising from a background
             fluctuation is 3.6×10(-12), corresponding to 6.8 gaussian
             standard deviations. The Ξ(b)(0) mass is measured to be
             5787.8±5.0(stat)±1.3(syst)  MeV/c2. In addition, the
             Ξ(b)- baryon is observed through the process
             Ξ(b)-→Ξ(c)(0)π-, where Ξ(c)(0)→Ξ- π+, Ξ-→Λπ-,
             and Λ→pπ-.},
   Doi = {10.1103/PhysRevLett.107.102001},
   Key = {fds309240}
}

@article{fds309298,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the $t\overline{t}$ production cross section
             in $p\overline{p}$ collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
             using events with large missing transverse energy and
             jets},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.032003},
   Abstract = {In this paper we report a measurement of the tt̄ production
             cross section in pp̄ collisions at √s=1.96TeV using data
             corresponding to an integrated luminosity of 2.2fb-1
             collected with the CDF II detector at the Tevatron
             accelerator. We select events with significant missing
             transverse energy and high jet multiplicity. This
             measurement vetoes the presence of explicitly identified
             electrons and muons, thus enhancing the tau contribution of
             tt̄ decays. Signal events are discriminated from the
             background using a neural network, and heavy flavor jets are
             identified by a secondary-vertex tagging algorithm. We
             measure a tt̄ production cross section of
             7.99±0.55(stat)±0.76(syst)±0.46(lumi) pb, assuming a top
             mass mtop=172.5GeV/c2, in agreement with previous
             measurements and standard model predictions. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.84.032003},
   Key = {fds309298}
}

@article{fds309300,
   Author = {Aaltonen, and T, and al, E},
   Title = {Measurement of the top pair production cross section in the
             $\mathrm{{lepton}}+\mathrm{{jets}}$ channel using a jet
             flavor discriminant},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {3},
   Pages = {031101},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.031101},
   Abstract = {We present a new method to measure the top quark pair
             production cross section and the background rates with data
             corresponding to an integrated luminosity of 2.7fb-1 from
             pp̄ collisions at √s=1.96TeV collected with the CDF II
             Detector. We select events with a single electron or muon
             candidate, missing transverse energy, and at least one
             b-tagged jet. We perform a simultaneous fit to a jet flavor
             discriminant across nine samples defined by the number of
             jets and b tags. An advantage of this approach is that many
             systematic uncertainties are measured in situ and inversely
             scale with integrated luminosity. We measure a top cross
             section of σ tt̄=7.64±0.57(stat+syst)±0.45(luminosity)pb.
             © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.031101},
   Key = {fds309300}
}

@article{fds309239,
   Author = {Aaltonen, TEA},
   Title = {Measurement of the Cross Section for Prompt Isolated
             Diphoton Production in $p\overline{p}$ Collisions at
             $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {10},
   Pages = {102003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.102003},
   Abstract = {This Letter reports a measurement of the cross section of
             prompt isolated photon pair production in pp collisions at a
             total energy square root(s)=1.96  TeV using data of
             5.36  fb(-1) integrated luminosity collected with the
             CDF II detector at the Fermilab Tevatron. The measured cross
             section, differential in basic kinematic variables, is
             compared with three perturbative QCD predictions, a leading
             order parton shower calculation and two next-to-leading
             order calculations. The next-to-leading order calculations
             reproduce most aspects of the data. By including photon
             radiation from quarks before and after hard scattering, the
             parton shower prediction becomes competitive with the
             next-to-leading order predictions.},
   Doi = {10.1103/PhysRevLett.107.102003},
   Key = {fds309239}
}

@article{fds309305,
   Author = {Aaltonen, TEA},
   Title = {Measurement of branching ratio and ${B}_{s}^{0}$ lifetime in
             the decay ${B}_{s}^{0}\rightarrow{J}/\psi{f}_{0}(980)$ at
             {CDF}},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {5},
   Pages = {052012},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.052012},
   Abstract = {We present a study of Bs0 decays to the CP-odd final state
             J/ψf 0(980) with J/ψ→μ+μ- and f 0(980)→π+π-. Using
             pp̄ collision data with an integrated luminosity of 3.8fb-1
             collected by the CDF II detector at the Tevatron we measure
             a Bs0 lifetime of τ(Bs0→J/ψf0(980))=1.70-0.11+0.12(stat)±0.03(syst)
             ps. This is the first measurement of the Bs0 lifetime in a
             decay to a CP eigenstate and corresponds in the standard
             model to the lifetime of the heavy Bs0 eigenstate. We also
             measure the product of branching fractions of
             Bs0→J/ψf0(980) and f0(980)→π +π- relative to the
             product of branching fractions of Bs0→J/ψ and →K+K- to
             be Rf0 /=0.257±0.020(stat)±0.014(syst), which is the most
             precise determination of this quantity to date. © 2011
             American Physical Society.},
   Doi = {10.1103/PhysRevD.84.052012},
   Key = {fds309305}
}

@article{fds309306,
   Author = {Aaltonen, TEA},
   Title = {Search for the {H}iggs boson in the all-hadronic final state
             using the {CDF II} detector},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {5},
   Pages = {052010},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.052010},
   Abstract = {We report on a search for the production of the Higgs boson
             decaying to two bottom quarks accompanied by two additional
             quarks. The data sample used corresponds to an integrated
             luminosity of approximately 4fb-1 of pp̄ collisions at
             √s=1.96TeV recorded by the CDF II experiment. This search
             includes twice the integrated luminosity of the previous
             published result, uses analysis techniques to distinguish
             jets originating from light flavor quarks and those from
             gluon radiation, and adds sensitivity to a Higgs boson
             produced by vector boson fusion. We find no evidence of the
             Higgs boson and place limits on the Higgs boson production
             cross section for Higgs boson masses between 100GeV/c2 and
             150GeV/c2 at the 95% confidence level. For a Higgs boson
             mass of 120GeV/c2, the observed (expected) limit is 10.5
             (20.0) times the predicted standard model cross section. ©
             2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.052010},
   Key = {fds309306}
}

@article{fds321636,
   Author = {ATLAS Collaboration},
   Title = {Measurement of the inelastic proton-proton cross-section at
             √s=7 TeV with the ATLAS detector.},
   Journal = {Nature communications},
   Volume = {2},
   Number = {1},
   Pages = {463},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1038/ncomms1472},
   Abstract = {The dependence of the rate of proton-proton interactions on
             the centre-of-mass collision energy, √s, is of fundamental
             importance for both hadron collider physics and particle
             astrophysics. The dependence cannot yet be calculated from
             first principles; therefore, experimental measurements are
             needed. Here we present the first measurement of the
             inelastic proton-proton interaction cross-section at a
             centre-of-mass energy, √s, of 7 TeV using the ATLAS
             detector at the Large Hadron Collider. Events are selected
             by requiring hits on scintillation counters mounted in the
             forward region of the detector. An inelastic cross-section
             of 60.3 ± 2.1 mb is measured for ξ > 5×10⁻⁶, where ξ
             is calculated from the invariant mass, M(X), of hadrons
             selected using the largest rapidity gap in the event. For
             diffractive events, this corresponds to requiring at least
             one of the dissociation masses to be larger than 15.7
             GeV.},
   Doi = {10.1038/ncomms1472},
   Key = {fds321636}
}

@article{fds309270,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Properties of jets measured from tracks in proton-proton
             collisions at center-of-mass energy √s=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.054001},
   Doi = {10.1103/PhysRevD.84.054001},
   Key = {fds309270}
}

@article{fds309236,
   Author = {Aaltonen, TEA},
   Title = {Search for New Physics in High ${p}_{T}$ Like-Sign Dilepton
             Events at {CDF II}},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {18},
   Pages = {181801},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.181801},
   Abstract = {We present a search for new physics in events with two high
             pT leptons of the same electric charge, using data with an
             integrated luminosity of 6.1 fb(-1). The observed data are
             consistent with standard model predictions. We set 95% C.L.
             lower limits on the mass of doubly charged scalars decaying
             to like-sign dileptons, m(H±±) > 190-245 GeV/c(2),
             assuming 100% BR to ee, μμ or eμ.},
   Doi = {10.1103/PhysRevLett.107.181801},
   Key = {fds309236}
}

@article{fds309238,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
   Title = {Inclusive search for same-sign dilepton signatures in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2011},
   Number = {10},
   Pages = {1-47},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2011)107},
   Abstract = {An inclusive search is presented for new physics in events
             with two isolated leptons (e or μ) having the same electric
             charge. The data are selected from events collected from pp
             collisions at √s = 7 TeV by the ATLAS detector and
             correspond to an integrated luminosity of 34 pb-1. The
             spectra in dilepton invariant mass, missing transverse
             momentum and jet multiplicity are presented and compared to
             Standard Model predictions. In this event sample, no
             evidence is found for contributions beyond those of the
             Standard Model. Limits are set on the cross-section in a
             fiducial region for new sources of same-sign high-mass
             dilepton events in the ee, eμ and μμ channels. Four
             models predicting same-sign dilepton signals are
             constrained: two descriptions of Majorana neutrinos, a
             cascade topology similar to supersymmetry or universal extra
             dimensions, and fourth generation d-type quarks. Assuming a
             new physics scale of 1 TeV, Majorana neutrinos produced by
             an effective operator V with masses below 460 GeV are
             excluded at 95% confidence level. A lower limit of 290 GeV
             is set at 95% confidence level on the mass of fourth
             generation d-type quarks. Copyright CERN.},
   Doi = {10.1007/JHEP10(2011)107},
   Key = {fds309238}
}

@article{fds309289,
   Author = {Aaltonen, TEA},
   Title = {Measurement of the top-quark mass in the lepton+jets channel
             using a matrix element technique with the {CDF II}
             detector},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {7},
   Pages = {071105},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.071105},
   Abstract = {A measurement of the top-quark mass is presented using
             Tevatron data from proton-antiproton collisions at
             center-of-mass energy √s=1.96TeV collected with the CDF II
             detector. Events are selected from a sample of candidates
             for production of tt̄ pairs that decay into the lepton+jets
             channel. The top-quark mass is measured with an unbinned
             maximum likelihood method where the event probability
             density functions are calculated using signal and background
             matrix elements, as well as a set of parametrized
             jet-to-parton transfer functions. The likelihood function is
             maximized with respect to the top-quark mass, the signal
             fraction in the sample, and a correction to the jet energy
             scale (JES) calibration of the calorimeter jets. The
             simultaneous measurement of the JES correction (ΔJES)
             amounts to an additional in situ jet energy calibration
             based on the known mass of the hadronically decaying W
             boson. Using the data sample of 578 lepton+jets candidate
             events, corresponding to 3.2fb-1 of integrated luminosity,
             the top-quark mass is measured to be mt=172.4±1.4(stat+ΔJES)±1.
             3(syst)GeV/c2. © 2011 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.84.071105},
   Key = {fds309289}
}

@article{fds309290,
   Author = {Aaltonen, TEA},
   Title = {Search for resonant production of $t\overline{t}$ decaying
             to jets in $p\overline{p}$ collisions at
             $\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.072003},
   Abstract = {This paper reports a search for nonstandard model topquark
             resonances, Z′, decaying to tt̄→W+bW -b̄, where both W
             decay to quarks. We examine the top-antitop quark invariant
             mass spectrum for the presence of narrow resonant states.
             The search uses a data sample of pp̄ collisions at a center
             of mass energy of 1.96 TeV collected by the CDF II detector
             at the Fermilab Tevatron, with an integrated luminosity of
             2.8fb-1. No evidence for top-antitop quark resonant
             production is found. We place upper limits on the production
             cross section times branching ratio for a specific topcolor
             assisted technicolor model in which the Z′ has a width of
             Γ Z′=0.012MZ′. Within this model, we exclude a Z′
             boson with masses below 805GeV/c2 at the 95% confidence
             level. © 2011 American Physical Society.},
   Doi = {10.1103/PhysRevD.84.072003},
   Key = {fds309290}
}

@article{fds309291,
   Author = {Aaltonen, TEA},
   Title = {Search for resonant production of $t\overline{t}$ pairs in
             $4.8{\,}{\,}{\mathrm{fb}}^{\mathbf{-}1}$ of integrated
             luminosity of $p\overline{p}$ collisions at
             $\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {7},
   Pages = {072004},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.072004},
   Abstract = {We search for resonant production of tt̄ pairs in 4.8fb-1
             integrated luminosity of pp̄ collision data at √s=1.96TeV
             in the lepton+jets decay channel, where one top quark decays
             leptonically and the other hadronically. A matrix-element
             reconstruction technique is used; for each event a
             probability density function of the tt̄ candidate invariant
             mass is sampled. These probability density functions are
             used to construct a likelihood function, whereby the cross
             section for resonant tt̄ production is estimated, given a
             hypothetical resonance mass and width. The data indicate no
             evidence of resonant production of tt̄ pairs. A benchmark
             model of leptophobic Z′→tt̄ is excluded with m
             Z′<900GeV/c2 at 95% confidence level. © 2011 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.84.072004},
   Key = {fds309291}
}

@article{fds309232,
   Author = {Aaltonen, TEA},
   Title = {Top-Quark Mass Measurement Using Events with Missing
             Transverse Energy and Jets at CDF},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {23},
   Pages = {232002},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.232002},
   Abstract = {We present a measurement of the top-quark mass using a
             sample of $t\bar{t}$ events in 5.7  fb-1 of integrated
             luminosity from $p\bar{p}$ collisions at the Fermilab
             Tevatron with $\sqrt{s}=1.96$  TeV and collected by the
             CDF II Detector. We select events having large missing
             transverse energy, and four, five, or six jets with at least
             one jet tagged as coming from a b quark, and reject events
             with identified charged leptons. This analysis considers
             events from the semileptonic tt̅ decay channel, including
             events that contain tau leptons. The measurement is based on
             a multidimensional template method. We fit the data to
             signal templates of varying top-quark masses and background
             templates, and measure a top-quark mass of Mtop=$172.32\pm
             2.4$(stat)$\pm 1.0$(syst)  GeV/c2.},
   Doi = {10.1103/PhysRevLett.107.232002},
   Key = {fds309232}
}

@article{fds309234,
   Author = {Aaltonen, TEA},
   Title = {Observation of the Baryonic Flavor-Changing Neutral Current
             Decay $\Lambda_{b}^{0}\rightarrow\Lambda\mu^{+}\mu^{-}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {20},
   Pages = {201802},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.201802},
   Abstract = {We report the first observation of the baryonic
             flavor-changing neutral current decay Λ(b)(0)→Λμ(+)μ(-)
             with 24 signal events and a statistical significance of 5.8
             Gaussian standard deviations. This measurement uses a pp
             collisions data sample corresponding to 6.8 fb(-1) at √s =
             1.96 TeV collected by the CDF II detector at the Tevatron
             collider. The total and differential branching ratios for
             Λ(b)(0)→Λμ(+)μ(-) are measured. We find
             B(Λ(b)(0)→Λμ(+)μ(-))=[1.73 ± 0.42(stat) ± (syst)] ×
             10(-6). We also report the first measurement of the
             differential branching ratio of B(s)(0)→ϕμ(+)μ(-),
             using 49 signal events. In addition, we report branching
             ratios for B(+)→K(+)μ(+)μ(-), B(0)→K(0)μ(+)μ(-), and
             B→K(*)(892)μ(+)μ(-) decays.},
   Doi = {10.1103/PhysRevLett.107.201802},
   Key = {fds309234}
}

@article{fds309235,
   Author = {Aaltonen, TEA},
   Title = {Search for New ${T}^\prime$ Particles in Final States with
             Large Jet Multiplicities and Missing Transverse Energy in
             $p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
   Journal = {Phys. Rev. Lett.},
   Volume = {107},
   Number = {19},
   Pages = {191803},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevLett.107.191803},
   Abstract = {We present a search for a new particle T' decaying to a top
             quark via T' → t + X, where X goes undetected. We use a
             data sample corresponding to 5.7 fb(-1) of integrated
             luminosity of p p collisions with sqrt[s] = 1.96 TeV,
             collected at Fermilab Tevatron by the CDF II detector. Our
             search for pair production of T' is focused on the hadronic
             decay channel, pp → T'T' → tt + XX → bqq b qq + XX. We
             interpret our results in terms of a model where T' is an
             exotic fourth generation quark and X is a dark matter
             particle. The data are consistent with standard model
             expectations. We set a limit on the generic production of
             T'T' → tt + XX, excluding the fourth generation exotic
             quarks T' at 95% confidence level up to m(T') = 400 GeV/c(2)
             for m(X) ≤ 70 GeV/c(2).},
   Doi = {10.1103/PhysRevLett.107.191803},
   Key = {fds309235}
}

@article{fds309307,
   Author = {Aaltonen, and T, and others},
   Title = {Measurements of branching fraction ratios and
             $CP$-asymmetries in suppressed ${B}^{-}\rightarrow
             D(\rightarrow{K}^{+}{\pi}^{-}){K}^{-}$ and
             ${B}^{-}\rightarrow D(\rightarrow{K}^{+} \pi^{-}){\pi}^{-}$
             decays},
   Journal = {Phys. Rev. D},
   Volume = {84},
   Number = {9},
   Pages = {091504},
   Publisher = {American Physical Society},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.091504},
   Abstract = {We report the first reconstruction in hadron collisions of
             the suppressed decays B-→D(→K+π-)K- and
             B-→D(→K+π-)π-, sensitive to the Cabibbo-Kobayashi-Maskawa
             phase γ, using data from 7  fb-1 of integrated
             luminosity collected by the CDF II detector at the Tevatron
             collider. We reconstruct a signal for the B-→D(→K+π-)K-
             suppressed mode with a significance of 3.2 standard
             deviations, and measure the ratios of the suppressed to
             favored branching fractions R(K)=[22.0$\pm$8.6(stat)$\pm$2.6(syst)]×10-3,
             R+(K)=[42.6$\pm$13.7(stat)$\pm$2.8(syst)]×10-3,
             R-(K)=[3.8$\pm$10.3(stat)$\pm$2.7(syst)]×10-3 as well as
             the direct CP-violating asymmetry A(K)=-0.82$\pm$0.44(stat)$\pm$0.09(syst)
             of this mode. Corresponding quantities for
             B-→D(→K+π-)π- decay are also reported.},
   Doi = {10.1103/PhysRevD.84.091504},
   Key = {fds309307}
}

@article{fds310122,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Search for a standard model Higgs boson in the
             H→ZZ→ℓ(+)ℓ(-)νν decay channel with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {22},
   Pages = {221802},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.107.221802},
   Abstract = {A search for a heavy standard model Higgs boson decaying via
             H→ZZ→→ℓ(+)ℓ(-)νν, where ℓ=e, μ, is presented.
             It is based on proton-proton collision data at √s=7 TeV,
             collected by the ATLAS experiment at the LHC in the first
             half of 2011 and corresponding to an integrated luminosity
             of 1.04 fb(-1). The data are compared to the expected
             standard model backgrounds. The data and the background
             expectations are found to be in agreement and upper limits
             are placed on the Higgs boson production cross section over
             the entire mass window considered; in particular, the
             production of a standard model Higgs boson is excluded in
             the region 340<m(H)<450 GeV at the 95% confidence
             level.},
   Doi = {10.1103/physrevlett.107.221802},
   Key = {fds310122}
}

@article{fds309277,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Search for new phenomena with the monojet and missing
             transverse momentum signature using the ATLAS detector in
             s=7TeV proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {4},
   Pages = {294-312},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.006},
   Abstract = {A search for new phenomena in events featuring a high energy
             jet and large missing transverse momentum in proton-proton
             collisions at s=7TeV is presented using a dataset
             corresponding to an integrated luminosity of 33 pb-1
             recorded with the ATLAS detector at the Large Hadron
             Collider. The number of observed events is consistent with
             the Standard Model prediction. This result is interpreted in
             terms of limits on a model of Large Extra Dimensions. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.10.006},
   Key = {fds309277}
}

@article{fds309273,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for the Standard Model Higgs boson in the two photon
             decay channel with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {5},
   Pages = {452-470},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.051},
   Abstract = {A search for the Standard Model Higgs boson in the two
             photon decay channel is reported, using 1.08 fb-1 of
             proton-proton collision data at a centre-of-mass energy of 7
             TeV recorded by the ATLAS detector. No significant excess is
             observed in the investigated mass range of 110-150 GeV.
             Upper limits on the cross-section times branching ratio of
             between 2.0 and 5.8 times the Standard Model prediction are
             derived for this mass range. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.10.051},
   Key = {fds309273}
}

@article{fds309274,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for the Standard Model Higgs boson in the decay
             channel H→ZZ(*)→4ℓ with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {5},
   Pages = {435-451},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.034},
   Abstract = {A search for the Standard Model Higgs boson in the decay
             channel H→ZZ(*)→ℓ+ℓ-ℓ'+ℓ'-, where ℓ=e, μ, is
             presented. Proton-proton collision data at s=7TeV recorded
             with the ATLAS detector and corresponding to an average
             integrated luminosity of 2.1fb-1 are compared to the
             Standard Model expectations. Upper limits on the production
             cross section of a Standard Model Higgs boson with a mass
             between 110 and 600GeV are derived. The observed (expected)
             95% confidence level upper limit on the production cross
             section for a Higgs boson with a mass of 194 GeV, the region
             with the best expected sensitivity for this search, is 0.99
             (1.01) times the Standard Model prediction. The Standard
             Model Higgs boson is excluded at 95% confidence level in the
             mass ranges 191-197, 199-200 and 214-224 GeV. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.10.034},
   Key = {fds309274}
}

@article{fds309275,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the transverse momentum distribution of
             Z/γ* bosons in proton-proton collisions at s=7
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {705},
   Number = {5},
   Pages = {415-434},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.10.018},
   Abstract = {A measurement of the Z/γ* transverse momentum (pTZ)
             distribution in proton-proton collisions at s=7 TeV is
             presented using Z/γ*→e+e- and Z/γ*→μ+μ- decays
             collected with the ATLAS detector in data sets with
             integrated luminosities of 35 pb-1 and 40 pb-1,
             respectively. The normalized differential cross sections are
             measured separately for electron and muon decay channels as
             well as for their combination up to pTZ of 350 GeV for
             invariant dilepton masses 66 GeV<mℓℓ<116 GeV. The
             measurement is compared to predictions of perturbative QCD
             and various event generators. The prediction of resummed QCD
             combined with fixed order perturbative QCD is found to be in
             good agreement with the data. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.10.018},
   Key = {fds309275}
}

@article{fds309227,
   Author = {Collaboration, AVKWGAEAATLAS},
   Title = {Search for dilepton resonances in pp collisions at 7 TeV
             with the ATLAS detector},
   Journal = {Physical Review Letters},
   Volume = {107},
   Number = {27},
   Pages = {272002},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.272002},
   Abstract = {This Letter reports on a search for narrow high-mass
             resonances decaying into dilepton final states. The data
             were recorded by the ATLAS experiment in pp collisions at
             √s=7  TeV at the Large Hadron Collider and correspond
             to a total integrated luminosity of 1.08 (1.21)  fb(-1)
             in the e(+)e(-) (μ(+)μ(-)) channel. No statistically
             significant excess above the standard model expectation is
             observed and upper limits are set at the 95% C.L. on the
             cross section times branching fraction of Z' resonances and
             Randall-Sundrum gravitons decaying into dileptons as a
             function of the resonance mass. A lower mass limit of 1.83
             TeV on the sequential standard model Z' boson is set. A
             Randall-Sundrum graviton with coupling k/M(Pl)=0.1 is
             excluded at 95% C.L. for masses below 1.63
             TeV.},
   Doi = {10.1103/physrevlett.107.272002},
   Key = {fds309227}
}

@article{fds309228,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
             M and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, H-C and Farrington, S and Feindt,
             M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
             E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
             T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
             J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
             R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan,
             N and Redondo, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
             S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
             M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
             RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
             D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
   Title = {Measurement of the B(s)0 lifetime in fully and partially
             reconstructed B(s)0→D(s)(-)(ϕπ(-))X decays in p¯p
             collisions at √s=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {27},
   Pages = {272001},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.272001},
   Abstract = {We present a measurement of the B(s)(0) lifetime in fully
             and partially reconstructed B(s)(0)→D(s)(-)(ϕπ(-))X
             decays in 1.3  fb(-1) collected in pp ¯ collisions at
             √s=1.96 TeV by the CDF II detector at the Fermilab
             Tevatron. We measure τ(B(s)(0))=1.518±0.041(stat)±0.027(syst)  ps.
             The ratio of this result and the world average B(0) lifetime
             yields τ(B(s)(0))/τ(B(0))=0.99±0.03, which is in
             agreement with recent theoretical predictions.},
   Doi = {10.1103/physrevlett.107.272001},
   Key = {fds309228}
}

@article{fds309229,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
             Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
             L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
             E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
             T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
             J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
             R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
             T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
             L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
             M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
             M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
             RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
             D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
   Title = {Search for a heavy toplike quark in pp collisions at
             √s=1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {26},
   Pages = {261801},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.261801},
   Abstract = {We present the results of a search for pair production of a
             heavy toplike (t') quark decaying to Wq final states using
             data corresponding to an integrated luminosity of 5.6 fb(-1)
             collected by the CDF II detector in pp collisions at
             √s=1.96 TeV. We perform parallel searches for t'→Wb and
             t'→Wq (where q is a generic down-type quark) in events
             containing a lepton and four or more jets. By performing a
             fit to the two-dimensional distribution of total transverse
             energy versus reconstructed t' quark mass, we set upper
             limits on the t't' production cross section and exclude a
             standard model fourth-generation t' quark decaying to Wb
             (Wq) with mass below 358 (340) GeV/c(2) at 95%
             C.L.},
   Doi = {10.1103/physrevlett.107.261801},
   Key = {fds309229}
}

@article{fds309230,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
             M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
             A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rosner, JL and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
             T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
             S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
             RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
             J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
             WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
             YC},
   Title = {Measurement of polarization and search for CP violation in
             B(s)0→φφ decays.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {26},
   Pages = {261802},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.261802},
   Abstract = {We present the first measurement of polarization and
             CP-violating asymmetries in a B(s)(0) decay into two light
             vector mesons, B(s)(0)→φφ, and an improved determination
             of its branching ratio using 295 decays reconstructed in a
             data sample corresponding to 2.9 fb(-1) of integrated
             luminosity collected by the CDF experiment at the Fermilab
             Tevatron collider. The fraction of longitudinal polarization
             is determined to be f(L)=0.348±0.041(stat)±0.021(syst),
             and the branching ratio B(B(s)(0)→φφ)=[2.32±0.18(stat)±0.82(syst)]×10(-5).
             Asymmetries of decay angle distributions sensitive to CP
             violation are measured to be A(u)=-0.007±0.064(stat)±0.018(syst)
             and A(v)=-0.120±0.064(stat)±0.016(syst).},
   Doi = {10.1103/physrevlett.107.261802},
   Key = {fds309230}
}

@article{fds309231,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Search for the Higgs boson in the H→WW→lνjj decay
             channel in pp collisions at √s=7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {107},
   Number = {23},
   Pages = {231801},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.107.231801},
   Abstract = {A search for a Higgs boson has been performed in the
             H→WW→ℓνjj channel in 1.04 fb(-1) of pp collision data
             at √s=7 TeV recorded with the ATLAS detector at the Large
             Hadron Collider. No significant excess of events is observed
             over the expected background and limits on the Higgs boson
             production cross section are derived for a Higgs boson mass
             in the range 240 GeV<m(H)<600 GeV. The best sensitivity is
             reached for m(H)=400 GeV, where the 95% confidence level
             upper bound on the cross section for H→WW production is
             3.1 pb, or 2.7 times the standard model prediction.},
   Doi = {10.1103/physrevlett.107.231801},
   Key = {fds309231}
}

@article{fds309271,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the inclusive isolated prompt photon
             cross-section in pp collisions at √s=7 TeV using 35
             pb-1 of ATLAS data},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {706},
   Number = {2-3},
   Pages = {150-167},
   Publisher = {Elsevier BV},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.010},
   Abstract = {A measurement of the differential cross-section for the
             inclusive production of isolated prompt photons in pp
             collisions at a center-of-mass energy √s=7 TeV is
             presented. The measurement covers the pseudorapidity ranges
             |η|<1.37 and 1.52≤|η|<2.37 in the transverse energy
             range 45≤ET<400 GeV. The results are based on an
             integrated luminosity of 35 pb-1, collected with the ATLAS
             detector at the LHC. The yields of the signal photons are
             measured using a data-driven technique, based on the
             observed distribution of the hadronic energy in a narrow
             cone around the photon candidate and the photon selection
             criteria. The results are compared with next-to-leading
             order perturbative QCD calculations and found to be in good
             agreement over four orders of magnitude in cross-section. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.010},
   Key = {fds309271}
}

@article{fds310557,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, T and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, A and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Search for a heavy neutral particle decaying into an
             electron and a muon using 1 fb-1 of atlas
             data},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1809-9},
   Abstract = {A search is presented for a high mass neutral particle that
             decays directly to the e±μ∓ final state. The data sample
             was recorded by the ATLAS detector in √ s = 7 TeV pp
             collisions at the LHC from March to June 2011 and
             corresponds to an integrated luminosity of 1.07 fb-1. The
             data are found to be consistent with the Standard Model
             background. The high e±μ∓ mass region is used to set 95%
             confidence level upper limits on the production of two
             possible new physics processes: tau sneutrinos in an
             R-parity violating supersymmetric model and Z'-like vector
             bosons in a lepton flavor violating model.},
   Doi = {10.1140/epjc/s10052-011-1809-9},
   Key = {fds310557}
}

@article{fds309268,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the Z→ττ cross section with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {84},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.84.112006},
   Abstract = {The Z→ττ cross section is measured with the ATLAS
             experiment at the LHC in four different final states
             determined by the decay modes of the τ leptons:
             muon-hadron, electron-hadron, electron-muon, and muon-muon.
             The analysis is based on a data sample corresponding to an
             integrated luminosity of 36pb-1, at a proton-proton
             center-of-mass energy of √s=7TeV. Cross sections are
             measured separately for each final state in fiducial regions
             of high detector acceptance, as well as in the full phase
             space, over the mass region 66-116 GeV. The individual cross
             sections are combined and the product of the total Z
             production cross section and Z→ττ branching fraction is
             measured to be 0.97±0.07(stat)±0.06(syst)±0.03(lumi)nb,
             in agreement with next-to-next-to-leading order
             calculations. © 2011 CERN.},
   Doi = {10.1103/PhysRevD.84.112006},
   Key = {fds309268}
}

@article{fds310558,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the jet fragmentation function and transverse
             profile in proton–proton collisions at a center-of-mass
             energy of 7 TeV with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {71},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2011},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1795-y},
   Abstract = {The jet fragmentation function and transverse profile for
             jets with 25 GeV< pTjet < 500 GeV and |ηjet| < 1.2 produced
             in proton–proton collisions with a center-ofmass energy of
             7 TeV are presented. The measurement is performed using data
             with an integrated luminosity of 36 pb−1. Jets are
             reconstructed and their momentum measured using calorimetric
             information. The momenta of the charged particle
             constituents are measured using the tracking system. The
             distributions corrected for detector effects are compared
             with various Monte Carlo event generators and generator
             tunes. Several of these choices show good agreement with the
             measured fragmentation function. None of these choices
             reproduce both the transverse profile and fragmentation
             function over the full kinematic range of the
             measurement.},
   Doi = {10.1140/epjc/s10052-011-1795-y},
   Key = {fds310558}
}

@article{fds341957,
   Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco,
             SD and Lorenzo, GD and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
             MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
             J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
             M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
             HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
             A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
             ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
             C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
             F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa,
             K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson,
             GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, C and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wen, A and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund,
             AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
             J},
   Title = {Production of Λ0, Λ ̄0, Ξ ±, and
             Ω± hyperons in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {1},
   Year = {2012},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.012002},
   Abstract = {We report a set of measurements of inclusive invariant p T
             differential cross sections of Λ0, Λ ̄0, Ξ ±, and Ω ±
             hyperons reconstructed in the central region with
             pseudorapidity |η|&lt;1 and p T up to 10GeV/c. Events are
             collected with a minimum-bias trigger in pp̄ collisions at
             a center-of-mass energy of 1.96 TeV using the CDF II
             detector at the Tevatron Collider. As p T increases, the
             slopes of the differential cross sections of the three
             particles are similar, which could indicate a universality
             of the particle production in p T. The invariant
             differential cross sections are also presented for different
             charged-particle multiplicity intervals. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.86.012002},
   Key = {fds341957}
}

@article{fds320779,
   Author = {ATLAS Collaboration},
   Title = {Search for a heavy top-quark partner in final states with
             two leptons with the ATLAS detector at the
             LHC},
   Journal = {JHEP},
   Volume = {1211},
   Number = {11},
   Pages = {094},
   Publisher = {Springer Nature},
   Year = {2012},
   url = {http://dx.doi.org/10.1007/JHEP11(2012)094},
   Abstract = {http://dx.doi.org/10.1007/JHEP11(2012)094},
   Doi = {10.1007/JHEP11(2012)094},
   Key = {fds320779}
}

@article{fds313389,
   Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
             M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou,
             V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh,
             SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov,
             O and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
             A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Squillacioti, P and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
             M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh,
             J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S},
   Title = {Measurement of the branching fraction B(Λb0→Λc+π
             -π +π -) at
             CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032003},
   Abstract = {We report an analysis of the Λb0→Λc+π -π +π - decay
             in a data sample collected by the CDF II detector at the
             Fermilab Tevatron corresponding to 2.4fb -1 of integrated
             luminosity. We reconstruct the currently largest samples of
             the decay modes Λb0→Λ c(2595) +π - (with Λ c(2595)
             +→Λc+π +π -), Λb0→Λ c(2625) +π - (with Λ c(2625)
             +→Λc+π +π -), Λb0→Σ c(2455) ++π -π - (with Σ
             c(2455) ++→Λc+π +), and Λb0→Σ c(2455)0π +π - (with
             Σ c(2455)0→Λc+π -) and measure the branching fractions
             relative to the Λb0→Λc+π - branching fraction. We
             measure the ratio B(Λb0→Λc+π -π +π -)/B(Λb0→Λc+π
             -)=3.04±0.33(stat)-0.55+0.70(syst) which is used to derive
             B(Λb0→Λc+π -π +π -)= (26.8-11.2+11.9)×10 -3. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.032003},
   Key = {fds313389}
}

@article{fds309049,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             TJ and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amonm, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeenm, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, R and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, R and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, R and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Bege,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botteri, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casadoll, MP and Cascela,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, R and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavalleri, R and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RI and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, TJ and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C},
   Title = {Search for the Standard Model Higgs boson produced in
             association with a vector boson and decaying to a
             b-quark pair with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {2},
   Pages = {369-390},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.10.061},
   Abstract = {© 2012 CERN This Letter presents the results of a direct
             search with the ATLAS detector at the LHC for a Standard
             Model Higgs boson of mass 110⩽mH⩽130 GeV produced in
             association with a W or Z boson and decaying to bb¯. Three
             decay channels are considered: ZH→ℓ+ℓ−bb¯
             WH→ℓνbb¯ and ZH→νν¯bb¯ where ℓ corresponds to
             an electron or a muon. No evidence for Higgs boson
             production is observed in a dataset of 7 TeV pp collisions
             corresponding to 4.7 fb−1 of integrated luminosity
             collected by ATLAS in 2011. Exclusion limits on Higgs boson
             production, at the 95% confidence level, of 2.5 to 5.5 times
             the Standard Model cross section are obtained in the mass
             range 110–130 GeV. The expected exclusion limits range
             between 2.5 and 4.9 for the same mass interval.},
   Doi = {10.1016/j.physletb.2012.10.061},
   Key = {fds309049}
}

@article{fds309065,
   Author = {ATLAS Collaboration},
   Title = {Search for light top squark pair production in final states
             with leptons and b-jets with the ATLAS detector in sqrt(s) =
             7 TeV proton-proton collisions},
   Journal = {Physics Letters B},
   Volume = {72},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2012},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2237-1},
   Abstract = {A search is presented for the pair production of light
             scalar top quarks in √s = 7 TeV proton–proton collisions
             recorded with the ATLAS detector at the Large Hadron
             Collider. This analysis uses the full data sample collected
             during 2011 running that corresponds to a total integrated
             luminosity of 4.7 fb−1. Light scalar top quarks are
             searched for in events with two opposite-sign leptons (e,
             μ), large missing transverse momentum and at least one jet
             in the final state. No excess over Standard Model
             expectations is found, and the results are interpreted under
             the assumption that the light scalar top decays to a b-quark
             in addition to an on-shell chargino whose decay occurs
             through a virtual W boson. If the chargino mass is 106 GeV,
             light scalar top-quark masses up to 130 GeV are excluded for
             neutralino masses below 70 GeV.},
   Doi = {10.1140/epjc/s10052-012-2237-1},
   Key = {fds309065}
}

@article{fds309118,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli,
             EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani,
             G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for TeV-scale gravity signatures in final states with
             leptons and jets with the ATLAS detector at √ s=7
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {122-141},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.009},
   Abstract = {The production of events with multiple high transverse
             momentum particles including charged leptons and jets is
             measured, using 1.04 fb-1 of proton-proton collision data
             recorded by the ATLAS detector during the first half of 2011
             at √s=7 TeV. No excess beyond Standard Model expectations
             is observed, and upper limits on the fiducial cross sections
             for non-Standard Model production of these final states are
             set. Using models for string ball and black hole production
             and decay, exclusion contours are determined as a function
             of mass threshold and the fundamental gravity scale. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.08.009},
   Key = {fds309118}
}

@article{fds309120,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli,
             EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani,
             G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for new particles decaying to ZZ using final states
             with leptons and jets with the ATLAS detector in √s=7 TeV
             proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {4-5},
   Pages = {331-350},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.05.020},
   Abstract = {A search is presented for a narrow resonance decaying to a
             pair of Z bosons using data corresponding to 1.02fb-1 of
             integrated luminosity collected by the ATLAS experiment from
             pp collisions at √s=7TeV. Events containing either four
             charged leptons (ℓℓℓℓ) or two charged leptons and
             two jets (ℓℓjj) are analyzed and found to be consistent
             with the Standard Model background expectation. Lower limits
             on a resonance mass are set using the Randall-Sundrum (RS1)
             graviton model as a benchmark. Using both ℓℓℓℓ and
             ℓℓjj events, an RS1 graviton with k/m-pl=0.1 and mass
             between 325 and 845 GeV is excluded at 95% confidence level.
             In addition, the ℓℓℓℓ events are used to set a
             model-independent fiducial cross section limit of
             σfid(pp→X→ZZ)&lt;0.92pb at 95% confidence level for any
             new sources of ZZ production with mZZ greater than 300 GeV.
             © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.05.020},
   Key = {fds309120}
}

@article{fds309122,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães Da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman De Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Forward-backward correlations and charged-particle azimuthal
             distributions in pp interactions using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {7},
   Year = {2012},
   url = {http://dx.doi.org/10.1007/JHEP07(1992)019},
   Abstract = {Using inelastic proton-proton interactions at √s =900 GeV
             and 7TeV, recorded by the ATLAS detector at the LHC,
             measurements have been made of the correlations between
             forward and backward charged-particle multiplicities and,
             for the first time, between forward and backward
             charged-particle summed transverse momentum. In addition,
             jet-like structure in the events is studied by means of
             azimuthal distributions of charged particles relative to the
             charged particle with highest transverse momentum in a
             selected kinematic region of the event. The results are
             compared with predictions from tunes of the PYTHIA and
             HERWIG++ Monte Carlo generators, which in most cases are
             found to provide a reasonable description of the
             data.},
   Doi = {10.1007/JHEP07(1992)019},
   Key = {fds309122}
}

@article{fds309125,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for contact interactions in dilepton events from pp
             collisions at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {1-2},
   Pages = {40-58},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.04.026},
   Abstract = {This Letter presents a search for contact interactions in
             the dielectron and dimuon channels using data from
             proton-proton collisions produced by the LHC at s=7 TeV and
             recorded by the ATLAS detector. The data sample, collected
             in 2011, corresponds to an integrated luminosity of 1.08 and
             1.21 fb-1 in the e+e- and μ+μ- channels, respectively. No
             significant deviations from the standard model are observed.
             Using a Bayesian approach with a prior flat in 1/Λ2, the
             following 95% CL lower limits are placed on the energy scale
             of ℓℓqq contact interactions: Λ-&gt;10.1 TeV
             (Λ+&gt;9.4 TeV) in the electron channel and Λ-&gt;8.0 TeV
             (Λ+&gt;7.0 TeV) in the muon channel for constructive
             (destructive) interference in the left-left isoscalar
             contact interaction model. Limits are also provided for a
             prior flat in 1/Λ4. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.04.026},
   Key = {fds309125}
}

@article{fds309126,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for extra dimensions using diphoton events in 7 TeV
             proton-proton collisions with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {4-5},
   Pages = {538-556},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.022},
   Abstract = {Using data recorded in 2011 with the ATLAS detector at the
             Large Hadron Collider, a search for evidence of extra
             spatial dimensions has been performed through an analysis of
             the diphoton final state. The analysis uses data
             corresponding to an integrated luminosity of 2.12fb-1 of
             s=7TeV proton-proton collisions. The diphoton invariant mass
             (mγγ) spectrum is observed to be in good agreement with
             the expected Standard Model background. In the large extra
             dimension scenario of Arkani-Hamed, Dimopoulos and Dvali,
             the results provide 95% CL lower limits on the fundamental
             Planck scale between 2.27 and 3.53 TeV, depending on the
             number of extra dimensions and the theoretical formalism
             used. The results also set 95% CL lower limits on the
             lightest Randall-Sundrum graviton mass of between 0.79 and
             1.85 TeV, for values of the dimensionless coupling k/-1 Pl
             varying from 0.01 to 0.1. Combining with previously
             published ATLAS results from the dielectron and dimuon final
             states, the 95% CL lower limit on the Randall-Sundrum
             graviton mass for k/M-1Pl=0.01 (0.1) is 0.80 (1.95) TeV. ©
             2012 CERN.},
   Doi = {10.1016/j.physletb.2012.03.022},
   Key = {fds309126}
}

@article{fds309155,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, SW and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart,
             H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
             M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
   Title = {Search for diphoton events with large missing transverse
             momentum in 1 fb -1 of 7 TeV proton-proton
             collision data with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {4-5},
   Pages = {519-537},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.054},
   Abstract = {A search for diphoton events with large missing transverse
             momentum has been performed using 1.07 fb -1 of
             proton-proton collision data at s=7 TeV recorded with the
             ATLAS detector. No excess of events was observed above the
             Standard Model prediction and 95% Confidence Level (CL)
             upper limits are set on the production cross section for new
             physics. The limits depend on each model parameter space and
             vary as follows: Λ&lt;(22-129) fb in the context of a
             generalised model of gauge-mediated supersymmetry breaking
             (GGM) with a bino-like lightest neutralino, σ&lt;(27-91) fb
             in the context of a minimal model of gauge-mediated
             supersymmetry breaking (SPS8), and σ&lt;(15-27) fb in the
             context of a specific model with one universal extra
             dimension (UED). A 95% CL lower limit of 805 GeV, for bino
             masses above 50 GeV, is set on the GGM gluino mass. Lower
             limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking
             scale Λ and on the UED compactification scale 1/R,
             respectively. These limits provide the most stringent tests
             of these models to date. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.054},
   Key = {fds309155}
}

@article{fds309160,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma,
             Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou,
             H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri,
             AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa,
             HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
             S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse,
             M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of the top quark pair production cross-section
             with ATLAS in the single lepton channel},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {711},
   Number = {3-4},
   Pages = {244-263},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.083},
   Abstract = {A measurement of the production cross-section for top quark
             pairs (tt-) in pp collisions at s=7TeV is presented using
             data recorded with the ATLAS detector at the Large Hadron
             Collider. Events are selected in the single lepton topology
             by requiring an electron or muon, large missing transverse
             momentum and at least three jets. With a data sample of 35
             pb -1, two different multivariate methods, one of which uses
             b-quark jet identification while the other does not, use
             kinematic variables to obtain cross-section measurements of
             σtt-=187±11(stat.)-17+18(syst.)±6(lumi.)pb and
             σtt-=173±17(stat.)-16+18(syst.)±6(lumi.)pb respectively.
             The two measurements are in agreement with each other and
             with QCD calculations. The first measurement has a better a
             priori sensitivity and constitutes the main result of this
             Letter. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.03.083},
   Key = {fds309160}
}

@article{fds309166,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and BenAmi, S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Böser, S and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik,
             J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
             LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino,
             G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya,
             GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J},
   Title = {Search for heavy vector-like quarks coupling to light quarks
             in proton-proton collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {1-2},
   Pages = {22-39},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.082},
   Abstract = {This Letter presents a search for singly produced
             vector-like quarks, Q, coupling to light quarks, q. The
             search is sensitive to both charged current (CC) and neutral
             current (NC) processes, pp→Qq→Wqq' and pp→Qq→Zqq'
             with a leptonic decay of the vector gauge boson. In 1.04fb-1
             of data taken in 2011 by the ATLAS experiment at a
             center-of-mass energy √s=7 TeV, no evidence of such heavy
             vector-like quarks is observed above the expected Standard
             Model background. Limits on the heavy vector-like quark
             production cross section times branching ratio as a function
             of mass mQ are obtained. For a coupling κqQ=v/mQ, where v
             is the Higgs vacuum expectation value, 95% C.L. lower limits
             on the mass of a vector-like quark are set at 900 GeV and
             760 GeV from CC and NC processes, respectively. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.03.082},
   Key = {fds309166}
}

@article{fds309167,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
             LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini,
             I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement,
             B},
   Title = {Search for events with large missing transverse momentum,
             jets, and at least two tau leptons in 7 TeV proton-proton
             collision data with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {714},
   Number = {2-5},
   Pages = {180-196},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.055},
   Abstract = {A search for events with large missing transverse momentum,
             jets, and at least two tau leptons has been performed using
             2 fb-1 of proton-proton collision data at s=7 TeV recorded
             with the ATLAS detector at the Large Hadron Collider. No
             excess above the Standard Model background expectation is
             observed and a 95% CL upper limit on the visible cross
             section for new phenomena is set, where the visible cross
             section is defined by the product of cross section,
             branching fraction, detector acceptance and event selection
             efficiency. A 95% CL lower limit of 32 TeV is set on the
             gauge-mediated supersymmetry breaking (GMSB) scale Λ
             independent of tanβ. These limits provide the most
             stringent tests to date in a large part of the considered
             parameter space. © 2012.},
   Doi = {10.1016/j.physletb.2012.06.055},
   Key = {fds309167}
}

@article{fds309170,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
             MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
             LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini,
             I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
             SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
             W},
   Title = {Search for the Standard Model Higgs boson in the decay
             channel H→ZZ(*)→4ℓ with 4.8 fb-1
             of pp collision data at √s=7 TeV with ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {3},
   Pages = {383-402},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.005},
   Abstract = {This Letter presents a search for the Standard Model Higgs
             boson in the decay channel H→ZZ(*)→ℓ+ℓ-ℓ'+ℓ'-,
             where ℓ, ℓ'=e or μ, using proton-proton collisions at
             √s=7 TeV recorded with the ATLAS detector and
             corresponding to an integrated luminosity of 4.8 fb-1. The
             four-lepton invariant mass distribution is compared with
             Standard Model background expectations to derive upper
             limits on the cross section of a Standard Model Higgs boson
             with a mass between 110 GeV and 600 GeV. The mass ranges
             134-156 GeV, 182-233 GeV, 256-265 GeV and 268-415 GeV are
             excluded at the 95% confidence level. The largest upward
             deviations from the background-only hypothesis are observed
             for Higgs boson masses of 125 GeV, 244 GeV and 500 GeV with
             local significances of 2.1, 2.2 and 2.1 standard deviations,
             respectively. Once the look-elsewhere effect is considered,
             none of these excesses are significant. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.03.005},
   Key = {fds309170}
}

@article{fds309175,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
             SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC},
   Title = {Measurement of the WW cross section in √s=7 TeV pp
             collisions with the ATLAS detector and limits on anomalous
             gauge couplings},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {4-5},
   Pages = {289-308},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.05.003},
   Abstract = {This Letter reports a measurement of the WW production cross
             section in √s=7 TeV pp collisions using data corresponding
             to an integrated luminosity of 1.02 fb-1 collected with the
             ATLAS detector. Using leptonic decays of oppositely charged
             W bosons, the total measured cross section is
             σ(pp→WW)=54.4±4.0(stat.)±3.9(syst.)±2.0(lumi.) pb,
             consistent with the Standard Model prediction of
             σ(pp→WW)=44.4±2.8 pb. Limits on anomalous electroweak
             triple-gauge couplings are extracted from a fit to the
             transverse-momentum distribution of the leading charged
             lepton in the event. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.05.003},
   Key = {fds309175}
}

@article{fds309179,
   Author = {ATLAS Collaboration},
   Title = {A search for ttbar resonances with the ATLAS detector in
             2.05 fb^-1 of proton-proton collisions at sqrt(s) = 7
             TeV},
   Journal = {The European Physical Journal C},
   Volume = {72},
   Number = {7},
   Pages = {2083},
   Year = {2012},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2083-1},
   Abstract = {A search for top quark pair resonances in final states
             containing at least one electron or muon has been performed
             with the ATLAS experiment at the CERN Large Hadron Collider.
             The search uses a data sample corresponding to an integrated
             luminosity of 2.05 fb<sup>-1</sup>, which was recorded in
             2011 at a proton-proton centre-of-mass energy of 7 TeV. No
             evidence for a resonance is found and limits are set on the
             production cross-section times branching ratio to [Formula:
             see text] for narrow and wide resonances. For narrow
             <i>Z</i>' bosons, the observed 95 % Bayesian credibility
             level limits range from 9.3 pb to 0.95 pb for masses in
             the range of <i>m</i><sub><i>Z</i>'</sub>=500 GeV to
             <i>m</i><sub><i>Z</i>'</sub>=1300 GeV. The corresponding
             excluded mass region for a leptophobic topcolour <i>Z</i>'
             boson (Kaluza-Klein gluon excitation in the Randall-Sundrum
             model) is <i>m</i><sub><i>Z</i>'</sub><880 GeV ([Formula:
             see text]).},
   Doi = {10.1140/epjc/s10052-012-2083-1},
   Key = {fds309179}
}

@article{fds309180,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J and Colombo,
             T},
   Title = {Search for a Standard Model Higgs boson in the mass range
             200-600GeV in the H→ZZ→ℓ+ℓ-qq̄ decay channel with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {70-88},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.020},
   Abstract = {A search for a heavy Standard Model Higgs boson decaying via
             H→ZZ→ℓ+ℓ-qq̄, where ℓ=e or μ, is presented. The
             search uses a data set of pp collisions at s=7TeV,
             corresponding to an integrated luminosity of 4.7fb-1
             collected in 2011 by the ATLAS detector at the CERN LHC. No
             significant excess of events above the estimated background
             is found. Upper limits at 95% confidence level on the
             production cross section of a Higgs boson with a mass in the
             range between 200 and 600GeV are derived. A Standard Model
             Higgs boson with a mass in the range 300GeV≤mH≤322GeV or
             353GeV≤mH≤410GeV is excluded at 95% CL. The
             corresponding expected exclusion range is
             351GeV≤mH≤404GeV at 95% CL. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.09.020},
   Key = {fds309180}
}

@article{fds309181,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J},
   Title = {Search for the Standard Model Higgs boson in the
             H→WW({star operator})→ℓνℓν decay mode
             with 4.7 fb-1 of ATLAS data at √s=7
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {62-81},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.010},
   Abstract = {A search for the Standard Model Higgs boson in the
             H→WW({star operator})→ℓνℓν (ℓ=e, μ) decay mode
             is presented. The search is performed using proton-proton
             collision data corresponding to an integrated luminosity of
             4.7 fb-1 at a centre-of-mass energy of 7 TeV collected
             during 2011 with the ATLAS detector at the Large Hadron
             Collider. No significant excess of events over the expected
             background is observed. An upper bound is placed on the
             Higgs boson production cross section as a function of its
             mass. A Standard Model Higgs boson with mass in the range
             between 133 GeV and 261 GeV is excluded at 95% confidence
             level, while the expected exclusion range is from 127 GeV to
             233 GeV. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.08.010},
   Key = {fds309181}
}

@article{fds309182,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J},
   Title = {Measurement of the b-hadron production cross section using
             decays to D *+μ -X final states in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {Nuclear Physics B},
   Volume = {864},
   Number = {3},
   Pages = {341-381},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2012.07.009},
   Abstract = {The b-hadron production cross section is measured with the
             ATLAS detector in pp collisions at s=7TeV, using 3.3pb -1 of
             integrated luminosity, collected during the 2010 LHC run.
             The b-hadrons are selected by partially reconstructing D
             z.ast;+μ -X final states. Differential cross sections are
             measured as functions of the transverse momentum and
             pseudorapidity. The measured production cross section for a
             b-hadron with p T&gt;9GeV and |n|&lt;2.5 is
             32.7±0.8(stat.)-6.8+4.5(syst.)μb, higher than the
             next-to-leading-order QCD predictions but consistent within
             the experimental and theoretical uncertainties. ©
             2012.},
   Doi = {10.1016/j.nuclphysb.2012.07.009},
   Key = {fds309182}
}

@article{fds309185,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós,
             G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi,
             F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
             J and Colombo, T},
   Title = {Measurement of the top quark pair cross section with ATLAS
             in pp collisions at s=7 TeV using final states with an
             electron or a muon and a hadronically decaying τ
             lepton},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {89-108},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.032},
   Abstract = {A measurement of the cross section of top quark pair
             production in proton-proton collisions recorded with the
             ATLAS detector at the Large Hadron Collider at a
             centre-of-mass energy of 7 TeV is reported. The data sample
             used corresponds to an integrated luminosity of 2.05 fb-1.
             Events with an isolated electron or muon and a τ lepton
             decaying hadronically are used. In addition, a large missing
             transverse momentum and two or more energetic jets are
             required. At least one of the jets must be identified as
             originating from a b quark. The measured cross section,
             σtt-=186±13(stat.)±20(syst.)±7(lumi.) pb, is in good
             agreement with the Standard Model prediction. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.09.032},
   Key = {fds309185}
}

@article{fds309186,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós,
             G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber,
             T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom,
             PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni,
             G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
             M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
             T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
             J and Colon, G and Muiño, PC and Coniavitis, E and Conidi,
             MC},
   Title = {Search for scalar top quark pair production in natural gauge
             mediated supersymmetry models with the ATLAS detector in pp
             collisions at s=7TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {715},
   Number = {1-3},
   Pages = {44-60},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.07.010},
   Abstract = {The results of a search for pair production of the lighter
             scalar partners of top quarks (t~1) in 2.05 fb-1 of pp
             collisions at s=7 TeV using the ATLAS experiment at the LHC
             are reported. Scalar top quarks are searched for in events
             with two same flavour opposite-sign leptons (e, μ) with
             invariant mass consistent with the Z boson mass, large
             missing transverse momentum and jets in the final state. At
             least one of the jets is identified as originating from a
             b-quark. No excess over Standard Model expectations is
             found. The results are interpreted in the framework of
             R-parity conserving, gauge mediated Supersymmetry breaking
             'natural' scenarios, where the neutralino (χ~10) is the
             next-to-lightest supersymmetric particle. Scalar top quark
             masses up to 310 GeV are excluded for 115GeV&lt;mχ~10&lt;230GeV
             at 95% confidence level, reaching an exclusion of
             mt~1&lt;330GeV for mχ~10=190GeV. Scalar top quark masses
             below 240 GeV are excluded for all values of mχ~10&gt;mZ.
             © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.07.010},
   Key = {fds309186}
}

@article{fds309191,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau,
             M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio,
             EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
             JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
             J and Colon, G and Muiño, PC and Coniavitis, E and Conidi, MC and Consonni, SM and Consorti, V},
   Title = {Search for the decay Bs0→μ+μ-
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {713},
   Number = {4-5},
   Pages = {387-407},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.013},
   Abstract = {A blind analysis searching for the decay Bs0→μ+μ- has
             been performed using proton-proton collisions at a
             centre-of-mass energy of 7 TeV recorded with the ATLAS
             detector at the LHC. With an integrated luminosity of 2.4
             fb-1 no excess of events over the background expectation is
             found and an upper limit is set on the branching fraction
             BR(Bs0→μ+μ-)&lt;2.2(1.9)×10-8 at 95% (90%) confidence
             level. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.06.013},
   Key = {fds309191}
}

@article{fds309220,
   Author = {Cho, BK and Lee, JH and Crellin, CC and Olson, KL and Hilden, DL and Kim,
             MK and Kim, PS and Heo, I and Oh, SH and Nam, IS},
   Title = {Selective catalytic reduction of NO x by diesel
             fuel: Plasma-assisted HC/SCR system},
   Journal = {Catalysis Today},
   Volume = {191},
   Number = {1},
   Pages = {20-24},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.cattod.2012.03.044},
   Abstract = {A new NO x reduction system has been developed which can
             reduce NO x emissions in diesel engine exhaust using
             oxygenated hydrocarbons (OHCs) generated from diesel fuel
             reforming as the primary reductants. The system consists of
             a sidestream hyperplasma reactor, a diesel fuel reformer and
             a dual-bed catalytic reactor. A unique feature of this
             system is a diesel fuel reformer that can produce highly
             reactive OHCs for NO x reduction. Steady-state performance
             as well as simulated FTP performance of this system for NO x
             reduction was evaluated in a sidestream connected to the
             main exhaust stream of a 4.9L, 6-cylinder Isuzu diesel
             engine dynamometer system. A dual-bed (BaY + CuY) catalyst
             yielded a mode-average FTP NO x conversion of 61% when the
             catalyst volume was 3.6 times the engine displacement. NO x
             reduction efficiency of the reformed diesel fuel was
             compared with that of an ethanol-dodecane mixture, E-diesel
             and NH 3 in laboratory microreactor experiments and engine
             dynamometer tests. © 2012 Elsevier B.V.},
   Doi = {10.1016/j.cattod.2012.03.044},
   Key = {fds309220}
}

@article{fds309223,
   Author = {Kang, SB and Han, SJ and Nam, SB and Nam, IS and Cho, BK and Kim, CH and Oh,
             SH},
   Title = {Activity function describing the effect of Pd loading on the
             catalytic performance of modern commercial
             TWC},
   Journal = {Chemical Engineering Journal},
   Volume = {207-208},
   Pages = {117-121},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.cej.2012.06.003},
   Abstract = {A catalyst activity function for the commercial Pd-based
             three-way catalyst (TWC) has been developed to describe the
             effect of Pd loading ranging from 20 to 240g/ft. 3 on its
             catalytic performance. Derived from the alteration of the Pd
             metallic surface area (MSA) due to the variation of the Pd
             loading, the activity function reasonably well captures the
             nonlinear dependence of catalytic activity on the Pd loading
             of the Pd-based TWCs. The overall reaction kinetics for the
             commercial TWC obtained from the combination of the catalyst
             activity function developed and the primary reaction
             kinetics over the 4k Pd240 reference catalyst has proven to
             be capable of well predicting the effect of Pd loading on
             the catalytic performance of the Pd-based TWCs. The accuracy
             of model predictions has been excellent for the oxidation of
             CO, C 3H 6 and H 2, while leaving some room for improvement
             in the model accuracy for the reduction of NO and related
             byproducts. © 2012 Elsevier B.V.},
   Doi = {10.1016/j.cej.2012.06.003},
   Key = {fds309223}
}

@article{fds309224,
   Author = {Kim, MK and Kim, PS and Cho, BK and Nam, IS and Oh, SH},
   Title = {Enhanced NOx reduction and byproduct removal by (HC +
             OHC)/SCR over multifunctional dual-bed monolith
             catalyst},
   Journal = {Catalysis Today},
   Volume = {184},
   Number = {1},
   Pages = {95-106},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.cattod.2011.11.010},
   Abstract = {Selective catalytic reduction of NOx over Ag/Al 2O 3
             monolith catalyst was investigated using a dodecane-ethanol
             mixture as the reductant, with special attention to the
             increased formation of harmful byproducts due to ethanol in
             the reductant hydrocarbon mixture. To compensate the
             tradeoff effect of ethanol by fully utilizing and/or
             efficiently removing these hazardous byproducts formed over
             the Ag/Al 2O 3 catalyst, additional catalysts were employed
             in a double-layer or dual-bed configuration, or a
             combination thereof. Among the catalysts tested, a
             trimetallic dual-bed monolith catalyst was identified as the
             best combination for the maximum NOx-to-N 2 conversion
             (∼90% above 300°C) with a minimum formation of harmful
             byproducts, through multifunctional cooperative catalytic
             processes on Ag/Al 2O 3, CuCoY and Pd/Al 2O 3. Reaction
             intermediates formed on catalyst surfaces were investigated
             using an in situ DRIFT for both single-bed and dual-bed
             catalysts, thereby identifying three important roles of
             Ag/Al 2O 3 in the front bed. The relative importance of
             various deNOx processes occurring on CuCoY in the rear bed
             strongly depends on the reaction temperature and the gas
             space velocity over the dual-bed catalyst system. Reaction
             pathways of (HC + OHC)/SCR in the dual-bed catalyst system
             were discussed in light of the maximum NOx conversion with a
             minimum consumption of OHC. © 2011 Elsevier
             B.V.},
   Doi = {10.1016/j.cattod.2011.11.010},
   Key = {fds309224}
}

@article{fds309225,
   Author = {Kim, MK and Kim, PS and Kwon, HJ and Nam, IS and Cho, BK and Oh,
             SH},
   Title = {Simulation of OHC/SCR process over Ag/Al2O3
             catalyst for removing NOx from diesel engine},
   Journal = {Chemical Engineering Journal},
   Volume = {209},
   Pages = {280-292},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.cej.2012.08.002},
   Abstract = {A reaction kinetic model was developed to describe the
             selective catalytic reduction of NOx over Ag/Al2O3 with
             ethanol as the reductant, which was then used for numerical
             simulation and optimization of the deNOx performance of the
             oxygenated hydrocarbon (OHC)/SCR process. Results of
             numerical simulation of the one-dimensional
             pseudo-homogeneous reactor model have demonstrated the
             capability of the model, describing reasonably well the
             general trends of the experimental data such as the
             conversions of NO and C2H5OH as well as the formation of N2,
             NH3, CO, CH3CHO, CO2, N2O and HOCH2CH2NH2 during the
             ethanol/SCR process with respect to the reaction
             temperature, the reactor space velocity and the C1/NOx feed
             ratio covered in the present study. After successful
             validation of the reactor model, the axial concentration
             profiles within the reactor were used for the optimal design
             of a dual-bed catalyst system to enhance the deNOx
             performance of the ethanol/SCR by best utilizing the
             reaction intermediates in the rear bed following the
             Ag/Al2O3 in the front bed. The methodology developed in this
             work may provide useful guidance on the design of an OHC/SCR
             system using ethanol as the reductant, including, but not
             limited to, the diesel engine operating on E-diesel fuel. ©
             2012 Elsevier B.V.},
   Doi = {10.1016/j.cej.2012.08.002},
   Key = {fds309225}
}

@article{fds309226,
   Author = {Wiebenga, MH and Kim, CH and Schmieg, SJ and Oh, SH and Brown, DB and Kim,
             DH and Lee, JH and Peden, CHF},
   Title = {Deactivation mechanisms of Pt/Pd-based diesel oxidation
             catalysts},
   Journal = {Catalysis Today},
   Volume = {184},
   Number = {1},
   Pages = {197-204},
   Publisher = {Elsevier BV},
   Year = {2012},
   url = {http://dx.doi.org/10.1016/j.cattod.2011.11.014},
   Abstract = {Currently precious metal-based diesel oxidation catalysts
             (DOC) containing platinum (Pt) and palladium (Pd) are most
             commonly used for the oxidation of hydrocarbon and NO in
             diesel exhaust hydrocarbon oxidation. The present work has
             been carried out to investigate the deactivation mechanisms
             of the DOC from its real-world vehicle operation by coupling
             its catalytic activity measurements with surface
             characterization including X-ray diffraction, transmission
             electron microscopy, and X-ray photoelectron spectroscopy. A
             production Pt-Pd DOC was obtained after being aged on a
             vehicle driven for 135,000 miles in order to study its
             deactivation behavior. The performance of the vehicle-aged
             part was correlated with that of the simulated hydrothermal
             lab aged sample assuming that Pt-Pd sintering plays a major
             role in irreversible catalyst deactivation. In addition to
             the hydrothermal sintering, the deterioration of hydrocarbon
             and NO oxidation performance was caused by surface
             poisoning. The role of the various aging factors in
             determining long-term performance in mobile applications
             will be discussed. © 2011 Elsevier B.V.},
   Doi = {10.1016/j.cattod.2011.11.014},
   Key = {fds309226}
}

@article{fds313369,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
             A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
             R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini,
             I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and El Moursli and RC and Chernyatin,
             V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Time-dependent angular analysis of the decay
             Bs0J/ψφ and
             extraction of ΔΓs and the
             CP-violating weak phase φs by
             ATLAS},
   Journal = {JOURNAL OF HIGH ENERGY PHYSICS},
   Volume = {2012},
   Number = {12},
   Year = {2012},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)072},
   Abstract = {A measurement of B0s → J /ψφ decay parameters, including
             the CP -violating weak phase φ s and the decay width
             difference ΔΓ s is reported, using 4.9 fb-1 of integrated
             luminosity collected in 2011 by the ATLAS detector from LHC
             pp collisions at a centre-of-mass energy √s = 7 TeV. The
             mean decay width Γ s and the transversity amplitudes |A
             0(0)|2 and |A arap;(0)|2 are also measured. The values
             reported for these parameters are: φs = 0.22 ± 0.41 (stat)
             ± 0.10 (syst) rad} ΔΓ s = 0.053 ± 0.021 (stat) ± 0.010
             (sast) ps-1 Γ s = 0.677 ± 0.007 (stat) ± 0.004 (sast)
             ps-1 |A0(0)|2 = 0.528 ± 0.006 (stat) ± 0.009 (sast)
             |A0(0)|2 = 0.220 ± 0.008 (stat) ± 0.007 (sast) where the
             values quoted for φ s and ΔΓ s correspond to the solution
             compatible with the external measurements to which the
             strong phase δ ⊥ is constrained and where ΔΓ s is
             constrained to be positive. The fraction of S-wave KK or f 0
             contamination through the decays B0s→ J /ψK +
             K-}}\left({{f-0}} \right)}} \right.} is measured as well and
             is found to be consistent with zero. Results for φ s and
             ΔΓ s are also presented as 68%, 90% and 95% likelihood
             contours, which show agreement with Standard Model
             expectations.[Figure not available: see fulltext.] © 2012
             CERN for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP12(2012)072},
   Key = {fds313369}
}

@article{fds212665,
   Author = {CDF collaboration},
   Title = {Production of Λ0, Ξ, and Ω Hyperons in ppbar
             Collisions at Ecm = 1.96 TeV},
   Journal = {Phy. Rev. D 86, 012002 (2012)},
   Year = {2012},
   Key = {fds212665}
}

@article{fds314433,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Forward-backward correlations and charged-particle azimuthal
             distributions in pp interactions using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP07(2012)019},
   Abstract = {Using inelastic proton-proton interactions at √s =900 GeV
             and 7TeV, recorded by the ATLAS detector at the LHC,
             measurements have been made of the correlations between
             forward and backward charged-particle multiplicities and,
             for the first time, between forward and backward
             charged-particle summed transverse momentum. In addition,
             jet-like structure in the events is studied by means of
             azimuthal distributions of charged particles relative to the
             charged particle with highest transverse momentum in a
             selected kinematic region of the event. The results are
             compared with predictions from tunes of the PYTHIA and
             HERWIG++ Monte Carlo generators, which in most cases are
             found to provide a reasonable description of the
             data.},
   Doi = {10.1007/JHEP07(2012)019},
   Key = {fds314433}
}

@article{fds309051,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
             N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Search for anomalous production of prompt like-sign lepton
             pairs at √s =7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)007},
   Abstract = {An inclusive search for anomalous production of two prompt,
             isolated leptons with the same electric charge is presented.
             The search is performed in a data sample corresponding to
             4.7 fb-1 of integrated luminosity collected in 2011 at √s
             =7 TeV with the ATLAS detector at the LHC. Pairs of leptons
             (e± e±, e± μ ±, and μ ± μ ±) with large transverse
             momentum are selected, and the dilepton invariant mass
             distribution is examined for any deviation from the Standard
             Model expectation. No excess is found, and upper limits on
             the production cross section of like-sign lepton pairs from
             physics processes beyond the Standard Model are placed as a
             function of the dilepton invariant mass within a fiducial
             region close to the experimental selection criteria. The 95%
             confidence level upper limits on the cross section of
             anomalous e± e ±, e± μ ±, or μ ± μ ± production
             range between 1.7 fb and 64 fb depending on the dilepton
             mass and flavour combination. © 2012 Cern for the benefit
             of the ATLAS collaboration.},
   Doi = {10.1007/JHEP12(2012)007},
   Key = {fds309051}
}

@article{fds309053,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {ATLAS search for a heavy gauge boson decaying to a charged
             lepton and a neutrino in pp collisions at √s =7
             TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2241-5},
   Abstract = {The ATLAS detector at the LHC is used to search for
             high-mass states, such as heavy charged gauge bosons (Wʹ),
             decaying to a charged lepton (electron or muon) and a
             neutrino. Results are presented based on the analysis of pp
             collisions at a center-of-mass energy of 7 TeV corresponding
             to an integrated luminosity of 4.7 fb−1. No excess beyond
             Standard Model expectations is observed. AWʹ with
             Sequential Standard Model couplings is excluded at the 95%
             credibility level for masses up to 2.55 TeV. Excited chiral
             bosons (W*) with equivalent coupling strength are excluded
             for masses up to 2.42 TeV.},
   Doi = {10.1140/epjc/s10052-012-2241-5},
   Key = {fds309053}
}

@article{fds309055,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for pair production of massive particles decaying
             into three quarks with the ATLAS detector in √s = 7 TeV pp
             collisions at the LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)086},
   Abstract = {A search is conducted for hadronic three-body decays of a
             new massive coloured particle in √s = 7 TeV pp collisions
             at the LHC using an integrated luminosity of 4.6 fb-1
             collected by the ATLAS detector. Supersymmetric gluino pair
             production in the context of a model with R-parity violation
             is used as a benchmark scenario. The analysis is divided
             into two search channels, each optimised separately for
             their sensitivity to high-mass and low-mass gluino
             production. The first search channel uses a stringent
             selection on the transverse momentum of the six leading jets
             and is performed as a counting experiment. The second search
             channel focuses on low-mass gluinos produced with a large
             boost. Large-radius jets are selected and the invariant mass
             of each of the two leading jets is used as a discriminant
             between the signal and the background. The results are found
             to be consistent with Standard Model expectations and limits
             are set on the allowed gluino mass.[Figure not available:
             see fulltext.] © 2012 Cern for the benefit of the ATLAS
             collaboration.},
   Doi = {10.1007/JHEP12(2012)086},
   Key = {fds309055}
}

@article{fds309066,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurements of the pseudorapidity dependence of the total
             transverse energy in proton-proton collisions at √s = 7TeV
             with ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {11},
   Pages = {1-53},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2012)033},
   Abstract = {This paper describes measurements of the sum of the
             transverse energy of particles as a function of particle
             pseudorapidity, η, in proton-proton collisions at a
             centre-of-mass energy, √s = 7TeV using the ATLAS detector
             at the Large Hadron Collider. The measurements are performed
             in the region |η| < 4.8 for two event classes: those
             requiring the presence of particles with a low transverse
             momentum and those requiring particles with a significant
             transverse momentum. In the second dataset measurements are
             made in the region transverse to the hard scatter. The
             distributions are compared to the predictions of various
             Monte Carlo event generators, which generally tend to
             underestimate the amount of transverse energy at high |η|.
             Copyright CERN.},
   Doi = {10.1007/JHEP11(2012)033},
   Key = {fds309066}
}

@article{fds309108,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benjamin,
             DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan,
             JG and Coggeshall, J and Cogneras, E and Cojocaru,
             CD},
   Title = {Measurement of the ZZ production cross section and limits on
             anomalous neutral triple gauge couplings in proton-proton
             collisions at sqrt[s] = 7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {4},
   Pages = {041804},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.108.041804},
   Abstract = {A measurement of the ZZ production cross section in
             proton-proton collisions at sqrt[s] = 7 TeV using data
             corresponding to an integrated luminosity of 1.02 fb(-1)
             recorded by the ATLAS experiment at the LHC is presented.
             Twelve events containing two Z boson candidates decaying to
             electrons and/or muons are observed, with an expected
             background of 0.3 ± 0.3(stat)(-0.3)(+0.4)(syst) events. The
             cross section measured in a phase-space region with good
             detector acceptance and for dilepton masses within the range
             66 to 116 GeV is σ(ZZ → ℓ+ ℓ- ℓ+ ℓ-)(fid) =
             19.4(-5.2)(+6.3)(stat)(-0.7)(+0.9)(syst) ± 0.7(lumi) fb.
             The resulting total cross section for on-shell ZZ
             production, σ(ZZ)(tot) = 8.5(-2.3)(+2.7)(stat)(-0.3)(+0.4)(syst)
             ± 0.3(lumi) pb, is consistent with the standard model
             expectation of 6.5(-0.2)(+0.3) pb calculated at the
             next-to-leading order in QCD. Limits on anomalous neutral
             triple gauge boson couplings are derived.},
   Doi = {10.1103/physrevlett.108.041804},
   Key = {fds309108}
}

@article{fds309109,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
             G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
             C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
             K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall,
             J},
   Title = {Search for new phenomena in tt events with large missing
             transverse momentum in proton-proton collisions at sqrt[s] =
             7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {4},
   Pages = {041805},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.108.041805},
   Abstract = {A search for new phenomena in tt events with large missing
             transverse momentum in proton-proton collisions at a
             center-of-mass energy of 7 TeV is presented. The measurement
             is based on 1.04 fb(-1) of data collected with the ATLAS
             detector at the LHC. Contributions to this final state may
             arise from a number of standard model extensions. The
             results are interpreted in terms of a model where new
             top-quark partners are pair produced and each decay to an
             on-shell top (or antitop) quark and a long-lived undetected
             neutral particle. The data are found to be consistent with
             standard model expectations. A limit at 95% confidence level
             is set excluding a cross section times branching ratio of
             1.1 pb for a top-partner mass of 420 GeV and a neutral
             particle mass less than 10 GeV. In a model of exotic fourth
             generation quarks, top-partner masses are excluded up to 420
             GeV and neutral particle masses up to 140
             GeV.},
   Doi = {10.1103/physrevlett.108.041805},
   Key = {fds309109}
}

@article{fds309110,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
             M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
             A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
             K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Ray, J and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro,
             A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri,
             F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari,
             M and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton,
             O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov,
             A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
   Title = {Search for a Higgs boson in the diphoton final state in pp
             collisions at sqrt[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {1},
   Pages = {011801},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.108.011801},
   Abstract = {A search for a narrow Higgs boson resonance in the diphoton
             mass spectrum is presented based on data corresponding to
             7.0  fb{-1} of integrated luminosity from pp collisions
             at sqrt[s]=1.96  TeV collected by the CDF experiment. No
             evidence of such a resonance is observed, and upper limits
             are set on the cross section times branching ratio of the
             resonant state as a function of Higgs boson mass. The limits
             are interpreted in the context of the standard model and one
             fermiophobic benchmark model where the data exclude
             fermiophobic Higgs bosons with masses below
             114  GeV/c{2} at a 95% Bayesian credibility
             level.},
   Doi = {10.1103/physrevlett.108.011801},
   Key = {fds309110}
}

@article{fds309111,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, J and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Performance of missing transverse momentum reconstruction in
             proton-proton collisions at√s = 7 TeV with
             atlas},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {1},
   Pages = {1-35},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1844-6},
   Abstract = {The measurement of missing transverse momentum in the ATLAS
             detector, described in this paper, makes use of the full
             event reconstruction and a calibration based on
             reconstructed physics objects. The performance of the
             missing transverse momentum reconstruction is evaluated
             using data collected in pp collisions at a centre-of-mass
             energy of 7 TeV in 2010. Minimum bias events and events with
             jets of hadrons are used from data samples corresponding to
             an integrated luminosity of about 0.3 nb1 and 600 nb1
             respectively, together with events containing a Z boson
             decaying to two leptons (electrons or muons) or aW boson
             decaying to a lepton (electron or muon) and a neutrino, from
             a data sample corresponding to an integrated luminosity of
             about 36 pb1. An estimate of the systematic uncertainty on
             the missing transverse momentum scale is presented. © CERN
             for the benefit of the ATLAS collaboration
             2011.},
   Doi = {10.1140/epjc/s10052-011-1844-6},
   Key = {fds309111}
}

@article{fds309112,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Performance of the ATLAS trigger system in
             2010},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {1},
   Pages = {1-61},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-011-1849-1},
   Abstract = {Proton-proton collisions at √S = 7 TeV and heavy ion
             collisions at √SNN = 2.76 TeV were produced by the LHC and
             recorded using the ATLAS experiment's trigger system in
             2010. The LHC is designed with a maximum bunch crossing rate
             of 40 MHz and the ATLAS trigger system is designed to record
             approximately 200 of these per second. The trigger system
             selects events by rapidly identifying signatures of muon,
             electron, photon, tau lepton, jet, and B meson candidates,
             as well as using global event signatures, such as missing
             transverse energy. An overview of the ATLAS trigger system,
             the evolution of the system during 2010 and the performance
             of the trigger system components and selections based on the
             2010 collision data are shown. A brief outline of plans for
             the trigger system in 2011 is presented.},
   Doi = {10.1140/epjc/s10052-011-1849-1},
   Key = {fds309112}
}

@article{fds309115,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {A search for tt̄ resonances in lepton+jets events with
             highly boosted top quarks collected in pp collisions at √s
             = 7TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2012)041},
   Abstract = {A search for resonant production of high-mass top-quark
             pairs is performed on 2.05 fb-1 of proton-proton collisions
             at √s = 7 TeV collected in 2011 with the ATLAS experiment
             at the Large Hadron Collider. This analysis of the
             lepton+jets final state is specifically designed for the
             particular topology that arises from the decay of highly
             boosted top quarks. The observed tt̄ invariant mass
             spectrum is found to be compatible with the Standard Model
             prediction and 95% credibility level upper limits are
             derived on the tt̄ production rate through new massive
             states. An upper limit of 0.7 pb is set on the production
             cross section times branching fraction of a narrow 1 TeV
             resonance. A Kaluza-Klein gluon with a mass smaller than 1.5
             TeV is excluded.},
   Doi = {10.1007/JHEP09(2012)041},
   Key = {fds309115}
}

@article{fds309116,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
             R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
             F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Measurement of the top quark mass with the template method
             in the [Formula: see text] channel using ATLAS
             data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {6},
   Pages = {2046},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2046-6},
   Abstract = {The top quark mass has been measured using the template
             method in the [Formula: see text] channel based on data
             recorded in 2011 with the ATLAS detector at the LHC. The
             data were taken at a proton-proton centre-of-mass energy of
             [Formula: see text] and correspond to an integrated
             luminosity of 1.04 fb<sup>-1</sup>. The analyses in the
             <i>e</i>+jets and <i>μ</i>+jets decay channels yield
             consistent results. The top quark mass is measured to be
             <i>m</i><sub>top</sub>=174.5±0.6<sub>stat</sub>±2.3<sub>syst</sub>
             GeV.},
   Doi = {10.1140/epjc/s10052-012-2046-6},
   Key = {fds309116}
}

@article{fds309117,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C},
   Title = {Search for heavy neutrinos and right-handed W bosons
             in events with two leptons and jets in pp collisions
             at [Formula: see text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {7},
   Pages = {2056},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2056-4},
   Abstract = {This letter reports on a search for hypothetical heavy
             neutrinos, <i>N</i>, and right-handed gauge bosons,
             <i>W</i><sub>R</sub>, in events with high transverse
             momentum objects which include two reconstructed leptons and
             at least one hadronic jet. The results were obtained from
             data corresponding to an integrated luminosity of
             2.1 fb<sup>-1</sup> collected in proton-proton collisions
             at [Formula: see text] with the ATLAS detector at the CERN
             Large Hadron Collider. No excess above the Standard Model
             background expectation is observed. Excluded mass regions
             for Majorana and Dirac neutrinos are presented using two
             approaches for interactions that violate lepton and
             lepton-flavor numbers. One approach uses an effective
             operator framework, the other approach is guided by the
             Left-Right Symmetric Model. The results described in this
             letter represent the most stringent limits to date on the
             masses of heavy neutrinos and <i>W</i><sub>R</sub> bosons
             obtained in direct searches.},
   Doi = {10.1140/epjc/s10052-012-2056-4},
   Key = {fds309117}
}

@article{fds309123,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati,
             S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
             R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
             F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
             W},
   Title = {Measurement of the charge asymmetry in top quark pair
             production in pp collisions at [Formula: see text]
             using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {6},
   Pages = {2039},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2039-5},
   Abstract = {A measurement of the top-antitop production charge asymmetry
             <i>A</i><sub><i>C</i></sub> is presented using data
             corresponding to an integrated luminosity of 1.04
             fb<sup>-1</sup> of <i>pp</i> collisions at [Formula: see
             text] TeV collected by the ATLAS detector at the LHC.
             Events are selected with a single lepton (electron or muon),
             missing transverse momentum and at least four jets of which
             at least one jet is identified as coming from a
             <i>b</i>-quark. A kinematic fit is used to reconstruct the
             [Formula: see text] event topology. After background
             subtraction, a Bayesian unfolding procedure is performed to
             correct for acceptance and detector effects. The measured
             value of <i>A</i><sub><i>C</i></sub> is [Formula: see text],
             consistent with the prediction from the MC@NLO Monte Carlo
             generator of <i>A</i><sub><i>C</i></sub> =0.006±0.002.
             Measurements of <i>A</i><sub><i>C</i></sub> in two ranges of
             invariant mass of the top-antitop pair are also
             shown.},
   Doi = {10.1140/epjc/s10052-012-2039-5},
   Key = {fds309123}
}

@article{fds309156,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {A study of the material in the ATLAS inner detector using
             secondary hadronic interactions},
   Journal = {Journal of Instrumentation},
   Volume = {7},
   Number = {1},
   Pages = {P01013-P01013},
   Publisher = {IOP Publishing},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/7/01/P01013},
   Abstract = {The ATLAS inner detector is used to reconstruct secondary
             vertices due to hadronic interactions of primary collision
             products, so probing the location and amount of material in
             the inner region of ATLAS. Data collected in 7 TeV pp
             collisions at the LHC, with a minimum bias trigger, are used
             for comparisons with simulated events. The reconstructed
             secondary vertices have spatial resolutions ranging from ∼
             200μm to 1 mm. The overall material description in the
             simulation is validated to within an experimental
             uncertainty of about 7%. This will lead to a better
             understanding of the reconstruction of various objects such
             as tracks, leptons, jets, and missing transverse momentum.
             © 2012 CERN.},
   Doi = {10.1088/1748-0221/7/01/P01013},
   Key = {fds309156}
}

@article{fds309163,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
             M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams,
             DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Aleppo, M and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim,
             A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders,
             CF and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, M and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos Santos Pedrosa and F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, GA and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov,
             VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, G and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
             M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat,
             P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertolucci,
             F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Biesiada, J and Biglietti,
             M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blocker, C and Blocki, J and Blondel, A and Blum,
             W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Bona, M and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Booth, P and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni,
             S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik,
             J and Braem, A and Brambilla, E and Branchini, P and Brandt, A and Brandt,
             G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Brett, ND and Bright-Thomas, PG and Britton, D and Brochu, FM and Brock,
             I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
             G and Brooks, WK and Brown, G and Brubaker, E and Bruckman de Renstrom,
             PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni,
             G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan,
             NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark,
             D and Buis, EJ and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Caballero, J and Cabrera Urbán and S and Caccia, M and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camard,
             A and Camarri, P and Cameron, D and Cammin, J and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carpentieri, C and Carrillo Montoya and GD and Carter, AA and Carter,
             JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso,
             C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavallari, A and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Cazzato, A and Ceradini, F and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, L and Chen, S and Chen, X and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {Search for lepton flavour violation in the 
             continuum with the ATLAS detector in [Formula: see
             text]pp collisions at the LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {6},
   Pages = {2040},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2040-z},
   Abstract = {This paper presents a search for the <i>t</i>-channel
             exchange of an <i>R</i>-parity violating scalar top quark
             ([Formula: see text]) in the <i>e</i><sup>±</sup><i>μ</i><sup>∓</sup>
             continuum using 2.1 fb<sup>-1</sup> of data collected by
             the ATLAS detector in [Formula: see text]<i>pp</i>
             collisions at the Large Hadron Collider. Data are found to
             be consistent with the expectation from the Standard Model
             backgrounds. Limits on <i>R</i>-parity-violating couplings
             at 95 % C.L. are calculated as a function of the scalar top
             mass ([Formula: see text]). The upper limits on the
             production cross section for <i>pp</i>→<i>eμX</i>,
             through the <i>t</i>-channel exchange of a scalar top quark,
             ranges from 170 fb for [Formula: see text] to 30 fb for
             [Formula: see text].},
   Doi = {10.1140/epjc/s10052-012-2040-z},
   Key = {fds309163}
}

@article{fds309164,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi,
             E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
   Title = {Measurement of [Formula: see text] production with a veto on
             additional central jet activity in pp collisions at
             [Formula: see text] TeV using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {6},
   Pages = {2043},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2043-9},
   Abstract = {A measurement of the jet activity in [Formula: see text]
             events produced in proton-proton collisions at a
             centre-of-mass energy of 7 TeV is presented, using
             2.05 fb<sup>-1</sup> of integrated luminosity collected by
             the ATLAS detector at the Large Hadron Collider. The
             [Formula: see text] events are selected in the dilepton
             decay channel with two identified <i>b</i>-jets from the top
             quark decays. Events are vetoed if they contain an
             additional jet with transverse momentum above a threshold in
             a central rapidity interval. The fraction of events
             surviving the jet veto is presented as a function of this
             threshold for four different central rapidity interval
             definitions. An alternate measurement is also performed, in
             which events are vetoed if the scalar transverse momentum
             sum of the additional jets in each rapidity interval is
             above a threshold. In both measurements, the data are
             corrected for detector effects and compared to the
             theoretical models implemented in MC@NLO, Powheg, Alpgen and
             Sherpa. The experimental uncertainties are often smaller
             than the spread of theoretical predictions, allowing
             deviations between data and theory to be observed in some
             regions of phase space.},
   Doi = {10.1140/epjc/s10052-012-2043-9},
   Key = {fds309164}
}

@article{fds309165,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi,
             E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W},
   Title = {Measurement of τ polarization in
             Wτν decays with the ATLAS detector in
             pp collisions at [Formula: see text].},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {72},
   Number = {7},
   Pages = {2062},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2062-6},
   Abstract = {In this paper, a measurement of <i>τ</i> polarization in
             <i>W</i>→<i>τν</i> decays is presented. It is measured
             from the energies of the decay products in hadronic
             <i>τ</i> decays with a single final state charged particle.
             The data, corresponding to an integrated luminosity of
             24 pb<sup>-1</sup>, were collected by the ATLAS experiment
             at the Large Hadron Collider in 2010. The measured value of
             the <i>τ</i> polarization is [Formula: see text], in
             agreement with the Standard Model prediction, and is
             consistent with a physically allowed 95 % CL
             interval [-1,-0.91]. Measurements of <i>τ</i> polarization
             have not previously been made at hadron colliders.},
   Doi = {10.1140/epjc/s10052-012-2062-6},
   Key = {fds309165}
}

@article{fds309178,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A},
   Title = {Measurement of the W boson polarization in top quark decays
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2012)088},
   Abstract = {This paper presents measurements of the polarization ofW
             bosons in top quark decays, derived from tt̄ events with
             missing transverse momentum, one charged lepton and at least
             four jets, or two charged leptons and at least two jets.
             Data from pp collisions at a centre-of-mass energy of 7 TeV
             were collected with the ATLAS experiment at the LHC and
             correspond to an integrated luminosity of 1.04 fb-1. The
             measured fractions of longitudinally, left- and right-handed
             polarization are F0 = 0.67 ± 0.07, FL = 0.32 ± 0.04 and FR
             = 0.01 ± 0.05, in agreement with the Standard Model
             predictions. As the polarization of the W bosons in top
             quark decays is sensitive to the Wtb vertex Lorentz
             structure and couplings, the measurements were used to set
             limits on anomalous contributions to the Wtb couplings. ©
             CERN.},
   Doi = {10.1007/JHEP06(2012)088},
   Key = {fds309178}
}

@article{fds309183,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin J-F., and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G},
   Title = {Search for the Standard Model Higgs boson in the H →
             τ+τ- decay mode in √s = 7TeV pp
             collisions with ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP09(2012)070},
   Abstract = {A search for the Standard Model Higgs boson decaying into a
             pair of τ leptons is reported. The analysis is based on a
             data sample of proton-proton collisions collected by the
             ATLAS experiment at the LHC and corresponding to an
             integrated luminosity of 4.7fb-1. No significant excess over
             the expected background is observed in the Higgs boson mass
             range of 100-150 GeV. The observed (expected) upper limits
             on the cross section times the branching ratio for H →
             τ+τ- are found to be between 2.9 (3.4) and 11.7 (8.2)
             times the Standard Model prediction for this mass
             range.},
   Doi = {10.1007/JHEP09(2012)070},
   Key = {fds309183}
}

@article{fds309187,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A},
   Title = {Search for a fermiophobic Higgs boson in the diphoton decay
             channel with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {9},
   Pages = {1-18},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2157-0},
   Abstract = {A search for a fermiophobic Higgs boson using diphoton
             events produced in proton-proton collisions at a
             centre-of-mass energy of √s = 7 TeV is performed using
             data corresponding to an integrated luminosity of 4.9
             fb−1collected by the ATLAS experiment at the Large Hadron
             Collider. A specific benchmark model is considered where all
             the fermion couplings to the Higgs boson are set to zero and
             the bosonic couplings are kept at the Standard Model values
             (fermiophobic Higgs model). The largest excess with respect
             to the background-only hypothesis is found at 125.5 GeV,
             with a local significance of 2.9 standard deviations, which
             reduces to 1.6 standard deviations when taking into account
             the look-elsewhere effect. The data exclude the fermiophobic
             Higgs model in the ranges 110.0–118.0 GeV and
             119.5–121.0 GeV at 95 % confidence level.},
   Doi = {10.1140/epjc/s10052-012-2157-0},
   Key = {fds309187}
}

@article{fds309204,
   Author = {Kotwal, AV and Collaboration, CDF},
   Title = {Search for new phenomena in events with two Z bosons and
             missing transverse momentum in ppbar collisions at
             sqrt(s)=1.96 TeV},
   Journal = {Phys. Rev. D},
   Volume = {85},
   Number = {1},
   Pages = {011104(R)},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.011104},
   Abstract = {We present a search for new phenomena in events with two
             reconstructed Z bosons and large missing transverse
             momentum, sensitive to processes pp̄→X 2X 2→ZZX 1X 1,
             where X 2 is an unstable particle decaying as X 2→ ZX 1
             and X 1 is undetected. The particles X 1 and X 2 may be,
             among other possibilities, fourth-generation neutrinos or
             supersymmetric particles. We study the final state in which
             one Z boson decays to two charged leptons and the second
             decays hadronically. In data corresponding to an integrated
             luminosity of 4.2fb -1 from proton-antiproton collisions
             recorded by the CDF II detector at the Tevatron, with
             center-of-mass energy of 1.96 TeV, we find agreement between
             data and standard-model backgrounds. We calculate 95%
             confidence level upper limits on the cross section of the
             process pp̄→X 2X 2→ZZX 1X 1 ranging from 50 fb to 1 pb,
             depending on the masses of X 1 and X 2. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.85.011104},
   Key = {fds309204}
}

@article{fds309221,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Search for decays of stopped, long-lived particles from 7
             TeV pp collisions with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {4},
   Pages = {1-21},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1965-6},
   Abstract = {New metastable massive particles with electric and colour
             charge are features of many theories beyond the Standard
             Model. A search is performed for long-lived gluino-based
             R-hadrons with the ATLAS detector at the LHC using a data
             sample corresponding to an integrated luminosity of 31
             pb−1. We search for evidence of particles that have come
             to rest in the ATLAS detector and decay at some later time
             during the periods in the LHC bunch structure without
             proton–proton collisions. No significant deviations from
             the expected backgrounds are observed, and a cross-section
             limit is set. It can be interpreted as excluding
             gluino-based R-hadrons with masses less than 341 GeV at the
             95 % C.L., for lifetimes from 10−5to 103seconds and a
             neutralino mass of 100 GeV.},
   Doi = {10.1140/epjc/s10052-012-1965-6},
   Key = {fds309221}
}

@article{fds310556,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of inclusive two-particle angular correlations
             in pp collisions with the atlas detector at the
             LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP05(2012)157},
   Abstract = {We present a measurement of two-particle angular
             correlations in protonproton collisions at √a = 900 GeV
             and 7TeV. The collision events were collected during 2009
             and 2010 with the ATLAS detector at the Large Hadron
             Collider using a single-arm minimum bias trigger.
             Correlations are measured for charged particles produced in
             the kinematic range of transverse momentum pT > 100MeV and
             pseudorapidity |n| < 2.5. A complex structure in
             pseudorapidity and azimuth is observed at both collision
             energies. Results are compared to pythia 8 and herwig++ as
             well as to the AMBT2B, DW and Perugia 2011 tunes of pythia
             6. The data are not satisfactorily described by any of these
             models.},
   Doi = {10.1007/JHEP05(2012)157},
   Key = {fds310556}
}

@article{fds310553,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abou
             Zeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amor’Os, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Measurement of the azimuthal anisotropy for charged particle
             production in √SNN = 2.76 TeV lead-lead
             collisions with the ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {86},
   Number = {1},
   Pages = {014907-1-014907-41},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevC.86.014907},
   Abstract = {Differential measurements of charged particle azimuthal
             anisotropy are presented for lead-lead collisions at √sNN
             = 2.76 TeV with the ATLAS detector at the LHC, based on an
             integrated luminosity of approximately 8 μb− 1. This
             anisotropy is characterized via a Fourier expansion of the
             distribution of charged particles in azimuthal angle
             relative to the reaction plane, with the coefficients vn
             denoting the magnitude of the anisotropy. Significant
             v2–v6 values are obtained as a function of transverse
             momentum (0.5 < pT < 20 GeV), pseudorapidity (|η| < 2.5),
             and centrality using an event plane method. The vn values
             for n ≥ 3 are found to vary weakly with both η and
             centrality, and their pT dependencies are found to follow an
             approximate scaling relation, v1/nn (pT) ∝ v1/22 (pT),
             except in the top 5% most central collisions. A Fourier
             analysis of the charged particle pair distribution in
             relative azimuthal angle (Δϕ = ϕa − ϕb) is performed
             to extract the coefficients vn, n = (cos nΔϕ). For pairs
             of charged particles with a large pseudorapidity gap (|Δη
             = ηa − ηb| > 2) and one particle with pT < 3 GeV, the
             v2,2–v6,6 values are found to factorize as vn, n(paT, pbT)
             ≈ vn(paT)vn(pbT) in central and midcentral events. Such
             factorization suggests that these values of v2,2–v6,6 are
             primarily attributable to the response of the created matter
             to the fluctuations in the geometry of the initial state. A
             detailed study shows that the v1,1(paT, pbT) data are
             consistent with the combined contributions from a
             rapidity-even v1 and global momentum conservation.A
             two-component fit is used to extract the v1 contribution.
             The extracted v1 isobserved to cross zero at pT ≈ 1.0 GeV,
             reaches a maximum at 4–5 GeV with a value comparable to
             that for v3, and decreases at higher pT.},
   Doi = {10.1103/PhysRevC.86.014907},
   Key = {fds310553}
}

@article{fds325846,
   Author = {Abelev, B and Adam, J and Adamova, D and Marshall Adare and A and Aggarwal,
             M and Aglieri Rinella and G and Gabor Agocs and A and Agostinelli, A and Aguilar Salazar and S and Ahammed, Z and Ahmad, A and Ahmad, N and Ahn, SA and Un Ahn and S and Akindinov, A and Aleksandrov, D and Alessandro, B and Molina, JRA and Alici, A and Alkin, A and Avina, EJA and Alme, J and Alt,
             T and Altini, V and Altinpinar, S and Altsybeev, I and Andrei, C and Andronic, A and Anguelov, V and Anielski, J and Anson, CD and Anticic,
             T and Antinori, F and Antonioli, P and Aphecetche, LB and Appelshauser,
             H and Arbor, N and Arcelli, S and Arend, A and Armesto, N and Arnaldi, R and Aronsson, TR and Arsene, IC and Arslandok, M and Asryan, A and Augustinus, A and Averbeck, RP and Awes, T and Aysto, JH and Azmi, MD and Bach, MJ and Badala, A and Baek, YW and Bailhache, RM and Bala, R and Ferroli, RB and Baldisseri, A and Baldit, A and Dos Santos Pedrosa,
             FB and Ban, J and Baral, RC and Barbera, R and Barile, F and Barnafoldi,
             GG and Barnby, LS and Barret, V and Bartke, JG and Basile, M and Bastid, N and Basu, S and Bathen, B and Batigne, G and Batyunya, B and Baumann, CH and Bearden, IG and Beck, H and Behera, NK and Belikov, I and Bellini, F and Bellwied, R and Belmont-Moreno, E and Bencedi, G and Beole, S and Berceanu, I and Bercuci, A and Berdnikov, Y and Berenyi, D and Bergognon, AAE and Berzano, D and Betev, L and Bhasin, A and Bhati, AK and Bhom, J and Bianchi, L and Bianchi, N and Bianchin, C and Bielcik, J and Bielcikova, J and Bilandzic, A},
   Title = {Measurement of prompt J/ψand beauty hadron production cross
             sections at mid-rapidity in pp collisions at √s = 7
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2012)065},
   Abstract = {The ALICE experiment at the LHC has studied J/ψ production
             at midrapidity in pp collisions at √s = 7TeV through its
             electron pair decay on a data sample corresponding to an
             integrated luminosity Lint = 5.6 nb-1. The fraction of J/ψ
             from the decay of long-lived beauty hadrons was determined
             for J/ψ candidates with transverse momentum pt > 1.3GeV/c
             and rapidity |y| < 0.9. The cross section for prompt J/ψ
             mesons, i.e. directly produced J/ψ and prompt decays of
             heavier charmonium states such as the ψ(2S) and c
             resonances, is σprompt J/ψ (pt > 1.3 GeV/c, |y| < 0.9) =
             8.3+0.8 (stat.)±} 1.1 (syst.) +1.5 -1.4 (syst. pol.) μb.
             The cross section for the production of b-hadrons decaying
             to J/ψ with pt > 1.3GeV/c and |y| < 0.9 is σJ/ψ←hB (pt
             > 1.3 GeV/c, |y| < 0.9) = 1.46±} 0.38 (stat.) +0.26 -0.32
             (syst.) μb. The results are compared to QCD model
             predictions. The shape of the pt and y distributions of
             b-quarks predicted by perturbative QCD model calculations
             are used to extrapolate the measured cross section to derive
             the bb pair total cross section and dσ/dy at mid-rapidity.
             © SISSA 2012.},
   Doi = {10.1007/JHEP11(2012)065},
   Key = {fds325846}
}

@article{fds309145,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the W→τντ cross section in pp
             collisions at s=7 TeV with the ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {706},
   Number = {4-5},
   Pages = {276-294},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.057},
   Abstract = {The cross section for the production of W bosons with
             subsequent decay W→τντ is measured with the ATLAS
             detector at the LHC. The analysis is based on a data sample
             that was recorded in 2010 at a proton-proton center-of-mass
             energy of s=7 TeV and corresponds to an integrated
             luminosity of 34 pb-1. The cross section is measured in a
             region of high detector acceptance and then extrapolated to
             the full phase space. The product of the total W production
             cross section and the W→τντ branching ratio is measured
             to be σW→τντtot=11.1±0.3(stat)±1.7(syst)±0.4(lumi)
             nb. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.057},
   Key = {fds309145}
}

@article{fds309146,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the cross-section for b-jets produced in
             association with a Z boson at s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {706},
   Number = {4-5},
   Pages = {295-313},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.059},
   Abstract = {A measurement is presented of the inclusive cross-section
             for b-jet production in association with a Z boson in pp
             collisions at a centre-of-mass energy of s=7 TeV. The
             analysis uses the data sample collected by the ATLAS
             experiment in 2010, corresponding to an integrated
             luminosity of approximately 36 pb-1. The event selection
             requires a Z boson decaying into high pT electrons or muons,
             and at least one b-jet, identified by its displaced vertex,
             with transverse momentum pT>25 GeV and rapidity |y|<2.1.
             After subtraction of background processes, the yield is
             extracted from the vertex mass distribution of the candidate
             b-jets. The ratio of this cross-section to the inclusive Z
             cross-section (the average number of b-jets per Z event) is
             also measured. Both results are found to be in good
             agreement with perturbative QCD predictions at
             next-to-leading order. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.059},
   Key = {fds309146}
}

@article{fds309139,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Ks0 and Λ production in pp interactions at √s=0.9 and 7
             TeV measured with the ATLAS detector at the
             LHC},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012001},
   Abstract = {The production of KS0 and Λ hadrons is studied in pp
             collision data at √s=0.9 and 7 TeV collected with the
             ATLAS detector at the LHC using a minimum-bias trigger. The
             observed distributions of transverse momentum, rapidity, and
             multiplicity are corrected to hadron level in a
             model-independent way within well-defined phase-space
             regions. The distribution of the production ratio of Λ̄ to
             Λ baryons is also measured. The results are compared with
             various Monte Carlo simulation models. Although most of
             these models agree with data to within 15% in the KS0
             distributions, substantial disagreements are found in the Λ
             distributions of transverse momentum. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.85.012001},
   Key = {fds309139}
}

@article{fds309201,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca almenar, C and Cuevas, J and Culbertson, R and Dagenhart, D},
   Title = {Search for WZ+ZZ production with missing transverse
             energy+jets with b enhancement at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012002},
   Abstract = {Diboson production (WW+WZ+ZZ) has been observed at the
             Tevatron in hadronic decay modes dominated by the WW
             process. This paper describes the measurement of the cross
             section of WZ and ZZ events in final states with large E T
             and using b-jet identification as a tool to suppress WW
             contributions. Because of the limited energy resolution, we
             cannot distinguish between partially hadronic decays of WZ
             and ZZ, and we measure the sum of these processes. The
             number of signal events is extracted using a simultaneous
             fit to the invariant mass distribution of the two jets for
             events with two b-jet candidates and events with fewer than
             two b-jet candidates. We measure a cross section
             σ(pp̄→WZ,ZZ)=5.8-3.0+3.6pb, in agreement with the
             standard model. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.012002},
   Key = {fds309201}
}

@article{fds309138,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the isolated diphoton cross section in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012003},
   Abstract = {The ATLAS experiment has measured the production cross
             section of events with two isolated photons in the final
             state, in proton-proton collisions at √s=7TeV. The full
             data set acquired in 2010 is used, corresponding to an
             integrated luminosity of 37pb -1. The background, consisting
             of hadronic jets and isolated electrons, is estimated with
             fully data-driven techniques and subtracted. The
             differential cross sections, as functions of the di-photon
             mass (m γγ), total transverse momentum (p T,γγ), and
             azimuthal separation (Δφ γγ), are presented and compared
             to the predictions of next-to-leading-order QCD. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.85.012003},
   Key = {fds309138}
}

@article{fds309142,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Search for a heavy Standard Model Higgs boson in the channel
             H→ZZ→ℓ+-qq̄ using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {1},
   Pages = {27-45},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.11.056},
   Abstract = {A search for a heavy Standard Model Higgs boson decaying via
             H→ZZ→ℓ+ℓ-qq̄, where ℓ=e, μ, is presented. The
             search is performed using a data set of pp collisions at
             √s=7 TeV, corresponding to an integrated luminosity of
             1.04 fb-1 collected in 2011 by the ATLAS detector at the
             CERN LHC collider. No significant excess of events above the
             estimated background is found. Upper limits at 95%
             confidence level on the production cross section (relative
             to that expected from the Standard Model) of a Higgs boson
             with a mass in the range between 200 and 600 GeV are
             derived. Within this mass range, there is at present
             insufficient sensitivity to exclude a Standard Model Higgs
             boson. For a Higgs boson with a mass of 360 GeV, where the
             sensitivity is maximal, the observed and expected cross
             section upper limits are factors of 1.7 and 2.7,
             respectively, larger than the Standard Model prediction. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.11.056},
   Key = {fds309142}
}

@article{fds309137,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for supersymmetry in final states with jets, missing
             transverse momentum and one isolated lepton in √s=7TeV pp
             collisions using 1fb -1 of ATLAS
             data},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012006},
   Abstract = {We present an update of a search for supersymmetry in final
             states containing jets, missing transverse momentum, and one
             isolated electron or muon, using 1.04fb -1 of proton-proton
             collision data at √s=7TeV recorded by the ATLAS experiment
             at the LHC in the first half of 2011. The analysis is
             carried out in four distinct signal regions with either
             three or four jets and variations on the (missing)
             transverse momentum cuts, resulting in optimized limits for
             various supersymmetry models. No excess above the standard
             model background expectation is observed. Limits are set on
             the visible cross section of new physics within the
             kinematic requirements of the search. The results are
             interpreted as limits on the parameters of the minimal
             supergravity framework, limits on cross sections of
             simplified models with specific squark and gluino decay
             modes, and limits on parameters of a model with bilinear
             R-parity violation. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.012006},
   Key = {fds309137}
}

@article{fds309152,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the transverse momentum distribution of W
             bosons in pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012005},
   Abstract = {This paper describes a measurement of the W boson transverse
             momentum distribution using ATLAS pp collision data from the
             2010 run of the LHC at √s=7TeV, corresponding to an
             integrated luminosity of about 31pb -1. Events form both
             W→eν and W→μν are used, and the transverse momentum
             of the W candidates is measured through the energy
             deposition in the calorimeter from the recoil of the W. The
             resulting distributions are unfolded to obtain the
             normalized differential cross sections as a function of the
             W boson transverse momentum. We present results for
             pTW<300GeV in the electron and muon channels as well as for
             their combination, and compare the combined results to the
             predictions of perturbative QCD and a selection of event
             generators. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.012005},
   Key = {fds309152}
}

@article{fds309199,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
   Title = {Search for heavy metastable particles decaying to jet pairs
             in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012007},
   Abstract = {A search is performed for heavy metastable particles that
             decay into jet pairs with a macroscopic lifetime (cτ∼1cm)
             in pp̄ collisions at √s=1.96TeV using data from the CDF
             II detector at Fermilab corresponding to an integrated
             luminosity of 3.2fb-1. To estimate the standard model
             background, a data-driven approach is used.
             Probability-density functions are constructed to model
             secondary vertices from known processes. No statistically
             significant excess is observed above the background. Limits
             on the production cross section in a hidden valley benchmark
             phenomenology are set for various Higgs boson masses as well
             as metastable particle masses and lifetimes. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.012007},
   Key = {fds309199}
}

@article{fds313366,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Search for high-mass resonances decaying into ZZ in pp̄
             collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   ISSN = {1550-7998},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000299925100002&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We search for high-mass resonances decaying into Z boson
             pairs using data corresponding to 6fb -1 collected by the
             CDF experiment in pp̄ collisions at √s=1.96TeV. The
             search is performed in three distinct final states: ZZ→
             +-+-, ZZ→ +-νν, and ZZ→ +-jj. For a Randall-Sundrum
             graviton G *, the 95% CL upper limits on the production
             cross section times branching ratio to ZZ, σ(pp̄→G
             *→ZZ), vary between 0.26 pb and 0.045 pb in the mass range
             300<M G*<1000GeV/c2. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.012008},
   Key = {fds313366}
}

@article{fds309208,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Measurement of CP-violating asymmetries in D0→π
             +π - and D0→K +K
             - decays at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.012009},
   Abstract = {We report on a measurement of CP-violating asymmetries (A
             CP) in the Cabibbo-suppressed D0→π +π - and D0→K +K -
             decays reconstructed in a data sample corresponding to 5.9fb
             -1 of integrated luminosity collected by the upgraded
             Collider Detector at Fermilab. We use the strong decay D
             *+→D0π + to identify the flavor of the charmed meson at
             production and exploit CP-conserving strong cc̄ pair
             production in pp̄ collisions. High-statistics samples of
             Cabibbo-favored D0→K -π + decays with and without a D *±
             tag are used to correct for instrumental effects and
             significantly reduce systematic uncertainties. We measure A
             CP(D0→π +π -)=(+0.22±0.24(stat) ±0.11(syst))% and A
             CP(D0→K +K -)=(-0.24±0.22(stat)±0.09(syst))%, in
             agreement with CP conservation. These are the most precise
             determinations from a single experiment to date. Under the
             assumption of negligible direct CP violation in D0→π +π
             - and D0→K +K - decays, the results provide an upper limit
             to the CP-violating asymmetry in D0 mixing,
             |ACPind(D0)|<0.13% at the 90% confidence level. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.012009},
   Key = {fds309208}
}

@article{fds309150,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the cross section for the production of a W
             boson in association with b-jets in pp collisions at √s =
             7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {418-437},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.046},
   Abstract = {A measurement is presented of the cross section for the
             production of a W boson with one or two jets, of which at
             least one must be a b-jet, in pp collisions at √s = 7 TeV.
             Production via top decay is not included in the signal
             definition. The measurement is based on 35 pb-1 of data
             collected with the ATLAS detector at the LHC. The W + b-jet
             cross section is defined for jets reconstructed with the
             antikt clustering algorithm with transverse momentum above
             25 GeV and rapidity within ±2.1. The b-jets are identified
             by reconstructing secondary vertices. The fiducial cross
             section is measured both for the electron and muon decay
             channel of the W boson and is found to be 10.2 ± 1.9(stat)
             ± 2.6(syst) pb for one lepton flavour. The results are
             compared with next-to-leading order QCD calculations, which
             predict a cross section smaller than, though consistent
             with, the measured value.},
   Doi = {10.1016/j.physletb.2011.12.046},
   Key = {fds309150}
}

@article{fds309162,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
             KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S},
   Title = {Measurement of the pseudorapidity and transverse momentum
             dependence of the elliptic flow of charged particles in
             lead-lead collisions at sNN=2.76 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {3-4},
   Pages = {330-348},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.056},
   Abstract = {This Letter describes the measurement of elliptic flow of
             charged particles in lead-lead collisions at sNN=2.76 TeV
             using the ATLAS detector at the Large Hadron Collider (LHC).
             The results are based on an integrated luminosity of
             approximately 7 μb-1. Elliptic flow is measured over a wide
             region in pseudorapidity, |η|<2.5, and over a broad range
             in transverse momentum, 0.5<pT<20 GeV. The elliptic flow
             parameter v2 is obtained by correlating individual tracks
             with the event plane measured using energy deposited in the
             forward calorimeters. As a function of transverse momentum,
             v2(pT) reaches a maximum at pT of about 3 GeV, then
             decreases and becomes weakly dependent on pT above 7-8 GeV.
             Over the measured pseudorapidity region, v2 is found to be
             only weakly dependent on η, with less variation than
             observed at lower beam energies. The results are discussed
             in the context of previous measurements at lower collision
             energies, as well as recent results from the LHC. © 2011
             CERN.},
   Doi = {10.1016/j.physletb.2011.12.056},
   Key = {fds309162}
}

@article{fds309209,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
             Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
             L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
             R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
             A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
             E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
             W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
             HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
             T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
             J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
             R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
             T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
             L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
             M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
             A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
             M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
             RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
             D and Weinberger, M and Wenzel, H and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
   Title = {Measurements of the angular distributions in the decays
             B→K(*)μ(+)μ(-) at CDF.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {8},
   Pages = {081807},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.108.081807},
   Abstract = {We report an indirect search for nonstandard model physics
             using the flavor-changing neutral current decays
             B→K(*)μ(+)μ(-). We reconstruct the decays and measure
             their angular distributions, as a function of
             q(2)=M(μμ)(2)c(2), where M(μμ) is the dimuon mass, in
             pp¯ collisions at √s=1.96 TeV using a data sample
             corresponding to an integrated luminosity of 6.8 fb(-1). The
             transverse polarization asymmetry A(T)(2) and the
             time-reversal-odd charge-and-parity asymmetry A(im) are
             measured for the first time, together with the K*
             longitudinal polarization fraction F(L) and the muon
             forward-backward asymmetry A(FB) for the decays
             B(0)→K(*0)μ(+)μ(-) and B(+)→K(*+)μ(+)μ(-). The
             B→K*μ(+)μ(-) forward-backward asymmetry in the most
             sensitive kinematic regime, 1≤q(2)<6 GeV(2)/c(2), is
             measured to be A(FB)=0.29(-0.23)(+0.20)(stat)±0.07(syst),
             the most precise result to date. No deviations from the
             standard model predictions are observed.},
   Doi = {10.1103/physrevlett.108.081807},
   Key = {fds309209}
}

@article{fds309200,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
   Title = {Search for the rare radiative decay W→πγ in pp̄
             collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032001},
   Abstract = {We present a search for the rare radiative decay W ±→ π
             ±γ using data corresponding to an integrated luminosity of
             4.3fb -1 of proton-antiproton collisions at a center-of-mass
             energy of 1.96 TeV collected by the CDF experiment at
             Fermilab. As no statistically significant signal is
             observed, we set a 95%-confidence-level upper limit on the
             relative branching fraction Γ(W ±→π ±γ)/Γ(W ±→e
             ±ν) at 6.4×10 -5, a factor of 10 improvement over the
             previous limit. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.032001},
   Key = {fds309200}
}

@article{fds309143,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the top quark pair production cross section
             in pp collisions at √s=7TeV in dilepton final states with
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {459-477},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.055},
   Abstract = {A measurement of the production cross section of top quark
             pairs (tt̄) in proton-proton collisions at a center-of-mass
             energy of 7 TeV recorded with the ATLAS detector at the
             Large Hadron Collider is reported. Candidate events are
             selected in the dilepton topology with large missing
             transverse energy and at least two jets. Using a data sample
             corresponding to an integrated luminosity of 35pb-1, a tt̄
             production cross section σtt̄=177±20(stat.)±14(syst.)±7(lum.)pb
             is measured for an assumed top quark mass of mt=172.5GeV. A
             second measurement requiring at least one jet identified as
             coming from a b quark yields a comparable result,
             demonstrating that the dilepton final states are consistent
             with being accompanied by b-quark jets. These measurements
             are in good agreement with Standard Model predictions. ©
             2011 CERN.},
   Doi = {10.1016/j.physletb.2011.12.055},
   Key = {fds309143}
}

@article{fds309153,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for displaced vertices arising from decays of new
             heavy particles in 7 TeV pp collisions at
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {478-496},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.057},
   Abstract = {We present the results of a search for new, heavy particles
             that decay at a significant distance from their production
             point into a final state containing charged hadrons in
             association with a high-momentum muon. The search is
             conducted in a pp-collision data sample with a
             center-of-mass energy of 7 TeV and an integrated luminosity
             of 33 pb-1 collected in 2010 by the ATLAS detector operating
             at the Large Hadron Collider. Production of such particles
             is expected in various scenarios of physics beyond the
             standard model. We observe no signal and place limits on the
             production cross-section of supersymmetric particles in an
             R-parity-violating scenario as a function of the neutralino
             lifetime. Limits are presented for different squark and
             neutralino masses, enabling extension of the limits to a
             variety of other models. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.12.057},
   Key = {fds309153}
}

@article{fds309157,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurements of the electron and muon inclusive
             cross-sections in proton-proton collisions at √s=7TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {707},
   Number = {5},
   Pages = {438-458},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2011.12.054},
   Abstract = {This Letter presents measurements of the differential
             cross-sections for inclusive electron and muon production in
             proton-proton collisions at a centre-of-mass energy of
             s=7TeV, using data collected by the ATLAS detector at the
             LHC. The muon cross-section is measured as a function of pT
             in the range 4<pT<100GeV and within pseudorapidity |η|<2.5.
             In addition the electron and muon cross-sections are
             measured in the range 7<pT<26GeV and within |η|<2.0,
             excluding 1.37<|η|<1.52. Integrated luminosities of 1.3pb-1
             and 1.4pb-1 are used for the electron and muon measurements,
             respectively. After subtraction of the W/Z/γ* contribution,
             the differential cross-sections are found to be in good
             agreement with theoretical predictions for heavy-flavour
             production obtained from Fixed Order NLO calculations with
             NLL high-pT resummation, and to be sensitive to the effects
             of NLL resummation. © 2011 CERN.},
   Doi = {10.1016/j.physletb.2011.12.054},
   Key = {fds309157}
}

@article{fds309148,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for new physics in the dijet mass distribution using
             1 fb -1 of pp collision data at √s=7 TeV
             collected by the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {708},
   Number = {1-2},
   Pages = {37-54},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.01.035},
   Abstract = {Invariant mass distributions of jet pairs (dijets) produced
             in LHC proton-proton collisions at a centre-of-mass energy
             s=7 TeV have been studied using a data set corresponding to
             an integrated luminosity of 1.0 fb -1 recorded in 2011 by
             ATLAS. Dijet masses up to ~4 TeV are observed in the data,
             and no evidence of resonance production over background is
             found. Limits are set at 95% C.L. for several new physics
             hypotheses: excited quarks are excluded for masses below 299
             TeV, axigluons are excluded for masses below 3.32 TeV, and
             colour octet scalar resonances are excluded for masses below
             1.92 TeV. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.01.035},
   Key = {fds309148}
}

@article{fds309132,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for anomalous production of prompt like-sign muon
             pairs and constraints on physics beyond the standard model
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032004},
   Abstract = {An inclusive search for anomalous production of two prompt,
             isolated muons with the same electric charge is presented.
             The search is performed in a data sample corresponding to
             1.6fb-1 of integrated luminosity collected in 2011 at
             √s=7TeV with the ATLAS detector at the LHC. Muon pairs are
             selected by requiring two isolated muons of the same
             electric charge with p T>20GeV and |η|<2.5. Minimal
             requirements are placed on the rest of the event activity.
             The distribution of the invariant mass of the muon pair
             m(μμ) is found to agree well with the background
             expectation. Upper limits on the cross section for anomalous
             production of two muons with the same electric charge are
             placed as a function of m(μμ) within a fiducial region
             defined by the event selection. The fiducial cross-section
             limit constrains the like-sign top-quark pair-production
             cross section to be below 3.7pb at 95% confidence level. The
             data are also analyzed to search for a narrow like-sign
             dimuon resonance as predicted for e.g. doubly charged Higgs
             bosons (H ±). Assuming pair production of H± bosons and a
             branching ratio to muons of 100% (33%), this analysis
             excludes masses below 355 (244)GeV and 251 (209)GeV for H±
             bosons coupling to left-handed and right-handed fermions,
             respectively. © 2012 CERN. Published by the American
             Physical Society under the terms of the uri
             xlink:href=http://creativecommons.org/licenses/by/3.0/Creative
             Commons Attribution 3.0 License. Further distribution of
             this work must maintain attribution to the author(s) and the
             published article's title, journal citation, and DOI. ©
             2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.032004},
   Key = {fds309132}
}

@article{fds309210,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
             M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D},
   Title = {Search for Higgs bosons produced in association with b
             quarks},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032005},
   Abstract = {We present a search for neutral Higgs bosons decaying into
             bb̄, produced in association with b quarks in pp̄
             collisions. This process could be observable in
             supersymmetric models with high values of tanβ. The event
             sample corresponds to 2.6fb -1 of integrated luminosity
             collected with the CDF II detector at the Fermilab Tevatron
             collider. We search for an enhancement in the mass of the
             two leading jets in events with three jets identified as
             coming from b quarks using a displaced vertex algorithm. A
             data-driven procedure is used to estimate the dijet mass
             spectrum of the nonresonant multijet background. The
             contributions of backgrounds and a possible Higgs boson
             signal are determined by a two-dimensional fit of the data,
             using the dijet mass together with an additional variable
             which is sensitive to the flavor composition of the three
             tagged jets. We set mass-dependent limits on
             σ(pp̄→)×B(→bb̄) which are applicable for a narrow
             scalar particle produced in association with b quarks. We
             also set limits on tanβ in supersymmetric Higgs models
             including the effects of the Higgs boson width. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.032005},
   Key = {fds309210}
}

@article{fds309147,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {A measurement of the ratio of the W and Z cross sections
             with exactly one associated jet in pp collisions at s=7TeV
             with ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {708},
   Number = {3-5},
   Pages = {221-240},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.01.042},
   Abstract = {The ratio of production cross sections of the W and Z bosons
             with exactly one associated jet is presented as a function
             of jet transverse momentum threshold. The measurement has
             been designed to maximise cancellation of experimental and
             theoretical uncertainties, and is reported both within a
             particle-level kinematic range corresponding to the detector
             acceptance and as a total cross-section ratio. Results are
             obtained with the ATLAS detector at the LHC in pp collisions
             at a centre-of-mass energy of 7 TeV using an integrated
             luminosity of 33 pb-1. The results are compared with
             perturbative leading-order, leading-log, and
             next-to-leading-order QCD predictions, and are found to
             agree within experimental and theoretical uncertainties. The
             ratio is measured for events with a single jet with pT>30
             GeV to be 8.73±0.30(stat)±0.40(syst) in the electron
             channel, and 8.49±0.23(stat)±0.33(syst) in the muon
             channel. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.01.042},
   Key = {fds309147}
}

@article{fds309151,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the production cross section for Z/γ* in
             association with jets in pp collisions at √s=7TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.032009},
   Abstract = {Results are presented on the production of jets of particles
             in association with a Z/γ* boson, in proton-proton
             collisions at √s=7TeV with the ATLAS detector. The
             analysis includes the full 2010 data set, collected with a
             low rate of multiple proton-proton collisions in the
             accelerator, corresponding to an integrated luminosity of
             36pb-1. Inclusive jet cross sections in Z/γ* events, with
             Z/γ* decaying into electron or muon pairs, are measured for
             jets with transverse momentum pT>30GeV and jet rapidity
             |y|<4.4. The measurements are compared to
             next-to-leading-order perturbative QCD calculations, and to
             predictions from different Monte Carlo generators
             implementing leading-order matrix elements supplemented by
             parton showers. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.032009},
   Key = {fds309151}
}

@article{fds309105,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
             G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Search for the standard model Higgs boson in the diphoton
             decay channel with 4.9 fb(-1) of pp collision data at √s=7
             TeV with ATLAS.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {11},
   Pages = {111803},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.108.111803},
   Abstract = {A search for the standard model Higgs boson is performed in
             the diphoton decay channel. The data used correspond to an
             integrated luminosity of 4.9 fb(-1) collected with the ATLAS
             detector at the Large Hadron Collider in proton-proton
             collisions at a center-of-mass energy of √s=7 TeV. In the
             diphoton mass range 110-150 GeV, the largest excess with
             respect to the background-only hypothesis is observed at
             126.5 GeV, with a local significance of 2.8 standard
             deviations. Taking the look-elsewhere effect into account in
             the range 110-150 GeV, this significance becomes 1.5
             standard deviations. The standard model Higgs boson is
             excluded at 95% confidence level in the mass ranges of
             113-115 GeV and 134.5-136 GeV.},
   Doi = {10.1103/physrevlett.108.111803},
   Key = {fds309105}
}

@article{fds309106,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of ZZ production in leptonic final states at
             sqrt[s] of 1.96 TeV at CDF.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {10},
   Pages = {101801},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.108.101801},
   Abstract = {In this Letter, we present a precise measurement of the
             total ZZ production cross section in pp collisions at
             sqrt[s]=1.96  TeV, using data collected with the CDF II
             detector corresponding to an integrated luminosity of
             approximately 6  fb(-1). The result is obtained by
             combining separate measurements in the four-charged
             (ℓℓℓ' ℓ') and two-charged-lepton and
             two-neutral-lepton (ℓℓνν) decay modes of the Z boson
             pair. The combined measured cross section for pp → ZZ is
             1.64(-0.38)(+0.44)  pb. This is the most precise
             measurement of the ZZ production cross section in 1.96 TeV
             pp collisions to date.},
   Doi = {10.1103/physrevlett.108.101801},
   Key = {fds309106}
}

@article{fds309134,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa,
             HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks,
             KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde,
             M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benitez Garcia and JA and Benjamin, DP and Benoit,
             M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
             JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
             S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
             J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C},
   Title = {Search for the Higgs boson in the H→WW(*)→ℓ(+)νℓ(-)ν
             decay channel in pp collisions at √s=7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {11},
   Pages = {111802},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.108.111802},
   Abstract = {A search for the Higgs boson has been performed in the
             H→WW(*)→ℓ(+)νℓ(-)ν[over ¯] channel (ℓ=e/μ)
             with an integrated luminosity of 2.05 fb(-1) of pp
             collisions at √s=7 TeV collected with the ATLAS detector
             at the Large Hadron Collider. No significant excess of
             events over the expected background is observed and limits
             on the Higgs boson production cross section are derived for
             a Higgs boson mass in the range 110 GeV<m(H)<300 GeV. The
             observations exclude the presence of a standard model Higgs
             boson with a mass 145<m(H)<206 GeV at 95% confidence
             level.},
   Doi = {10.1103/physrevlett.108.111802},
   Key = {fds309134}
}

@article{fds309144,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Electron performance measurements with the ATLAS detector
             using the 2010 LHC proton-proton collision
             data},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {3},
   Pages = {1-46},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1909-1},
   Abstract = {Detailed measurements of the electron performance of the
             ATLAS detector at the LHC are reported, using decays of the
             Z, W and J/ψ particles. Data collected in 2010 at √s = 7
             TeV are used, corresponding to an integrated luminosity of
             almost 40 pb-1. The inter-alignment of the inner detector
             and the electromagnetic calorimeter, the determination of
             the electron energy scale and resolution, and the
             performance in terms of response uniformity and linearity
             are discussed. The electron identification, reconstruction
             and trigger efficiencies, as well as the charge
             misidentification probability, are also presented. © 2012
             CERN for the benefit of the ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-012-1909-1},
   Key = {fds309144}
}

@article{fds309124,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Rapidity gap cross sections measured with the ATLAS detector
             in pp collisions at √s =7 TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {3},
   Pages = {1-31},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1926-0},
   Abstract = {Pseudorapidity gap distributions in proton-proton collisions
             at √s = 7 TeV are studied using a minimum bias data sample
             with an integrated luminosity of 7.1 μb<sup>−1</sup>.
             Cross sections are measured differentially in terms of
             Δη<sup>F</sup>, the larger of the pseudorapidity regions
             extending to the limits of the ATLAS sensitivity, at η =
             ±4.9, in which no final state particles are produced above
             a transverse momentum threshold p<sup>cut</sup><inf>T</inf>.
             The measurements span the region 0 < Δη<sup>F</sup> < 8
             for 200 MeV < p<sup>cut</sup><inf>T</inf> < 800 MeV. At
             small Δη<sup>F</sup>, the data test the reliability of
             hadronisation models in describing rapidity and transverse
             momentum fluctuations in final state particle production.
             The measurements at larger gap sizes are dominated by
             contributions from the single diffractive dissociation
             process (pp →Xp), enhanced by double dissociation (pp →
             XY) where the invariant mass of the lighter of the two
             dissociation systems satisfies M<inf>Y</inf> < 7 GeV. The
             resulting cross section is dσ/dΔη<sup>F</sup> ≈1 mb for
             Δη<sup>F</sup> > 3. The large rapidity gap data are used
             to constrain the value of the Pomeron intercept appropriate
             to triple Regge models of soft diffraction. The cross
             section integrated over all gap sizes is compared with other
             LHC inelastic cross section measurements.},
   Doi = {10.1140/epjc/s10052-012-1926-0},
   Key = {fds309124}
}

@article{fds309128,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov,
             A},
   Title = {Search for first generation scalar leptoquarks in pp
             collisions at s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {3},
   Pages = {158-176},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.004},
   Abstract = {We report a search for first generation scalar leptoquarks
             using 1.03fb-1 of proton-proton collisions data produced by
             the Large Hadron Collider at s=7 TeV and recorded by the
             ATLAS experiment. Leptoquarks are sought via their decay
             into an electron or neutrino and a quark, producing events
             with two oppositely charged electrons and at least two jets,
             or events with an electron, missing transverse momentum and
             at least two jets. Control data samples are used to validate
             background predictions from Monte Carlo simulation. In the
             signal region, the observed event yields are consistent with
             the background expectations. We exclude at 95% confidence
             level the production of first generation scalar leptoquark
             with masses mLQ<660(607) GeV when assuming the branching
             fraction of a leptoquark to a charged lepton is equal to 1.0
             (0.5). © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.004},
   Key = {fds309128}
}

@article{fds309140,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Kesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Measurement of D  meson production in jets
             from pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.052005},
   Abstract = {This paper reports a measurement of D *± meson production
             in jets from proton-proton collisions at a center-of-mass
             energy of √s=7TeV at the CERN Large Hadron Collider. The
             measurement is based on a data sample recorded with the
             ATLAS detector with an integrated luminosity of 0.30pb -1
             for jets with transverse momentum between 25 and 70 GeV in
             the pseudorapidity range |η|<2.5. D *± mesons found in
             jets are fully reconstructed in the decay chain: D *+→D0π
             +, D0→K -π +, and its charge conjugate. The production
             rate is found to be N(D *±)/N(jet)=0.025±0.
             001(stat.)±0.004(syst.) for D *± mesons that carry a
             fraction z of the jet momentum in the range 0.3<z<1. Monte
             Carlo predictions fail to describe the data at small values
             of z, and this is most marked at low jet transverse
             momentum. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.052005},
   Key = {fds309140}
}

@article{fds309154,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Searches for supersymmetry with the ATLAS detector using
             final states with two leptons and missing transverse
             momentum in s=7TeV proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {3},
   Pages = {137-157},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.01.076},
   Abstract = {Results of three searches are presented for the production
             of supersymmetric particles decaying into final states with
             missing transverse momentum and exactly two isolated
             leptons, e or μ. The analysis uses a data sample collected
             during the first half of 2011 that corresponds to a total
             integrated luminosity of 1fb-1 of s=7TeV proton-proton
             collisions recorded with the ATLAS detector at the Large
             Hadron Collider. Opposite-sign and same-sign dilepton events
             are separately studied, with no deviations from the Standard
             Model expectation observed. Additionally, in opposite-sign
             events, a search is made for an excess of same-flavour over
             different-flavour lepton pairs. Effective production cross
             sections in excess of 9.9 fb for opposite-sign events
             containing supersymmetric particles with missing transverse
             momentum greater than 250 GeV are excluded at 95% CL. For
             same-sign events containing supersymmetric particles with
             missing transverse momentum greater than 100 GeV, effective
             production cross sections in excess of 14.8 fb are excluded
             at 95% CL. The latter limit is interpreted in a simplified
             electroweak gaugino production model excluding chargino
             masses up to 200 GeV, under the assumption that slepton
             decay is dominant. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.01.076},
   Key = {fds309154}
}

@article{fds309159,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni, G},
   Title = {Measurement of the W ±Z production cross section
             and limits on anomalous triple gauge couplings in
             proton-proton collisions at s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {4-5},
   Pages = {341-357},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.053},
   Abstract = {This Letter presents a measurement of W ±Z production in
             1.02 fb -1 of pp collision data at s=7 TeV collected by the
             ATLAS experiment in 2011. Doubly leptonic decay events are
             selected with electrons, muons and missing transverse
             momentum in the final state. In total 71 candidates are
             observed, with a background expectation of
             12.1±1.4(stat.)-2.0+4.1(syst.) events. The total cross
             section for W ±Z production for Z/γ * masses within the
             range 66 GeV to 116 GeV is determined to be
             σWZtot=20.5-2.8+3.1(stat.)-1.3+1.4(syst.)-0.8+0.9(lumi.)
             pb, which is consistent with the Standard Model expectation
             of 17.30.8+1.3 pb. Limits on anomalous triple gauge boson
             couplings are extracted. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.053},
   Key = {fds309159}
}

@article{fds309161,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
             G and Arutinov, D},
   Title = {Search for strong gravity signatures in same-sign dimuon
             final states using the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {709},
   Number = {4-5},
   Pages = {322-340},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.049},
   Abstract = {A search for microscopic black holes has been performed in a
             same-sign dimuon final state using 1.3 fb -1 of
             proton-proton collision data collected with the ATLAS
             detector at a centre of mass energy of 7 TeV at the CERN
             Large Hadron Collider. The data are found to be consistent
             with the expectation from the Standard Model and the results
             are used to derive exclusion contours in the context of a
             low scale gravity model. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.049},
   Key = {fds309161}
}

@article{fds309149,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Search for squarks and gluinos using final states with jets
             and missing transverse momentum with the Atlas detector in
             s=7 TeV proton-proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {1},
   Pages = {67-85},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.051},
   Abstract = {A search for squarks and gluinos in events containing jets,
             missing transverse momentum and no electrons or muons is
             presented. The data were recorded in 2011 by the ATLAS
             experiment in s=7 TeV proton-proton collisions at the Large
             Hadron Collider. No excess above the Standard Model
             background expectation is observed in 1.04 fb-1 of data.
             Gluino and squark masses below 700 GeV and 875 GeV
             respectively are excluded at the 95% confidence level in
             simplified models containing only squarks of the first two
             generations, a gluino octet and a massless neutralino. The
             exclusion limit increases to 1075 GeV for squarks and
             gluinos of equal mass. In MSUGRA/CMSSM models with tanβ=10,
             A0=0 and μ>0, squarks and gluinos of equal mass are
             excluded for masses below 950 GeV. These limits extend the
             region of supersymmetric parameter space excluded by
             previous measurements. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.051},
   Key = {fds309149}
}

@article{fds309173,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Combined search for the Standard Model Higgs boson using up
             to 4.9 fb-1 of pp collision data at s=7TeV with
             the ATLAS detector at the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {1},
   Pages = {49-66},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.044},
   Abstract = {A combined search for the Standard Model Higgs boson with
             the ATLAS experiment at the LHC using datasets corresponding
             to integrated luminosities from 1.04 fb-1 to 4.9 fb-1 of pp
             collisions collected at s=7TeV is presented. The Higgs boson
             mass ranges 112.9-115.5 GeV, 131-238 GeV and 251-466 GeV are
             excluded at the 95% confidence level (CL), while the range
             124-519 GeV is expected to be excluded in the absence of a
             signal. An excess of events is observed around mH~126GeV
             with a local significance of 3.5 standard deviations (σ).
             The local significances of H→γγ, H→ZZ(z.ast;)→ℓ+ℓ-ℓ'+ℓ'-
             and H→WW(z.ast;)→ℓ+νℓ'-ν- the three most sensitive
             channels in this mass range, are 2.8σ, 2.1σ and 1.4σ,
             respectively. The global probability for the background to
             produce such a fluctuation anywhere in the explored Higgs
             boson mass range 110-600 GeV is estimated to be ~1.4% or,
             equivalently, 2.2σ. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.02.044},
   Key = {fds309173}
}

@article{fds309102,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Observation of a new χ(b) state in radiative transitions to
             Υ(1S) and Υ(2S) at ATLAS.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {15},
   Pages = {152001},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.108.152001},
   Abstract = {The χ(b)(nP) quarkonium states are produced in
             proton-proton collisions at the Large Hadron Collider at
             sqrt[s] = 7  TeV and recorded by the ATLAS detector.
             Using a data sample corresponding to an integrated
             luminosity of 4.4  fb(-1), these states are
             reconstructed through their radiative decays to Υ(1S,2S)
             with Υ → μ+ μ-. In addition to the mass peaks
             corresponding to the decay modes χ(b)(1P,2P) → Υ(1S)γ,
             a new structure centered at a mass of 10.530 ± 0.005(stat)
             ± 0.009(syst)  GeV is also observed, in both the
             Υ(1S)γ and Υ(2S)γ decay modes. This structure is
             interpreted as the χ(b)(3P) system.},
   Doi = {10.1103/physrevlett.108.152001},
   Key = {fds309102}
}

@article{fds309103,
   Author = {Kotwal, AV and Collaboration, CDF},
   Title = {Precise Measurement of the W-Boson Mass with the CDF II
             Detector},
   Journal = {Phys. Rev. Lett.},
   Volume = {108},
   Number = {15},
   Pages = {151803},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.108.151803},
   Abstract = {We have measured the W-boson mass M(W) using data
             corresponding to 2.2  fb(-1) of integrated luminosity
             collected in pp collisions at sqrt[s] = 1.96  TeV with
             the CDF II detector at the Fermilab Tevatron collider.
             Samples consisting of 470,126 W → eν candidates and
             624,708 W → μν candidates yield the measurement M(W) =
             80,387 ± 12(stat.) ± 15(syst.) = 80,387 ± 19  MeV/c2.
             This is the most precise measurement of the W-boson mass to
             date and significantly exceeds the precision of all previous
             measurements combined.},
   Doi = {10.1103/physrevlett.108.151803},
   Key = {fds309103}
}

@article{fds309104,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurements of the angular distributions of muons from Υ
             decays in pp collisions at sqrt[s] = 1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {15},
   Pages = {151802},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.108.151802},
   Abstract = {The angular distributions of muons from Υ(1S,2S,3S) → μ+
             μ- decays are measured using data from pp collisions at
             sqrt[s] = 1.96  TeV corresponding to an integrated
             luminosity of 6.7  fb(-1) and collected with the CDF II
             detector at the Fermilab Tevatron. This analysis is the
             first to report the full angular distributions as functions
             of transverse momentum p(T) for Υ mesons in both the
             Collins-Soper and s-channel helicity frames. This is also
             the first measurement of the spin alignment of Υ(3S)
             mesons. Within the kinematic range of Υ rapidity |y|<0.6
             and p(T) up to 40  GeV/c, the angular distributions are
             found to be nearly isotropic.},
   Doi = {10.1103/physrevlett.108.151802},
   Key = {fds309104}
}

@article{fds309168,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonak, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for same-sign top-quark production and
             fourth-generation down-type quarks in pp collisions at √s
             = 7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2012)069},
   Abstract = {A search is presented for same-sign top-quark production and
             down-type heavy quarks of charge -1/3 in events with two
             isolated leptons (e or μ) that have the same electric
             charge, at least two jets and large missing transverse
             momentum. The data are selected from pp collisions at ps = 7
             TeV recorded by the ATLAS detector and correspond to an
             integrated luminosity of 1.04 fb-1. The observed data are
             consistent with expectations from Standard Model processes.
             Upper limits are set at 95% confidence level on the cross
             section of new sources of same-sign top-quark pair
             production of 1.4-2.0 pb depending on the assumed mediator
             mass. Upper limits are also set on the pair-production
             cross-section for new heavy down-type quarks; a lower limit
             of 450 GeV is set at 95% confidence level on the mass of
             heavy down-type quarks under the assumption that they decay
             100% of the time to Wt. Copyright CERN.},
   Doi = {10.1007/JHEP04(2012)069},
   Key = {fds309168}
}

@article{fds309203,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci,
             MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
   Title = {Search for standard model Higgs boson production in
             association with a W boson using a matrix element technique
             at CDF in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072001},
   Abstract = {This paper presents a search for standard model Higgs boson
             production in association with a W boson using events
             recorded by the CDF experiment in a data set corresponding
             to an integrated luminosity of 5.6fb -1. The search is
             performed using a matrix element technique in which the
             signal and background hypotheses are used to create a
             powerful discriminator. The discriminant output
             distributions for signal and background are fit to the
             observed events using a binned likelihood approach to search
             for the Higgs boson signal. We find no evidence for a Higgs
             boson, and 95% confidence level (C.L.) upper limits are set
             on σ(pp̄→WH)×B(H→bb̄). The observed limits range
             from 3.5 to 37.6 relative to the standard model expectation
             for Higgs boson masses between m H=100GeV/c2 and m
             H=150GeV/c2. The 95% C.L. expected limit is estimated from
             the median of an ensemble of simulated experiments and
             varies between 2.9 and 32.7 relative to the production rate
             predicted by the standard model over the Higgs boson mass
             range studied. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.85.072001},
   Key = {fds309203}
}

@article{fds309218,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan,
             A and Arisawa, T and Artikov, A and Ashmanskas, W and Auerbach, B and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
             L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Calancha, C and Campanelli, M and Campbell, M and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cerri, A and Cerrito, L and Chen, YC and Chiarelli, G and Chlachidze,
             G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
             Cecco, S and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M},
   Title = {An additional study of multi-muon events produced in pp-
             collisions at s=1.96 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {2},
   Pages = {278-283},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.081},
   Abstract = {We present one additional study of multi-muon events
             produced at the Fermilab Tevatron collider and recorded by
             the CDF II detector. We use a data set acquired with a
             dedicated dimuon trigger and corresponding to an integrated
             luminosity of 3.9 fb -1. We investigate the distribution of
             the azimuthal angle between the two trigger muons in events
             containing at least four additional muon candidates to test
             the compatibility of these events with originating from
             known QCD processes. We find that this distribution is
             markedly different from what is expected from such QCD
             processes and this observation strongly disfavors the
             possibility that multi-muon events result from an
             underestimate of the rate of misidentified muons in ordinary
             QCD events. © 2012 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2012.02.081},
   Key = {fds309218}
}

@article{fds309158,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
   Title = {Measurement of the centrality dependence of the charged
             particle pseudorapidity distribution in lead-lead collisions
             at √s NN=2.76 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {710},
   Number = {3},
   Pages = {363-382},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.02.045},
   Abstract = {The ATLAS experiment at the LHC has measured the centrality
             dependence of charged particle pseudorapidity distributions
             over |η|<2 in lead-lead collisions at a nucleon-nucleon
             centre-of-mass energy of √s NN=2.76 TeV. In order to
             include particles with transverse momentum as low as 30 MeV,
             the data were recorded with the central solenoid magnet off.
             Charged particles were reconstructed with two algorithms
             (2-point "tracklets" and full tracks) using information from
             the pixel detector only. The lead-lead collision centrality
             was characterized by the total transverse energy in the
             forward calorimeter in the range 3.2<|η|<4.9. Measurements
             are presented of the per-event charged particle
             pseudorapidity distribution, dN ch/dη, and the average
             charged particle multiplicity in the pseudorapidity interval
             |η|<0.5 in several intervals of collision centrality. The
             results are compared to previous mid-rapidity measurements
             at the LHC and RHIC. The variation of the mid-rapidity
             charged particle yield per colliding nucleon pair with the
             number of participants is consistent with lower sNN results.
             The shape of the dN ch/dη distribution is found to be
             independent of centrality within the systematic
             uncertainties of the measurement. © 2012
             CERN.},
   Doi = {10.1016/j.physletb.2012.02.045},
   Key = {fds309158}
}

@article{fds309136,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
   Title = {Measurement of the inclusive W± and Z/γ∗
             cross sections in the e and μ decay channels in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072004},
   Abstract = {The production cross sections of the inclusive Drell-Yan
             processes W ±→ν and Z/γ∗→(=e, μ) are measured in
             proton-proton collisions at √s=7TeV with the ATLAS
             detector. The cross sections are reported integrated over a
             fiducial kinematic range, extrapolated to the full range,
             and also evaluated differentially as a function of the W
             decay lepton pseudorapidity and the Z boson rapidity,
             respectively. Based on an integrated luminosity of about
             35pb-1 collected in 2010, the precision of these
             measurements reaches a few percent. The integrated and the
             differential W± and Z/γ∗ cross sections in the e and μ
             channels are combined, and compared with perturbative QCD
             calculations, based on a number of different parton
             distribution sets available at next-to-next-to-leading
             order.},
   Doi = {10.1103/PhysRevD.85.072004},
   Key = {fds309136}
}

@article{fds309202,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Bousson, N and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
   Title = {Measurement of the CP-violating phase βsJ/ψ in Bs0→J/ψ
             decays with the CDF II detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072002},
   Abstract = {We present a measurement of the CP-violating parameter
             βsJ/ψ using approximately 6500 Bs0→J/ψ decays
             reconstructed with the CDF II detector in a sample of pp̄
             collisions at √s=1.96TeV corresponding to 5.2fb -1
             integrated luminosity produced by the Tevatron collider at
             Fermilab. We find the CP-violating phase to be within the
             range βsJ/ψ [0.02,0.52] [1.08,1.55] at 68% confidence
             level where the coverage property of the quoted interval is
             guaranteed using a frequentist statistical analysis. This
             result is in agreement with the standard model expectation
             at the level of about one Gaussian standard deviation. We
             consider the inclusion of a potential S-wave contribution to
             the Bs0→J/ψK +K - final state which is found to be
             negligible over the mass interval 1.009<m(K +K
             -)<1.028GeV/c2. Assuming the standard model prediction for
             the CP-violating phase βsJ/ψ, we find the Bs0 decay width
             difference to be ΔΓ s=0.075±0.035(stat) ±0.006(syst)ps
             -1. We also present the most precise measurements of the Bs0
             mean lifetime τ(Bs0)=1.529±0.025(stat) ±0.012(syst)ps,
             the polarization fractions |A 0(0)|2=0. 524±0.013(stat)±0.015(syst)
             and |A -(0)|2=0. 231±0.014(stat)±0.015(syst), as well as
             the strong phase δ -=2.95±0.64(stat)±0.07(syst)rad. In
             addition, we report an alternative Bayesian analysis that
             gives results consistent with the frequentist approach. ©
             2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.072002},
   Key = {fds309202}
}

@article{fds309129,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for excited leptons in proton-proton collisions at
             √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.072003},
   Abstract = {The ATLAS detector is used to search for excited leptons in
             the electromagnetic radiative decay channel *→γ. Results
             are presented based on the analysis of pp collisions at a
             center-of-mass energy of 7 TeV corresponding to an
             integrated luminosity of 2.05fb-1. No evidence for excited
             leptons is found, and limits are set on the compositeness
             scale Λ as a function of the excited lepton mass m *. In
             the special case where Λ=m *, excited electron and muon
             masses below 1.87 TeV and 1.75 TeV are excluded at 95% C.L.,
             respectively. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.85.072003},
   Key = {fds309129}
}

@article{fds309194,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Asman, B and Atkins, S and Atramentov, O and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barreto, J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Belanger-Champagne, C and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bezzubov, VA and Bhatia, S and Bhatnagar, V and Bhatti, A and Bhat, PC and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Brooijmans, G and Bross, A and Brown, D and Brown, J and Brucken, E and Bu,
             XB},
   Title = {Combination of CDF and D0 measurements of the W boson
             helicity in top quark decays},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.071106},
   Abstract = {We report the combination of recent measurements of the
             helicity of the W boson from top quark decay by the CDF and
             D0 collaborations, based on data samples corresponding to
             integrated luminosities of 2.7-5.4fb -1 of pp̄ collisions
             collected during Run II of the Fermilab Tevatron collider.
             Combining measurements that simultaneously determine the
             fractions of W bosons with longitudinal (f 0) and
             right-handed (f +) helicities, we find f
             0=0.722±0.081[±0.062(stat)±0.052(syst)] and f
             +=-0.033±0.046[±0.034(stat)±0.031(syst)]. Combining
             measurements where one of the helicity fractions is fixed to
             the value expected in the standard model, we find f
             0=0.682±0. 057[±0.035(stat)±0.046(syst)] for fixed f +
             and f +=-0.015±0.035[±0.018(stat)±0.030(syst)] for fixed
             f 0. The results are consistent with standard model
             expectations. © 2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.071106},
   Key = {fds309194}
}

@article{fds309094,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
             G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
             W},
   Title = {Observation of spin correlation in tt¯ events from pp
             collisions at √s=7 TeV using the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {212001},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.212001},
   Abstract = {A measurement of spin correlation in tt[over ¯] production
             is reported using data collected with the ATLAS detector at
             the LHC, corresponding to an integrated luminosity of 2.1
             fb(-1). Candidate events are selected in the dilepton
             topology with large missing transverse energy and at least
             two jets. The difference in azimuthal angle between the two
             charged leptons in the laboratory frame is used to extract
             the correlation between the top and antitop quark spins. In
             the helicity basis the measured degree of correlation
             corresponds to A(helicity)=0.40(-0.08)(+0.09), in agreement
             with the next-to-leading-order standard model prediction.
             The hypothesis of zero spin correlation is excluded at 5.1
             standard deviations.},
   Doi = {10.1103/physrevlett.108.212001},
   Key = {fds309094}
}

@article{fds309095,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benitez Garcia and JA and Benjamin, DP and Benoit,
             M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for production of resonant states in the photon-jet
             mass distribution using pp collisions at √s=7 TeV
             collected by the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211802},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211802},
   Abstract = {This Letter describes a model-independent search for the
             production of new resonant states in photon+jet events in
             2.11 fb(-1) of proton-proton collisions at √s=7 TeV. We
             compare the photon+jet mass distribution to a background
             model derived from data and find consistency with the
             background-only hypothesis. Given the lack of evidence for a
             signal, we set 95% credibility level limits on generic
             Gaussian-shaped signals and on a benchmark excited-quark
             (q*) model, excluding 2 TeV Gaussian resonances with cross
             section times branching fraction times acceptance times
             efficiency near 5 fb and excluding q* masses below 2.46 TeV,
             respectively.},
   Doi = {10.1103/physrevlett.108.211802},
   Key = {fds309095}
}

@article{fds309096,
   Author = {Aaltonen, T and Adelman, J and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for a heavy particle decaying to a top quark and a
             light quark in pp ¯ collisions at √s=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211805},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211805},
   Abstract = {We present a search for a new heavy particle X produced in
             association with a top quark, pp[over ¯]→t(X→t[over
             ¯]q) or pp[over ¯]→t[over ¯](X[over ¯]→tq[over ¯]),
             where q stands for up quarks and down quarks. Such a
             particle may explain the recent anomalous measurements of
             top-quark forward-backward asymmetry. If the light-flavor
             quark (q) is reconstructed as a jet (j), this gives a t[over
             ¯]+j or t+j resonance in tt[over ¯]+jet events, a
             previously unexplored experimental signature. In a sample of
             events with exactly one lepton, missing transverse momentum
             and at least five jets, corresponding to an integrated
             luminosity of 8.7 fb(-1) collected by the CDF II detector,
             we find the data to be consistent with the standard model.
             We set cross-section upper limits on the production (pp[over
             ¯]→Xt or X[over ¯]t[over ¯]) at 95% confidence level
             from 0.61 pb to 0.02 pb for X masses ranging from 200
             GeV/c(2) to 800 GeV/c(2), respectively.},
   Doi = {10.1103/physrevlett.108.211805},
   Key = {fds309096}
}

@article{fds309097,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Bai,
             Y and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Fox, PJ and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harnik, R and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins,
             W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
             T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
             DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
             J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paus, C and Pellett,
             DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for dark matter in events with one jet and missing
             transverse energy in pp¯ collisions at √s=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211804},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211804},
   Abstract = {We present the results of a search for dark matter
             production in the monojet signature. We analyze a sample of
             Tevatron pp[over ¯] collisions at √s=1.96 TeV
             corresponding to an integrated luminosity of 6.7 fb(-1)
             recorded by the CDF II detector. In events with large
             missing transverse energy and one energetic jet, we find
             good agreement between the standard model prediction and the
             observed data. We set 90% confidence level upper limits on
             the dark matter production rate. The limits are translated
             into bounds on nucleon-dark matter scattering rates which
             are competitive with current direct detection bounds on
             spin-independent interaction below a dark matter candidate
             mass of 5 GeV/c(2), and on spin-dependent interactions up to
             masses of 200 GeV/c(2).},
   Doi = {10.1103/physrevlett.108.211804},
   Key = {fds309097}
}

@article{fds309098,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzá, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Fuks, B and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for a dark matter candidate produced in association
             with a single top quark in pp collisions at
             √[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {20},
   Pages = {201802},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.201802},
   Abstract = {We report a new search for dark matter in a data sample of
             an integrated luminosity of 7.7  fb-1 of Tevatron
             pp[over ¯] collisions at √[s]=1.96  TeV, collected by
             the CDF II detector. We search for production of a
             dark-matter candidate, D, in association with a single top
             quark. We consider the hadronic decay mode of the top quark
             exclusively, yielding a final state of three jets with
             missing transverse energy. The data are consistent with the
             standard model; we thus set 95% confidence level upper
             limits on the cross section of the process pp[over ¯]→t+D
             as a function of the mass of the dark-matter candidate. The
             limits are approximately 0.5 pb for a dark-matter particle
             with mass in the range of 0-150  GeV/c2.},
   Doi = {10.1103/physrevlett.108.201802},
   Key = {fds309098}
}

@article{fds309099,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of Bs0→Ds(*)+Ds(*)- branching
             ratios.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {20},
   Pages = {201801},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.201801},
   Abstract = {The decays Bs0→Ds(*)+Ds(*)- are reconstructed in a data
             sample corresponding to an integrated luminosity of
             6.8  fb-1 collected by the CDF II detector at the
             Tevatron pp[over ¯] collider. All decay modes are observed
             with a significance of more than 10σ, and we measure the
             Bs0 production rate times Bs0→Ds(*)+Ds(*)- branching
             ratios relative to the normalization mode B0→Ds+D-to be
             0.183±0.021±0.017 for Bs0→Ds+Ds-, 0.424±0.046±0.035
             for Bs0→Ds*±Ds^∓, 0.654±0.072±0.065 for
             Bs0→Ds*+Ds*-, and 1.261±0.095±0.112 for the inclusive
             decay Bs0→Ds(*)+Ds(*)-, where the uncertainties are
             statistical and systematic. These results are the most
             precise single measurements to date and provide important
             constraints for indirect searches for nonstandard model
             physics in Bs0 mixing.},
   Doi = {10.1103/physrevlett.108.201801},
   Key = {fds309099}
}

@article{fds309100,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati,
             S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
             N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
             R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
             F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
             U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for scalar bottom quark pair production with the
             ATLAS detector in pp collisions at sqrt[s]=7  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {18},
   Pages = {181802},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.181802},
   Abstract = {The results of a search for pair production of the scalar
             partners of bottom quarks in 2.05  fb(-1) of pp
             collisions at sqrt[s]=7  TeV using the ATLAS experiment
             are reported. Scalar bottom quarks are searched for in
             events with large missing transverse momentum and two jets
             in the final state, where both jets are identified as
             originating from a bottom quark. In an R-parity conserving
             minimal supersymmetric scenario, assuming that the scalar
             bottom quark decays exclusively into a bottom quark and a
             neutralino, 95% confidence-level upper limits are obtained
             in the b(1) - χ(1)(0) mass plane such that for neutralino
             masses below 60 GeV scalar bottom masses up to 390 GeV are
             excluded.},
   Doi = {10.1103/physrevlett.108.181802},
   Key = {fds309100}
}

@article{fds309101,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
             HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
             C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
             G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
             JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
             K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
             M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
             A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
             DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
             E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
             P and Makhoul, K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín,
             R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
             E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
             R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
             A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
             M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
             T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
             M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
             P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
             J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
             T},
   Title = {Search for a low-mass standard model Higgs boson in the ττ
             decay channel in pp collisions at sqrt[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {18},
   Pages = {181804},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.181804},
   Abstract = {We report on a search for the standard model Higgs boson
             decaying into pairs of τ leptons in pp collisions produced
             by the Tevatron at sqrt[s]=1.96  TeV. The analyzed data
             sample was recorded by the CDFII detector and corresponds to
             an integrated luminosity of 6.0  fb(-1). The search is
             performed in the final state with one τ decaying
             leptonically and the second one identified through its
             semihadronic decay. Since no significant excess is observed,
             a 95% credibility level upper limit on the production cross
             section times branching ratio to the ττ final state is set
             for hypothetical Higgs boson masses between 100 and
             150  GeV/c2. For a Higgs boson of 120  GeV/c2 the
             observed (expected) limit is 14.6 (15.3) the predicted
             value.},
   Doi = {10.1103/physrevlett.108.181804},
   Key = {fds309101}
}

@article{fds309119,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the polarisation of W bosons produced with
             large transverse momentum in pp collisions at √s =7 TeV
             with the ATLAS experiment},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {5},
   Pages = {1-30},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2001-6},
   Abstract = {This paper describes an analysis of the angular distribution
             of W→eν and W→μν decays, using data from pp
             collisions at √s =7 TeV recorded with the ATLAS detector
             at the LHC in 2010, corresponding to an integrated
             luminosity of about 35 pb-1. Using the decay lepton
             transverse momentum and the missing transverse momentum, the
             W decay angular distribution projected onto the transverse
             plane is obtained and analysed in terms of helicity
             fractions f0, fL and fR over two ranges of W transverse
             momentum (pWT): 35 < pWT < 50 GeV and pWT > 50 GeV. Good
             agreement is found with theoretical predictions. For pWT >50
             GeV, the values of f0 and fL-fR, averaged over charge and
             lepton flavour, are measured to be: f0=0. 127±0. 030±0.
             108 and fL-fR=0. 252±0. 017±0. 030, where the first
             uncertainties are statistical, and the second include all
             systematic effects. © 2012 CERN for the benefit of the
             ATLAS collaboration.},
   Doi = {10.1140/epjc/s10052-012-2001-6},
   Key = {fds309119}
}

@article{fds309215,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt,
             N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S and CDF Collaboration},
   Title = {Evidence for the charmless annihilation decay mode
             B(s)(0)→π(+)π(-).},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {21},
   Pages = {211803},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.108.211803},
   Abstract = {We search for annihilation decay modes of neutral b mesons
             into pairs of charmless charged hadrons with the upgraded
             Collider Detector at the Fermilab Tevatron. Using a data
             sample corresponding to 6 fb(-1) of integrated luminosity,
             we obtain the first evidence for the B(s)(0)→π(+)π(-)
             decay, with a significance of 3.7σ, and a measured
             branching ratio B(B(s)(0)→π(+)π(-))=(0.57±0.15(stat)±0.10(syst))×10(-6).
             A search for the B(0)→K(+)K(-) mode in the same sample
             yields a significance of 2.0σ, and a central value estimate
             B(B(0)→K(+)K(-))=(0.23±0.10(stat)±0.10(syst))×10(-6).},
   Doi = {10.1103/physrevlett.108.211803},
   Key = {fds309215}
}

@article{fds309135,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C},
   Title = {Study of jets produced in association with a W boson in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092002},
   Abstract = {We report a study of final states containing a W boson and
             hadronic jets, produced in proton-proton collisions at a
             center-of-mass energy of 7 TeV. The data were collected with
             the ATLAS detector at the CERN LHC and comprise the full
             2010 data sample of 36pb-1. Cross sections are determined
             using both the electron and muon decay modes of the W boson
             and are presented as a function of inclusive jet
             multiplicity, Njet, for up to five jets. At each
             multiplicity, cross sections are presented as a function of
             jet transverse momentum, the scalar sum of the transverse
             momenta of the charged lepton, missing transverse momentum,
             and all jets, the invariant mass spectra of jets, and the
             rapidity distributions of various combinations of leptons
             and final-state jets.},
   Doi = {10.1103/PhysRevD.85.092002},
   Key = {fds309135}
}

@article{fds309196,
   Author = {Aaltonen, T and Alon, R and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi,
             J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli,
             M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
             C and Cuevas, J and Culbertson, R},
   Title = {Study of substructure of high transverse momentum jets
             produced in proton-antiproton collisions at
             √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.091101},
   Abstract = {A study of the substructure of jets with transverse momentum
             greater than 400GeV/c produced in proton-antiproton
             collisions at a center-of-mass energy of 1.96 TeV at the
             Fermilab Tevatron Collider and recorded by the CDF II
             detector is presented. The distributions of the jet mass,
             angularity, and planar flow are measured for the first time
             in a sample with an integrated luminosity of 5.95fb -1. The
             observed substructure for high mass jets is consistent with
             predictions from perturbative quantum chromodynamics. ©
             2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.85.091101},
   Key = {fds309196}
}

@article{fds309213,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Search for anomalous production of multiple leptons in
             association with W and Z bosons at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092001},
   Abstract = {This paper presents a search for anomalous production of
             multiple low-energy leptons in association with a W or Z
             boson using events collected at the CDF experiment
             corresponding to 5.1fb -1 of integrated luminosity. This
             search is sensitive to a wide range of topologies with
             low-momentum leptons, including those with the leptons near
             one another. The observed rates of production of additional
             electrons and muons are compared with the standard model
             predictions. No indications of phenomena beyond the standard
             model are found. A 95% confidence level limit is presented
             on the production cross section for a benchmark model of
             supersymmetric hidden-valley Higgs production. Particle
             identification efficiencies are also provided to enable the
             calculation of limits on additional models. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.85.092001},
   Key = {fds309213}
}

@article{fds309197,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
             M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
             R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Di Canto,
             A},
   Title = {Measurement of the masses and widths of the bottom baryons
             Σb± and Σb*±},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092011},
   Abstract = {Using data from pp̄ collisions at √s=1.96TeV recorded by
             the CDF II detector at the Fermilab Tevatron, we present
             improved measurements of the masses and first measurements
             of natural widths of the four bottom baryon resonance states
             Σb+, Σb*+ and Σb-, Σb*-. These states are fully
             reconstructed in their decay modes to Λb0π ± where
             Λb0→Λc+π - with Λc+→pK -π +. The analysis is based
             on a data sample corresponding to an integrated luminosity
             of 6.0fb -1 collected by an online event selection based on
             tracks displaced from the pp̄ interaction point. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.092011},
   Key = {fds309197}
}

@article{fds309130,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the production cross section of an isolated
             photon associated with jets in proton-proton collisions at
             √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.092014},
   Abstract = {A measurement of the cross section for the production of an
             isolated photon in association with jets in proton-proton
             collisions at a center-of-mass energy √s=7TeV is
             presented. Photons are reconstructed in the pseudorapidity
             range |ηγ|<1.37 and with a transverse energy ETγ>25GeV.
             Jets are reconstructed in the rapidity range |yjet|<4.4 and
             with a transverse momentum pTjet>20GeV. The differential
             cross section dσ/dETγ is measured, as a function of the
             photon transverse energy, for three different rapidity
             ranges of the leading-pT jet: |yjet|<1.2, 1.2≤|yjet|<2.8
             and 2.8≤|yjet|<4.4. For each rapidity configuration the
             same-sign (ηγyjet 0) and opposite-sign (ηγyjet<0) cases
             are studied separately. The results are based on an
             integrated luminosity of 37pb-1, collected with the ATLAS
             detector at the LHC. Next-to-leading order perturbative QCD
             calculations are found to be in fair agreement with the
             data, except for ETγ 45GeV, where the theoretical
             predictions overestimate the measured cross sections. ©
             2012 CERN.},
   Doi = {10.1103/PhysRevD.85.092014},
   Key = {fds309130}
}

@article{fds309169,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Erratum to: "Search for first generation scalar leptoquarks
             in pp collisions at s=7TeV with the ATLAS detector" [Phys.
             Lett. B 709 (2012) 158]},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {711},
   Number = {5},
   Pages = {442-455},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.03.023},
   Doi = {10.1016/j.physletb.2012.03.023},
   Key = {fds309169}
}

@article{fds309090,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova,
             L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa,
             HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
             A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Cherkaoui
             El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot, J and Colon,
             G and Conde Muiño and P and Coniavitis, E and Conidi,
             MC},
   Title = {Search for supersymmetry in events with three leptons and
             missing transverse momentum in √[s]=7 TeV pp collisions
             with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {26},
   Pages = {261804},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.261804},
   Abstract = {A search for the weak production of charginos and
             neutralinos decaying to a final state with three leptons
             (electrons or muons) and missing transverse momentum is
             presented. The analysis uses 2.06 fb(-1) of √[s]=7 TeV
             proton-proton collision data delivered by the Large Hadron
             Collider and recorded with the ATLAS detector. Observations
             are consistent with standard model expectations in two
             signal regions that are either depleted or enriched in
             Z-boson decays. Upper limits at 95% confidence level are set
             in R-parity conserving phenomenological minimal
             supersymmetric and simplified models. For the simplified
             models, degenerate lightest chargino and next-to-lightest
             neutralino masses up to 300 GeV are excluded for mass
             differences from the lightest neutralino up to 300
             GeV.},
   Doi = {10.1103/physrevlett.108.261804},
   Key = {fds309090}
}

@article{fds309091,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Search for pair production of a heavy up-type quark decaying
             to a W boson and a b quark in the lepton + jets channel with
             the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {26},
   Pages = {261802},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.261802},
   Abstract = {A search is presented for production of a heavy up-type
             quark (t') together with its antiparticle, assuming
             subsequent decay to a W boson and a b quark, t't[over
             ¯]'→W(+)bW(-)b[over ¯]. The search is based on 1.04
             fb(-1) of proton-proton collisions at √[s]=7 TeV collected
             by the ATLAS detector at the CERN Large Hadron Collider.
             Data are analyzed in the lepton+jets final state,
             characterized by a high transverse momentum isolated
             electron or muon, high missing transverse momentum, and at
             least three jets. No significant excess of events above the
             background expectation is observed. A 95% C.L. lower limit
             of 404 GeV is set for the mass of the t'
             quark.},
   Doi = {10.1103/physrevlett.108.261802},
   Key = {fds309091}
}

@article{fds309092,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
             K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau,
             T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for a light Higgs boson decaying to long-lived weakly
             interacting particles in proton-proton collisions at sqrt[s]
             = 7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {25},
   Pages = {251801},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.251801},
   Abstract = {A search for the decay of a light Higgs boson (120-140 GeV)
             to a pair of weakly interacting, long-lived particles in
             1.94 fb(-1) of proton-proton collisions at sqrt[s] = 7 TeV
             recorded in 2011 by the ATLAS detector is presented. The
             search strategy requires that both long-lived particles
             decay inside the muon spectrometer. No excess of events is
             observed above the expected background and limits on the
             Higgs boson production times branching ratio to weakly
             interacting, long-lived particles are derived as a function
             of the particle proper decay length.},
   Doi = {10.1103/physrevlett.108.251801},
   Key = {fds309092}
}

@article{fds309093,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
             G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
             S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
             U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth,
             CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B},
   Title = {Search for gluinos in events with two same-sign leptons,
             jets, and missing transverse momentum with the ATLAS
             detector in pp collisions at sqrt[s]=7  TeV.},
   Journal = {Physical review letters},
   Volume = {108},
   Number = {24},
   Pages = {241802},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.108.241802},
   Abstract = {A search is presented for gluinos decaying via the
             supersymmetric partner of the top quark using events with
             two same-sign leptons, jets, and missing transverse
             momentum. The analysis is performed with 2.05  fb(-1) of
             integrated luminosity from pp collisions at
             sqrt[s]=7  TeV collected by the ATLAS detector at the
             LHC. No excess beyond the standard model expectation is
             observed, and exclusion limits are derived for simplified
             models where the gluino decays via the supersymmetric
             partner of the top quark and in the minimal supergravity and
             constrained minimal supersymmetric standard model framework.
             In those scenarios, gluino masses below 550 GeV are excluded
             at 95% C.L. within the parameter space considered,
             significantly extending the coverage with respect to
             existing limits. Depending on the model parameters, gluino
             masses up to 750 GeV can also be excluded at 95%
             C.L.},
   Doi = {10.1103/physrevlett.108.241802},
   Key = {fds309093}
}

@article{fds309222,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Search for anomaly-mediated supersymmetry breaking with the
             ATLAS detector based on a disappearing-track signature in pp
             collisions at √s=7 TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {4},
   Pages = {1-20},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-1993-2},
   Abstract = {In models of anomaly-mediated supersymmetry breaking (AMSB),
             the lightest chargino is predicted to have a lifetime long
             enough to be detected in collider experiments. This letter
             explores AMSB scenarios in pp collisions at (Formula
             Presented) = 7 TeV by attempting to identify decaying
             charginos which result in tracks that appear to have few
             associated hits in the outer region of the tracking system.
             The search was based on data corresponding to an integrated
             luminosity of 1.02 fb−1collected with the ATLAS detector
             in 2011. The pT spectrum of candidate tracks is found to be
             consistent with the expectation from Standard Model
             background processes and constraints on the lifetime and the
             production cross section were obtained. In the minimal AMSB
             framework with m3/2< 32 TeV, m0< 1.5 TeV, tanβ = 5 and μ >
             0, a chargino having mass below 92 GeV and a lifetime
             between 0.5 ns and 2 ns is excluded at 95 % confidence
             level.},
   Doi = {10.1140/epjc/s10052-012-1993-2},
   Key = {fds309222}
}

@article{fds309127,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the cross section for top-quark pair
             production in pp collisions at √s = 7 TeV with the ATLAS
             detector using final states with two high-pT
             leptons},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP05(2012)059},
   Abstract = {A measurement is reported of the production cross section of
             top-quark pairs (tt̄) in proton-proton collisions at a
             center-of-mass energy of 7 TeV recorded with the ATLAS
             detector at the LHC. Candidate events have a signature
             consistent with containing two isolated leptons, large
             missing transverse momentum, and at least two jets. Using a
             data sample corresponding to an integrated luminosity of
             0.70 fb-1, a tt̄ production cross section σtt̄ = 176 ±
             5(stat.)-1111+(syst.) ± 8(lum.) pb is measured for an
             assumed top-quark mass of mt = 172.5 GeV. This measurement
             is in good agreement with Standard Model predictions. ©
             CERN.},
   Doi = {10.1007/JHEP05(2012)059},
   Key = {fds309127}
}

@article{fds309121,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for FCNC single top-quark production at √s=7 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {712},
   Number = {4-5},
   Pages = {351-369},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.05.022},
   Abstract = {A search for the production of single top-quarks via
             flavour-changing neutral-currents is presented. Data
             collected with the ATLAS detector at a centre-of-mass energy
             of s=7 TeV, corresponding to an integrated luminosity of
             2.05 fb−1, are used. Candidate events with a semileptonic
             top-quark decay signature are classified as signal- or
             background-like events by using several kinematic variables
             as input to a neural network. No signal is observed in the
             neural network output distribution and a Bayesian upper
             limit is placed on the production cross-section. The
             observed upper limit at 95% confidence level on the
             cross-section multiplied by the t→Wb branching fraction is
             measured to be σqg→t×B(t→Wb)<3.9 pb. This upper limit
             is converted using a model-independent approach into upper
             limits on the coupling strengths κugt/Λ<6.9⋅10−3
             TeV−1 and κcgt/Λ<1.6⋅10−2 TeV−1, where Λ is the
             new physics scale, and on the branching fractions
             B(t→ug)<5.7⋅10−5 and B(t→cg)<2.7⋅10−4.},
   Doi = {10.1016/j.physletb.2012.05.022},
   Key = {fds309121}
}

@article{fds309177,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for supersymmetry in pp collisions at √s=7TeV in
             final states with missing transverse momentum and b-jets
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.112006},
   Abstract = {The results of a search for supersymmetry in events with
             large missing transverse momentum and heavy-flavor jets
             using an integrated luminosity corresponding to 2.05fb-1 of
             pp collisions at √s=7TeV recorded with the ATLAS detector
             at the Large Hadron Collider are reported. No significant
             excess is observed with respect to the prediction for
             standard model processes. Results are interpreted in a
             variety of R-parity conserving models in which scalar
             bottoms and tops are the only scalar quarks to appear in the
             gluino decay cascade, and in an SO(10) model framework.
             Gluino masses up to 600-900GeV are excluded, depending on
             the model considered. © 2012 CERN. Published by the
             American Physical Society.},
   Doi = {10.1103/PhysRevD.85.112006},
   Key = {fds309177}
}

@article{fds310555,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for resonant WZ production in the WZ → ℓνℓ′
             ℓ ′ channel in √ (s) = 7 TeV pp collisions with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {85},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.85.112012},
   Abstract = {A generic search is presented for a heavy particle decaying
             to WZ → ℓν′ ℓ ′ (ℓ, ℓ′ = e, μ)final
             states. The data were recorded by the ATLAS detector in
             ffiffiffis √ s = 7 TeV pp collisions at the Large Hadron
             Collider and correspond to an integrated luminosity of 1:02
             fb-1. The transverse mass distribution of the selected WZ
             candidates is found to be consistent with the standard model
             expectation. Upper limits on the production cross section
             times branching ratio are derived using two benchmark models
             predicting a heavy particle decaying to a WZ
             pair.},
   Doi = {10.1103/PhysRevD.85.112012},
   Key = {fds310555}
}

@article{fds309085,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
             JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C},
   Title = {Search for down-type fourth generation quarks with the ATLAS
             detector in events with one lepton and hadronically decaying
             W bosons.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {3},
   Pages = {032001},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.109.032001},
   Abstract = {This Letter presents a search for pair production of heavy
             down-type quarks decaying via b' → Wt in the lepton + jets
             channel, as b'b' → W- tW+ t → bbW+ W- W+ W- → l±
             νbbqqqqqq. In addition to requiring exactly one lepton,
             large missing transverse momentum, and at least six jets,
             the invariant mass of nearby jet pairs is used to identify
             high transverse momentum W bosons. In data corresponding to
             an integrated luminosity of 1.04  fb(-1) from pp
             collisions at sqrt[s] = 7  TeV recorded with the ATLAS
             detector, a heavy down-type quark with mass less than 480
             GeV can be excluded at the 95% confidence
             level.},
   Doi = {10.1103/physrevlett.109.032001},
   Key = {fds309085}
}

@article{fds309086,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
             K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
             V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
             A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
             F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
             M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
             JC and Clement, B and Clement, C and Clifft, RW},
   Title = {Determination of the strange-quark density of the proton
             from ATLAS measurements of the W→ℓν and Z→ℓℓ
             cross sections.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {1},
   Pages = {012001},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.109.012001},
   Abstract = {A QCD analysis is reported of ATLAS data on inclusive W(±)
             and Z boson production in pp collisions at the LHC, jointly
             with ep deep-inelastic scattering data from HERA. The ATLAS
             data exhibit sensitivity to the light quark sea composition
             and magnitude at Bjorken x∼0.01. Specifically, the data
             support the hypothesis of a symmetric composition of the
             light quark sea at low x. The ratio of the strange-to-down
             sea quark distributions is determined to be
             1.00(-0.28)(+0.25) at absolute four-momentum transfer
             squared Q(2)=1.9  GeV(2) and x=0.023.},
   Doi = {10.1103/physrevlett.109.012001},
   Key = {fds309086}
}

@article{fds309089,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Hunt for new phenomena using large jet multiplicities and
             missing transverse momentum with ATLAS in 4.7
             fb-1 of √s = 7 TeV proton-proton
             collisions},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {7},
   Pages = {1-39},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2012)167},
   Abstract = {Results are presented of a search for new particles decaying
             to large numbers of jets in association with missing
             transverse momentum, using 4.7 fb-1 of pp collision data at
             √s = 7 TeV collected by the ATLAS experiment at the Large
             Hadron Collider in 2011. The event selection requires
             missing transverse momentum, no isolated electrons or muons,
             and from ≥6 to ≥9 jets. No evidence is found for physics
             beyond the Standard Model. The results are interpreted in
             the context of a MSUGRA/CMSSM supersymmetric model, where,
             for large universal scalar mass m0, gluino masses smaller
             than 840 GeV are excluded at the 95% confidence level,
             extending previously published limits. Within a simplified
             model containing only a gluino octet and a neutralino,
             gluino masses smaller than 870 GeV are similarly excluded
             for neutralino masses below 100 GeV. Copyright
             CERN.},
   Doi = {10.1007/JHEP07(2012)167},
   Key = {fds309089}
}

@article{fds309133,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for pair-produced heavy quarks decaying to Wq in the
             two-lepton channel at √(s)=7TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.012007},
   Abstract = {A search is presented for heavy-quark pair production (QQ̄)
             under the decay hypothesis QQ̄→W+qW-q̄ with q=d, s, b
             for up-type Q or q=u, c for down-type Q. The search is
             performed with 1.04fb-1 of integrated luminosity from pp
             collisions at √s=7TeV collected by the ATLAS detector at
             the CERN LHC. Dilepton final states are selected, requiring
             large missing transverse momentum and at least two jets.
             Mass reconstruction of heavy-quark candidates is performed
             by assuming that the W boson decay products are nearly
             collinear. The data are in agreement with standard model
             expectations; a heavy quark with mass less than 350 GeV is
             excluded at 95% confidence level. © 2012 CERN. Published by
             the American Physical Society under the terms of the
             http://creativecommons.org/licenses/by/ 3.0/ Creative
             Commons Attribution 3.0 License. Further distribution of
             this work must maintain attribution to the author(s) and the
             published article's title, journal citation, and
             DOI.},
   Doi = {10.1103/PhysRevD.86.012007},
   Key = {fds309133}
}

@article{fds309141,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
             E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Measurement of inclusive jet and dijet production in pp
             collisions at √s=7TeV using the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.014022},
   Abstract = {Inclusive jet and dijet cross sections have been measured in
             proton-proton collisions at a center-of-mass energy of 7 TeV
             using the ATLAS detector at the Large Hadron Collider. The
             cross sections were measured using jets clustered with the
             anti-kt algorithm with parameters R=0.4 and R=0.6. These
             measurements are based on the 2010 data sample, consisting
             of a total integrated luminosity of 37pb-1. Inclusive jet
             double-differential cross sections are presented as a
             function of jet transverse momentum, in bins of jet
             rapidity. Dijet double-differential cross sections are
             studied as a function of the dijet invariant mass, in bins
             of half the rapidity separation of the two leading jets. The
             measurements are performed in the jet rapidity range
             |y|<4.4, covering jet transverse momenta from 20 GeV to 1.5
             TeV and dijet invariant masses from 70 GeV to 5 TeV. The
             data are compared to expectations based on
             next-to-leading-order QCD calculations corrected for
             nonperturbative effects, as well as to next-to-leading-order
             Monte Carlo predictions. In addition to a test of the theory
             in a new kinematic regime, the data also provide sensitivity
             to parton distribution functions in a region where they are
             currently not well-constrained. © 2012 CERN. Published by
             the American Physical Society under the terms of the
             http://creativecommons.org/licenses/by/ 3.0/ Creative
             Commons Attribution 3.0 License. Further distribution of
             this work must maintain attribution to the author(s) and the
             published article's title, journal citation, and
             DOI.},
   Doi = {10.1103/PhysRevD.86.014022},
   Key = {fds309141}
}

@article{fds309217,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M},
   Title = {Measurement of the top quark mass in the all-hadronic mode
             at CDF},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {714},
   Number = {1},
   Pages = {24-31},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.007},
   Abstract = {A measurement of the top quark mass (M top) in the
             all-hadronic decay channel is presented. It uses 5.8 fb -1
             of pp data collected with the CDF II detector at the
             Fermilab Tevatron Collider. Events with six to eight jets
             are selected by a neural network algorithm and by the
             requirement that at least one of the jets is tagged as a
             b-quark jet. The measurement is performed with a likelihood
             fit technique, which simultaneously determines M top and the
             jet energy scale (JES) calibration. The fit yields a value
             of M top=172.5±1.4(stat)±1.0(JES)±1.1(syst) GeV/c 2. ©
             2012 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2012.06.007},
   Key = {fds309217}
}

@article{fds309082,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Search for tb resonances in proton-proton collisions at
             √s=7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {8},
   Pages = {081801},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.109.081801},
   Abstract = {This Letter presents a search for tb resonances in 1.04
             fb(-1) of LHC proton-proton collision data collected by the
             ATLAS detector at a center-of-mass energy of 7 TeV. Events
             with a lepton, missing transverse momentum, and two jets are
             selected and the invariant mass of the corresponding final
             state is reconstructed. The search exploits the shape of the
             tb invariant mass distribution compared to the expected
             standard model backgrounds. The model of a right-handed
             W(R)' with standard model-like couplings is chosen as the
             benchmark model for this search. No statistically
             significant excess of events is observed in the data, and
             upper limits on the cross section times the branching ratio
             of W(R)' resonances at 95% C.L. lie in the range of 6.1-1.0
             pb for W(R)' masses ranging from 0.5 to 2.0 TeV. These
             limits are translated into a lower bound on the allowed
             right-handed W(R)' mass, giving m(W(R)'))>1.13 TeV at 95%
             C.L.},
   Doi = {10.1103/physrevlett.109.081801},
   Key = {fds309082}
}

@article{fds309083,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
             Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
             PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
             I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
             G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
             X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
   Title = {Search for pair production of a new b' quark that decays
             into a Z boson and a bottom quark with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {7},
   Pages = {071801},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.109.071801},
   Abstract = {A search is reported for the pair production of a new quark
             b' with at least one b' decaying to a Z boson and a bottom
             quark. The data, corresponding to 2.0 fb(-1) of integrated
             luminosity, were collected from pp collisions at √s = 7
             TeV with the ATLAS detector at the CERN Large Hadron
             Collider. Using events with a b-tagged jet and a Z boson
             reconstructed from opposite-charge electrons, the mass
             distribution of large transverse momentum b' candidates is
             tested for an enhancement. No evidence for a b' signal is
             detected in the observed mass distribution, resulting in the
             exclusion at a 95% confidence level of b' quarks with masses
             m (b') < 400 GeV that decay entirely via b' → Z+b. In the
             case of a vectorlike singlet b' mixing solely with the third
             standard model generation, masses m(b') < 358 GeV are
             excluded.},
   Doi = {10.1103/physrevlett.109.071801},
   Key = {fds309083}
}

@article{fds309084,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
             S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
             M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto,
             G and Bussey, P and Buszello, CP and Buzatu, A and Calamba, A and Calancha,
             C and Camacho-Pérez, E and Camarda, S and Campanelli, M and Campbell,
             M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
             S and Carron, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chakrabarti, S and Chakraborty, D and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chevalier-Théry,
             S and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, DK and Cho,
             K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Chung, WH and Chung, YS and Cihangir, S and Ciocci, MA and Claes, D and Clark, A and Clarke, C and Clutter, J and Compostella, G and Convery, ME and Conway,
             J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Crescioli, F and Croc, A and Cuevas, J and Culbertson, R and Cutts, D and Dagenhart, D and d'Ascenzo, N and Das, A and Datta, M and Davies, G and de Barbaro, P and de
             Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Dell'orso, M and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
             SP and d'Errico, M and Desai, S and Deterre, C and Devaughan, K and Devoto,
             F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
             PF and Dittmann, JR and Dominguez, A and Donati, S and Dong, P and D'Onofrio, M and Dorigo, M and Dorigo, T and Dubey, A and Dudko, LV and Duggan, D and Duperrin, A and Dutt, S and Dyshkant, A and Eads, M and Ebina, K and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Evans, H and Evdokimov, A and Evdokimov, VN and Facini, G and Farrington, S and Feindt, M and Feng, L and Ferbel, T and Fernandez, JP and Ferrazza, C and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Frank, MJ and Franklin, M and Freeman, JC and Fuess, S and Funakoshi, Y and Gallinaro, M and Garcia-Bellido, A and Garcia, JE and García-González, JA and García-Guerra, GA and Garfinkel, AF and Garosi, P and Gavrilov, V and Gay, P and Geng, W and Gerbaudo, D and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev,
             V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Golovanov, G and Gomez-Ceballos, G and Gomez, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Goussiou, A and Grannis, PD and Greder, S and Greenlee,
             H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hagopian, S and Hahn, SR and Haley, J and Halkiadakis, E and Hamaguchi, A and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, D and Hare, M and Harel, A and Harr, RF and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Heck, M and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hewamanage, S and Hildreth,
             MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen,
             B and Hogan, J and Hohlfeld, M and Hopkins, W and Horn, D and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jeong,
             MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere, A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung, AW and Junk, TR and Juste, A and Kaadze, K and Kajfasz, E and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kasper, PA and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava,
             A and Kharzheev, YN and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim,
             YK and Kimura, N and Kirby, M and Kiselevich, I and Klimenko, S and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Krop,
             D and Kruse, M and Krutelyov, V and Kuhr, T and Kulikov, S and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lammers, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lebrun, P and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
             H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Lin,
             C-J and Lindgren, M and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lubatti, HJ and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lysak, R and Lys, J and Maciel, AKA and Madar, R and Madrak,
             R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G},
   Title = {Evidence for a particle produced in association with weak
             bosons and decaying to a bottom-antibottom quark pair in
             higgs boson searches at the tevatron.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {7},
   Pages = {071804},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.109.071804},
   Abstract = {We combine searches by the CDF and D0 Collaborations for the
             associated production of a Higgs boson with a W or Z boson
             and subsequent decay of the Higgs boson to a
             bottom-antibottom quark pair. The data, originating from
             Fermilab Tevatron pp collisions at √s = 1.96 TeV,
             correspond to integrated luminosities of up to 9.7 fb(-1).
             The searches are conducted for a Higgs boson with mass in
             the range 100-150 GeV/c(2). We observe an excess of events
             in the data compared with the background predictions, which
             is most significant in the mass range between 120 and 135
             GeV/c(2). The largest local significance is 3.3 standard
             deviations, corresponding to a global significance of 3.1
             standard deviations. We interpret this as evidence for the
             presence of a new particle consistent with the standard
             model Higgs boson, which is produced in association with a
             weak vector boson and decays to a bottom-antibottom quark
             pair.},
   Doi = {10.1103/physrevlett.109.071804},
   Key = {fds309084}
}

@article{fds309216,
   Author = {Kotwal, AV and Collaboration, CDF},
   Title = {Search for the standard model Higgs boson produced in
             association with a Z boson in 7.9/fb of ppbar collisions at
             sqrt(s)=1.96 TeV using the CDF II detector},
   Journal = {Phys. Lett. B},
   Volume = {715},
   Number = {1-3},
   Pages = {98},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.07.045},
   Abstract = {We present a search for the standard model Higgs boson
             produced in association with a Z boson, using up to 7.9 fb
             -1 of integrated luminosity from pp- collisions collected
             with the CDF II detector. We utilize several novel
             techniques, including multivariate lepton selection,
             multivariate trigger parametrization, and a multi-stage
             signal discriminant consisting of specialized functions
             trained to distinguish individual backgrounds. By increasing
             acceptance and enhancing signal discrimination, these
             techniques have significantly improved the sensitivity of
             the analysis above what was expected from a larger dataset
             alone. We observe no significant evidence for a signal, and
             we set limits on the ZH production cross section. For a
             Higgs boson with mass 115 GeV/c 2, we expect (observe) a
             limit of 3.9 (4.8) times the standard model predicted value,
             at the 95% credibility level. © 2012 Elsevier
             B.V.},
   Doi = {10.1016/j.physletb.2012.07.045},
   Key = {fds309216}
}

@article{fds309114,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Combined search for the Standard Model Higgs boson in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032003},
   Abstract = {A combined search for the Standard Model Higgs boson with
             the ATLAS detector at the LHC is presented. The data sets
             used correspond to integrated luminosities from 4.6fb-1 to
             4.9fb-1 of proton-proton collisions collected at √s=7TeV
             in 2011. The Higgs boson mass ranges of 111.4 GeV to 116.6
             GeV, 119.4 GeV to 122.1 GeV, and 129.2 GeV to 541 GeV are
             excluded at the 95% confidence level, while the range 120
             GeV to 560 GeV is expected to be excluded in the absence of
             a signal. An excess of events is observed at Higgs boson
             mass hypotheses around 126 GeV with a local significance of
             2.9 standard deviations (σ). The global probability for the
             background to produce an excess at least as significant
             anywhere in the entire explored Higgs boson mass range of
             110-600 GeV is estimated to be ∼15%, corresponding to a
             significance of approximately 1σ. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.86.032003},
   Key = {fds309114}
}

@article{fds309184,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwoo-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio, LB and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Search for charged Higgs bosons decaying via H±
             → τν in tt̄ events using pp collision data at √s = 7
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP06(2012)039},
   Abstract = {The results of a search for charged Higgs bosons are
             presented. The analysis is based on 4.6 fb?1 of
             proton-proton collision data at √s = 7TeV collected by the
             ATLAS experiment at the Large Hadron Collider, using top
             quark pair events with a τ lepton in the final state. The
             data are consistent with the expected background from
             Standard Model processes. Assuming that the branching ratio
             of the charged Higgs boson to a τ lepton and a neutrino is
             100%, this leads to upper limits on the branching ratio of
             top quark decays to a b quark and a charged Higgs boson
             between 5% and 1% for charged Higgs boson masses ranging
             from 90GeV to 160GeV, respectively. In the context of the
             mhmaxscenario of the MSSM, tan β above 12-26, as well as
             between 1 and 2-6, can be excluded for charged Higgs boson
             masses between 90GeV and 150GeV. Copyright
             CERN.},
   Doi = {10.1007/JHEP06(2012)039},
   Key = {fds309184}
}

@article{fds309219,
   Author = {Aaltonen, T and Ãlvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Measurement of CP-violation asymmetries in D0→KS0π
             +π -},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032007},
   Abstract = {We report a measurement of time-integrated CP-violation
             asymmetries in the resonant substructure of the three-body
             decay D0→KS0π +π - using CDF II data corresponding to
             6.0fb -1 of integrated luminosity from Tevatron pp̄
             collisions at √s=1.96TeV. The charm mesons used in this
             analysis come from D *+(2010) →D0π + and D *-(2010)→D
             ̄0π -, where the production flavor of the charm meson is
             determined by the charge of the accompanying pion. We apply
             a Dalitz-amplitude analysis for the description of the
             dynamic decay structure and use two complementary
             approaches, namely, a full Dalitz-plot fit employing the
             isobar model for the contributing resonances and a
             model-independent bin-by-bin comparison of the D0 and D ̄0
             Dalitz plots. We find no CP-violation effects and measure an
             asymmetry of A CP=(-0.05±0. 57(stat)±0.54(syst))% for the
             overall integrated CP-violation asymmetry, consistent with
             the standard model prediction. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.032007},
   Key = {fds309219}
}

@article{fds309174,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for supersymmetry with jets, missing transverse
             momentum and at least one hadronically decaying τ lepton in
             proton-proton collisions at s=7TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {714},
   Number = {2-5},
   Pages = {197-214},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {August},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.06.061},
   Abstract = {A search for production of supersymmetric particles in final
             states containing jets, missing transverse momentum, and at
             least one hadronically decaying τ lepton is presented. The
             data were recorded by the ATLAS experiment in s=7TeV
             proton-proton collisions at the Large Hadron Collider. No
             excess above the Standard Model background expectation was
             observed in 2.05fb-1 of data. The results are interpreted in
             the context of gauge mediated supersymmetry breaking models
             with Mmess=250TeV, N5=3, μ>0, and Cgrav=1. The production
             of supersymmetric particles is excluded at 95% C.L. up to a
             supersymmetry breaking scale Λ=30TeV, independent of tanβ,
             and up to Λ=43TeV for large tanβ. © 2012.},
   Doi = {10.1016/j.physletb.2012.06.061},
   Key = {fds309174}
}

@article{fds309195,
   Author = {Aaltonen, T and Albrow, M and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F},
   Title = {Diffractive dijet production in p̄p collisions at
             √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032009},
   Abstract = {We report on a study of diffractive dijet production in p̄p
             collisions at √s=1.96TeV using the CDF II detector at the
             Fermilab Tevatron p̄p collider. A data sample from 310pb -1
             of integrated luminosity collected by triggering on a high
             transverse energy jet, ETjet, in coincidence with a recoil
             antiproton detected in a Roman pot spectrometer is used to
             measure the ratio of single-diffractive to inclusive-dijet
             event rates as a function of xp ̄ of the interacting parton
             in the antiproton, the Bjorken-x, xBjp̄, and a Q2(ETjet)2
             in the ranges 10 -3<xBjp̄<10 -1 and 102<Q2<104GeV2,
             respectively. Results are presented for the region of
             p̄-momentum-loss fraction 0.03<ξ p̄<0.09 and a
             four-momentum transfer squared t p̄>-4GeV2. The t p̄
             dependence is measured as a function of Q2 and xBjp̄ and
             compared with that of inclusive single diffraction
             dissociation. We find weak xBjp̄ and Q2 dependencies in the
             ratio of single diffractive to inclusive event rates, and no
             significant Q2 dependence in the diffractive t p̄
             distributions. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.032009},
   Key = {fds309195}
}

@article{fds309171,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Jet mass and substructure of inclusive jets in √s = 7TeV
             pp collisions with the ATLAS experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP05(2012)128},
   Abstract = {Recent studies have highlighted the potential of jet
             substructure techniques to identify the hadronic decays of
             boosted heavy particles. These studies all rely upon the
             assumption that the internal substructure of jets generated
             by QCD radiation is well understood. In this article, this
             assumption is tested on an inclusive sample of jets recorded
             with the ATLAS detector in 2010, which corresponds to 35 pb
             -1 of pp collisions delivered by the LHC at Rs =
             7TeV.},
   Doi = {10.1007/JHEP05(2012)128},
   Key = {fds309171}
}

@article{fds309214,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Search for the standard model Higgs boson produced in
             association with a W ± boson with 7.5fb
             -1 integrated luminosity at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.032011},
   Abstract = {We present a search for the standard model Higgs boson
             produced in association with a W ± boson. This search uses
             data corresponding to an integrated luminosity of 7.5fb -1
             collected by the CDF detector at the Tevatron. We select
             WH→νbb̄ candidate events with two jets, large missing
             transverse energy, and exactly one charged lepton. We
             further require that at least one jet be identified to
             originate from a bottom quark. Discrimination between the
             signal and the large background is achieved through the use
             of a Bayesian artificial neural network. The number of
             tagged events and their distributions are consistent with
             the standard model expectations. We observe no evidence for
             a Higgs boson signal and set 95% C.L. upper limits on the WH
             production cross section times the branching ratio to decay
             to bb̄ pairs, σ(pp̄→W ±H) ×B(H→bb̄), relative to
             the rate predicted by the standard model. For the Higgs
             boson mass range of 100 to 150GeV/c2 we set observed
             (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For
             115GeV/c2 the upper limit is 3.64 (2.78). The combination of
             the present search with an independent analysis that selects
             events with three jets yields more stringent limits ranging
             from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For
             115 and 125GeV/c2 the upper limits are 2.65 (2.60) and 4.36
             (3.69), respectively. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.032011},
   Key = {fds309214}
}

@article{fds309205,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Measurement of the WZ cross section and triple gauge
             couplings in pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.031104},
   Abstract = {This article describes the current most precise measurement
             of the WZ production cross section as well as limits on
             anomalous WWZ couplings at a center-of-mass energy of 1.96
             TeV in proton-antiproton collisions for the Collider
             Detector at Fermilab (CDF). WZ candidates are reconstructed
             from decays containing three charged leptons and missing
             energy from a neutrino, where the charged leptons are either
             electrons or muons. Using data collected by the CDF II
             detector (7.1fb -1 of integrated luminosity), 63 candidate
             events are observed with the expected background
             contributing 8±1 events. The measured total cross section
             σ(pp̄→WZ)=3.93-0.53+0.60(stat)-0. 46+0.59(syst)pb is in
             good agreement with the standard model prediction of
             3.50±0.21. The same sample is used to set limits on
             anomalous WWZ couplings. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.031104},
   Key = {fds309205}
}

@article{fds309078,
   Author = {Kotwal, AV and Collaboration, CDF},
   Title = {Search for the standard model Higgs boson decaying to a
             b-bbar pair in events with two oppositely charged leptons
             using the full CDF data set},
   Journal = {Phys. Rev. Lett.},
   Volume = {109},
   Number = {11},
   Pages = {111803},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111803},
   Abstract = {We present a search for the standard model Higgs boson
             produced in association with a Z boson in data collected
             with the CDF II detector at the Tevatron, corresponding to
             an integrated luminosity of 9.45  fb(-1). In events
             consistent with the decay of the Higgs boson to a
             bottom-quark pair and the Z boson to electron or muon pairs,
             we set 95% credibility level upper limits on the ZH
             production cross section times the H→bb branching ratio as
             a function of Higgs boson mass. At a Higgs boson mass of
             125  GeV/c(2), we observe (expect) a limit of 7.1 (3.9)
             times the standard model value.},
   Doi = {10.1103/physrevlett.109.111803},
   Key = {fds309078}
}

@article{fds309079,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
             ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
             A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
             P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
             S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jindariani, S and Jones,
             M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi,
             A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for the standard model Higgs boson decaying to a bb
             pair in events with one charged lepton and large missing
             transverse energy using the full CDF data
             set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {11},
   Pages = {111804},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111804},
   Abstract = {We present a search for the standard model Higgs boson
             produced in association with a W boson in
             sqrt[s]=1.96  TeV pp collision data collected with the
             CDF II detector at the Tevatron corresponding to an
             integrated luminosity of 9.45  fb(-1). In events
             consistent with the decay of the Higgs boson to a
             bottom-quark pair and the W boson to an electron or muon and
             a neutrino, we set 95% credibility level upper limits on the
             WH production cross section times the H→bb branching ratio
             as a function of Higgs boson mass. At a Higgs boson mass of
             125  GeV/c(2), we observe (expect) a limit of 4.9 (2.8)
             times the standard model value.},
   Doi = {10.1103/physrevlett.109.111804},
   Key = {fds309079}
}

@article{fds309080,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
             A and Artoni, G},
   Title = {A search for flavour changing neutral currents in top-quark
             decays in pp collision data collected with the ATLAS
             detector at √s = 7 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {9},
   Pages = {1-36},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2012)139},
   Abstract = {A search for flavour changing neutral current (FCNC)
             processes in top-quark decays by the ATLAS Collaboration is
             presented. Data collected from pp collisions at the LHC at a
             centre-of-mass energy of √s = 7 TeV during 2011,
             corresponding to an integrated luminosity of 2.1 fb-1, were
             used. A search was performed for top-quark pair-production
             events, with one top quark decaying through the t → Zq
             FCNC (q = u, c) channel, and the other through the Standard
             Model dominant mode t → Wb. Only the decays of the Z boson
             to charged leptons and leptonic W-boson decays were
             considered as signal. Consequently, the final-state topology
             is characterised by the presence of three isolated charged
             leptons, at least two jets and missing transverse momentum
             from the undetected neutrino. No evidence for an FCNC signal
             was found. An upper limit on the t → Zq branching ratio of
             BR(t → Zq) < 0.73% is set at the 95% confidence level.
             Copyright CERN.},
   Doi = {10.1007/JHEP09(2012)139},
   Key = {fds309080}
}

@article{fds310552,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
             ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
             A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
             P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
             S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
             JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
             S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jindariani, S and Jones,
             M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi,
             A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Tipton, P and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
             AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Combined search for the standard model Higgs boson decaying
             to a bb pair using the full CDF data set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {11},
   Pages = {111802},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111802},
   Abstract = {We combine the results of searches for the standard model
             (SM) Higgs boson based on the full CDF Run II data set
             obtained from sqrt[s]=1.96  TeV pp collisions at the
             Fermilab Tevatron corresponding to an integrated luminosity
             of 9.45  fb(-1). The searches are conducted for Higgs
             bosons that are produced in association with a W or Z boson,
             have masses in the range 90-150  GeV/c(2), and decay
             into bb pairs. An excess of data is present that is
             inconsistent with the background prediction at the level of
             2.5 standard deviations (the most significant local excess
             is 2.7 standard deviations).},
   Doi = {10.1103/physrevlett.109.111802},
   Key = {fds310552}
}

@article{fds309207,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the difference in CP-violating asymmetries in
             D(0)→K(+)K(-) and D(0)→π(+)π(-) decays at
             CDF.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {11},
   Pages = {111801},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111801},
   Abstract = {We report a measurement of the difference (ΔA(CP)) between
             time-integrated CP-violating asymmetries in D(0)→K(+)K(-)
             and D(0)→π(+)π(-) decays reconstructed in the full data
             set of proton-antiproton collisions collected by the
             Collider Detector at Fermilab, corresponding to
             9.7  fb(-1) of integrated luminosity. The strong decay
             D(*+)→D(0)π(+) is used to identify the charm meson at
             production as D(0) or D[over ¯](0). We measure
             ΔA(CP)=[-0.62±0.21(stat)±0.10(syst)]%, which differs from
             zero by 2.7 Gaussian standard deviations. This result
             supports similar evidence for CP violation in charm-quark
             decays obtained in proton-proton collisions.},
   Doi = {10.1103/physrevlett.109.111801},
   Key = {fds309207}
}

@article{fds310551,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
             ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
             A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
             P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
             S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest,
             R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic,
             I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for the standard model Higgs boson decaying to a bb
             pair in events with no charged leptons and large missing
             transverse energy using the full CDF data
             set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {11},
   Pages = {111805},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.109.111805},
   Abstract = {We report on a search for the standard model Higgs boson
             produced in association with a vector boson in the full data
             set of proton-antiproton collisions at sqrt[s]=1.96  TeV
             recorded by the CDF II detector at the Tevatron,
             corresponding to an integrated luminosity of
             9.45  fb(-1). We consider events having no identified
             charged lepton, a transverse energy imbalance, and two or
             three jets, of which at least one is consistent with
             originating from the decay of a b quark. We place 95%
             credibility level upper limits on the production cross
             section times standard model branching fraction for several
             mass hypotheses between 90 and 150  GeV/c(2). For a
             Higgs boson mass of 125  GeV/c(2), the observed
             (expected) limit is 6.7 (3.6) times the standard model
             prediction.},
   Doi = {10.1103/physrevlett.109.111805},
   Key = {fds310551}
}

@article{fds309176,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Search for second generation scalar leptoquarks in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {9},
   Pages = {1-21},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2151-6},
   Abstract = {The results of a search for the production of second
             generation scalar leptoquarks are presented for final states
             consisting of either two muons and at least two jets or a
             muon plus missing transverse momentum and at least two jets.
             A total of 1.03 fb<sup>−1</sup> integrated luminosity of
             protonproton collision data produced by the Large Hadron
             Collider at √s = 7 TeV and recorded by the ATLAS detector
             is used for the search. The event yields in the signal
             regions are found to be consistent with the Standard Model
             background expectations. The production of second generation
             leptoquarks is excluded for a leptoquark mass m<inf>LQ</inf>
             < 594 (685) GeV at 95 % confidence level, for a branching
             ratio of 0.5 (1.0) for leptoquark decay to a muon and a
             quark.},
   Doi = {10.1140/epjc/s10052-012-2151-6},
   Key = {fds309176}
}

@article{fds309131,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
             H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the azimuthal ordering of charged hadrons
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.052005},
   Abstract = {This paper presents a study of the possible ordering of
             charged hadrons in the azimuthal angle relative to the beam
             axis in high-energy proton-proton collisions at the Large
             Hadron Collider (LHC). A spectral analysis of correlations
             between longitudinal and transverse components of the
             momentum of the charged hadrons, driven by the search for
             phenomena related to the structure of the QCD field, is
             performed. Data were recorded with the ATLAS detector at
             center-of-mass energies of √s=900GeV and √s=7TeV. The
             correlations measured in a kinematic region dominated by
             low-pT particles are not well described by conventional
             models of hadron production. The measured spectra show
             features consistent with the fragmentation of a QCD string
             represented by a helixlike ordered gluon chain. © 2012
             CERN.},
   Doi = {10.1103/PhysRevD.86.052005},
   Key = {fds309131}
}

@article{fds309113,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and A°kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Observation of a new particle in the search for the Standard
             Model Higgs boson with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {1-29},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.020},
   Abstract = {A search for the Standard Model Higgs boson in proton-proton
             collisions with the ATLAS detector at the LHC is presented.
             The datasets used correspond to integrated luminosities of
             approximately 4.8 fb -1 collected at s=7 TeV in 2011 and 5.8
             fb -1 at s=8 TeV in 2012. Individual searches in the
             channels H→ZZ (*) →4ℓ, H→γγ and H→WW (*)
             →eνμν in the 8 TeV data are combined with previously
             published results of searches for H→ZZ (*) , WW (*) , bb-
             and τ + τ - in the 7 TeV data and results from improved
             analyses of the H→ZZ (*) →4ℓ and H→γγ channels in
             the 7 TeV data. Clear evidence for the production of a
             neutral boson with a measured mass of 126.0±0.4(stat)±0.4(sys)GeV
             is presented. This observation, which has a significance of
             5.9 standard deviations, corresponding to a background
             fluctuation probability of 1.7×10 -9 , is compatible with
             the production and decay of the Standard Model Higgs boson.
             © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.08.020},
   Key = {fds309113}
}

@article{fds309189,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Evidence for the associated production of a W boson and a
             top quark in ATLAS at √s=7TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {716},
   Number = {1},
   Pages = {142-159},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.011},
   Abstract = {This Letter presents evidence for the associated production
             of a W boson and a top quark using 2.05 fb−1 of pp
             collision data at s=7TeV accumulated with the ATLAS detector
             at the LHC. The analysis is based on the selection of the
             dileptonic final states with events featuring two isolated
             leptons, electron or muon, with significant transverse
             missing momentum and at least one jet. An approach based on
             boosted decision trees has been developed to improve the
             discrimination of single top-quark Wt events from
             background. A template fit to the final classifier
             distributions is performed to determine the cross-section.
             The result is incompatible with the background-only
             hypothesis at the 3.3σ level, the expected sensitivity
             assuming the Standard Model production rate being 3.4σ. The
             corresponding cross-section is determined and found to be
             σWt=16.8±2.9 (stat)±4.9 (syst) pb, in good agreement with
             the Standard Model expectation. From this result the CKM
             matrix element |Vtb|=1.03−0.19+0.16 is derived assuming
             that the Wt production through |Vts| and |Vtd| is
             small.},
   Doi = {10.1016/j.physletb.2012.08.011},
   Key = {fds309189}
}

@article{fds309206,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Transverse momentum cross section of e +e
             - pairs in the Z-boson region from pp̄
             collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.052010},
   Abstract = {The transverse momentum cross section of e +e - pairs in the
             Z-boson mass region of 66-116GeV/c2 is precisely measured
             using Run II data corresponding to 2.1fb -1 of integrated
             luminosity recorded by the Collider Detector at Fermilab.
             The cross section is compared with two quantum chromodynamic
             calculations. One is a fixed-order perturbative calculation
             at O(αs2), and the other combines perturbative predictions
             at high transverse momentum with the gluon resummation
             formalism at low transverse momentum. Comparisons of the
             measurement with calculations show reasonable agreement. The
             measurement is of sufficient precision to allow refinements
             in the understanding of the transverse momentum
             distribution. © 2012 American Physical Society.},
   Doi = {10.1103/PhysRevD.86.052010},
   Key = {fds309206}
}

@article{fds309072,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grillo, L and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
             M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the bottom-strange meson mixing phase in the
             full CDF data set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {17},
   Pages = {171802},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.109.171802},
   Abstract = {We report a measurement of the bottom-strange meson mixing
             phase β(s) using the time evolution of B(s)(0)→J/ψ(→μ(+)μ(-))φ(→K(+)K(-))
             decays in which the quark-flavor content of the
             bottom-strange meson is identified at production. This
             measurement uses the full data set of proton-antiproton
             collisions at √s=1.96 TeV collected by the Collider
             Detector experiment at the Fermilab Tevatron, corresponding
             to 9.6 fb(-1) of integrated luminosity. We report confidence
             regions in the two-dimensional space of β(s) and the
             B(s)(0) decay-width difference ΔΓ(s) and measure
             β(s)∈[-π/2,-1.51]∪[-0.06,0.30]∪[1.26,π/2] at the
             68% confidence level, in agreement with the standard model
             expectation. Assuming the standard model value of β(s), we
             also determine ΔΓ(s)=0.068±0.026(stat)±0.009(syst)
             ps(-1) and the mean B(s)(0) lifetime τ(s)=1.528±0.019(stat)±0.009(syst)
             ps, which are consistent and competitive with determinations
             by other experiments.},
   Doi = {10.1103/physrevlett.109.171802},
   Key = {fds309072}
}

@article{fds309075,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Precision top-quark mass measurement at CDF.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {15},
   Pages = {152003},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.109.152003},
   Abstract = {We present a precision measurement of the top-quark mass
             using the full sample of Tevatron √s = 1.96 TeV
             proton-antiproton collisions collected by the CDF II
             detector, corresponding to an integrated luminosity of 8.7
             fb(-1). Using a sample of tt¯ candidate events decaying
             into the lepton+jets channel, we obtain distributions of the
             top-quark masses and the invariant mass of two jets from the
             W boson decays from data. We then compare these
             distributions to templates derived from signal and
             background samples to extract the top-quark mass and the
             energy scale of the calorimeter jets with in situ
             calibration. The likelihood fit of the templates from signal
             and background events to the data yields the single
             most-precise measurement of the top-quark mass,
             M(top)=172.85±0.71(stat)±0.85(syst) GeV/c(2).},
   Doi = {10.1103/physrevlett.109.152003},
   Key = {fds309075}
}

@article{fds309076,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
             N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Measurement of W±Z production in proton-proton
             collisions At √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2173-0},
   Abstract = {A study of W ± Z production in proton-proton collisions at
             √s = 7 TeV is presented using data corresponding to an
             integrated luminosity of 4.6 fb−1 collected with the ATLAS
             detector at the Large Hadron Collider in 2011. In total, 317
             candidates, with a background expectation of 68 ± 10
             events, are observed in double-leptonic decay final states
             with electrons, muons and missing transverse momentum. The
             total cross-section is determined to be be σtotWZ =
             19.0+1.4−1.3 (stat.) ± 0.9(syst.) ± 0.4(lumi.) pb,
             consistent with the Standard Model expectation of
             17.6+1.1−1.0 pb. Limits on anomalous triple gauge boson
             couplings are derived using the transverse momentum spectrum
             of Z bosons in the selected events. The cross-section is
             also presented as a function of Z boson transverse momentum
             and diboson invariant mass.},
   Doi = {10.1140/epjc/s10052-012-2173-0},
   Key = {fds309076}
}

@article{fds309077,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for top and bottom squarks from gluino pair
             production in final states with missing transverse energy
             and at least three b-jets with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2174-z},
   Abstract = {This letter reports the results of a search for top and
             bottom squarks from gluino pair production in 4.7 fb−1of
             pp collisions at √s = 7 TeV using the ATLAS detector at
             the LHC. The search is performed in events with large
             missing transverse momentum and at least three jets
             identified as originating from a b-quark. Exclusion limits
             are presented for a variety of gluino-mediated models with
             gluino masses up to 1 TeV excluded.},
   Doi = {10.1140/epjc/s10052-012-2174-z},
   Key = {fds309077}
}

@article{fds309192,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Underlying event characteristics and their dependence on jet
             size of charged-particle jet events in pp collisions at
             √(s)=7TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.072004},
   Abstract = {Distributions sensitive to the underlying event are studied
             in events containing one or more charged-particle jets
             produced in pp collisions at √s=7TeV with the ATLAS
             detector at the Large Hadron Collider (LHC). These
             measurements reflect 800μb-1 of data taken during 2010.
             Jets are reconstructed using the anti-kt algorithm with
             radius parameter R varying between 0.2 and 1.0.
             Distributions of the charged-particle multiplicity, the
             scalar sum of the transverse momentum of charged particles,
             and the average charged-particle pT are measured as
             functions of pTjet in regions transverse to and opposite the
             leading jet for 4GeV<pTjet<100GeV. In addition, the R
             dependence of the mean values of these observables is
             studied. In the transverse region, both the multiplicity and
             the scalar sum of the transverse momentum at fixed pTjet
             vary significantly with R, while the average
             charged-particle transverse momentum has a minimal
             dependence on R. Predictions from several Monte Carlo tunes
             have been compared to the data; the predictions from Pythia
             6, based on tunes that have been determined using LHC data,
             show reasonable agreement with the data, including the
             dependence on R. Comparisons with other generators indicate
             that additional tuning of soft-QCD parameters is necessary
             for these generators. The measurements presented here
             provide a testing ground for further development of the
             Monte Carlo models. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.86.072004},
   Key = {fds309192}
}

@article{fds309193,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {ATLAS measurements of the properties of jets for boosted
             particle searches},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.072006},
   Abstract = {Measurements are presented of the properties of high
             transverse momentum jets, produced in proton-proton
             collisions at a center-of-mass energy of √s=7TeV. The data
             correspond to an integrated luminosity of 35pb -1 and were
             collected with the ATLAS detector in 2010. Jet mass, width,
             eccentricity, planar flow and angularity are measured for
             jets reconstructed using the anti-kt algorithm with distance
             parameters R=0.6 and 1.0, with transverse momentum pT>300GeV
             and pseudorapidity |η|<2. The measurements are compared to
             the expectations of Monte Carlo generators that match
             leading-logarithmic parton showers to leading-order, or
             next-to-leading-order, matrix elements. The generators
             describe the general features of the jets, although
             discrepancies are observed in some distributions. © 2012
             CERN, for the ATLAS Collaboration Published by the American
             Physical Society under the terms of the http://creativecommons.
             org/licenses/by/3.0/ Creative Commons Attribution 3.0
             License. Further distribution of this work must maintain
             attribution to the author(s) and the published article's
             title, journal citation, and DOI.},
   Doi = {10.1103/PhysRevD.86.072006},
   Key = {fds309193}
}

@article{fds309074,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M},
   Title = {Search for a Higgs boson in the diphoton final state using
             the full CDF data set from pp collisions at
             s=1.96TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {173-181},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.08.051},
   Abstract = {A search for a narrow Higgs boson resonance in the diphoton
             mass spectrum is presented based on data corresponding to
             10fb -1 of integrated luminosity collected by the CDF
             experiment from proton-antiproton collisions at s=1.96TeV.
             To increase the sensitivity of the search, we employ a
             multivariate discriminant technique for the first time in
             this channel at CDF. No evidence of signal is observed, and
             upper limits are set on the cross section times branching
             ratio of the resonant state as a function of the Higgs boson
             mass. The limits are interpreted in the context of the
             standard model with an expected (observed) limit on the
             cross section times branching ratio of 9.9 (17.0) times the
             standard model prediction at the 95% credibility level for a
             Higgs boson mass of 125GeV/c 2. Moreover, a Higgs boson with
             suppressed couplings to fermions is excluded for masses
             below 114GeV/c 2 at the 95% credibility level. © 2012
             Elsevier B.V.},
   Doi = {10.1016/j.physletb.2012.08.051},
   Key = {fds309074}
}

@article{fds309188,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Measurement of Wγ and Zγ production cross sections in pp
             collisions at √s=7 TeV and limits on anomalous triple
             gauge couplings with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {49-69},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.017},
   Abstract = {This Letter presents measurements of l±νγ and l+l−γ
             (l=e,μ) production in 1.02 fb−1 of pp collision data
             recorded at s=7 TeV with the ATLAS detector at the LHC in
             the first half of 2011. Events dominated by Wγ and Zγ
             production with leptonic decays of the W and Z bosons are
             selected, and their production cross sections and kinematic
             properties are measured in several ranges of the photon
             transverse energy. The results are compared to Standard
             Model predictions and are used to determine limits on
             anomalous WWγ and ZZγ/Zγγ couplings.},
   Doi = {10.1016/j.physletb.2012.09.017},
   Key = {fds309188}
}

@article{fds309190,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D},
   Title = {Search for a standard model Higgs boson in the
             H→ZZ→ℓ+νν¯ decay
             channel using 4.7 fb−1 of √s=7 TeV data with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {1-3},
   Pages = {29-48},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.016},
   Abstract = {A search for a Standard Model Higgs boson decaying via
             H→ZZ→ℓ+ℓ−νν¯ where ℓ represents electrons or
             muons, is presented. It is based on proton-proton collision
             data at s=7 TeV, collected by the ATLAS experiment at the
             LHC during 2011 and corresponding to an integrated
             luminosity of 4.7 fb−1. The data agree with the expected
             Standard Model backgrounds. Upper limits on the Higgs boson
             production cross section are derived for Higgs boson masses
             between 200 GeV and 600 GeV and the production of a Standard
             Model Higgs boson with a mass in the range 319–558 GeV is
             excluded at the 95% confidence level.},
   Doi = {10.1016/j.physletb.2012.09.016},
   Key = {fds309190}
}

@article{fds310550,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d’Ascenzo, N and Datta, M and de
             Barbaro, P and Dell’Orso, M and Demortier, L and Deninno, M and Devoto, F and d’Errico, M},
   Title = {Search for scalar top quark production in (Formula
             presented.) collisions at (Formula presented.) = 1.96
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2012)158},
   Abstract = {We report on a search for the supersymmetric partner of the
             top quark (scalar top) decaying into a charm quark and a
             neutralino in (Formula presented.) collisions at (Formula
             presented.) = 1.96TeV. The data sample, collected by the CDF
             II detector at the Fermilab Tevatron, corresponds to an
             integrated luminosity of 2.6 fb<sup>−1</sup>. Candidate
             events are selected by requiring two or more jets and a
             large imbalance in the transverse momentum. To enhance the
             analysis sensitivity, at least one of the jets is required
             to be identified as originating from a charm quark using an
             algorithm specifically designed for this analysis. The
             selected events are in good agreement with standard model
             predictions. In the case of large mass splitting between the
             scalar top quark and the neutralino we exclude a scalar top
             quark mass below 180 GeV/c<sup>2</sup> at 95% confidence
             level.},
   Doi = {10.1007/JHEP10(2012)158},
   Key = {fds310550}
}

@article{fds309071,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'errico, M},
   Title = {Novel inclusive search for the Higgs boson in the
             four-lepton final state at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {7},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.072012},
   Abstract = {An inclusive search for the standard model Higgs boson using
             the four-lepton final state in proton-antiproton collisions
             produced by the Tevatron at √s=1.96TeV is conducted. The
             data are recorded by the CDF II detector and correspond to
             an integrated luminosity of 9.7fb -1. Three distinct Higgs
             decay modes, namely ZZ, WW, and ττ, are simultaneously
             probed. Nine potential signal events are selected and found
             to be consistent with the background expectation. We set a
             95% credibility limit on the production cross section times
             the branching ratio and subsequent decay to the four-lepton
             final state for hypothetical Higgs boson masses between
             120GeV/c2 and 300GeV/c2. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.072012},
   Key = {fds309071}
}

@article{fds309172,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
             AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
             OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ},
   Title = {Measurement of the t-channel single top-quark production
             cross section in pp collisions at s=7 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {717},
   Number = {4-5},
   Pages = {330-350},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.09.031},
   Abstract = {We report a measurement of the cross section of single
             top-quark production in the t-channel using 1.04 fb−1 of
             pp collision data at s=7 TeV recorded with the ATLAS
             detector at the LHC. Selected events feature one electron or
             muon, missing transverse momentum, and two or three jets,
             exactly one of them identified as originating from a b
             quark. The cross section is measured by fitting the
             distribution of a multivariate discriminant constructed with
             a neural network, yielding σt=83±4(stat.)−19+20(syst.)
             pb, which is in good agreement with the prediction of the
             Standard Model. Using the ratio of the measured to the
             theoretically predicted cross section and assuming that the
             top-quark-related CKM matrix elements obey the relation
             |Vtb|≫|Vts|,|Vtd|, the coupling strength at the W-t-b
             vertex is determined to be |Vtb|=1.13−0.13+0.14. If it is
             assumed that |Vtb|⩽1 a lower limit of |Vtb|>0.75 is
             obtained at the 95% confidence level.},
   Doi = {10.1016/j.physletb.2012.09.031},
   Key = {fds309172}
}

@article{fds309058,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer,
             F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
             J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for a supersymmetric partner to the top quark in
             final states with jets and missing transverse momentum at
             sqrt[s] = 7 TeV with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {21},
   Pages = {211802},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.109.211802},
   Abstract = {A search for direct pair production of supersymmetric top
             squarks (t(1)) is presented, assuming the t(1) decays into a
             top quark and the lightest supersymmetric particle,
             χ(1)(0), and that both top quarks decay to purely hadronic
             final states. A total of 16 (4) events are observed compared
             to a predicted standard model background of
             13.5(-3.6)(+3.7)(4.4(-1.3)(+1.7)) events in two signal
             regions based on ∫Ldt = 4.7 fb(-1) of pp collision data
             taken at sqrt[s] = 7 TeV with the ATLAS detector at the LHC.
             An exclusion region in the t(1) versus χ(1)(0) mass plane
             is evaluated: 370<m(t)(1)}<465 GeV is excluded for
             m(χ)(1)(0) ~ 0 GeV while m(t)(1) = 445 GeV is excluded for
             m(χ)(1)(0) ≤ 50 GeV.},
   Doi = {10.1103/physrevlett.109.211802},
   Key = {fds309058}
}

@article{fds309059,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, AD and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
             R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
             A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for direct top squark pair production in final states
             with one isolated lepton, jets, and missing transverse
             momentum in sqrt[s] = 7 TeV pp collisions using 4.7 fb(-10
             of ATLAS data.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {21},
   Pages = {211803},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.109.211803},
   Abstract = {A search is presented for direct top squark pair production
             in final states with one isolated electron or muon, jets,
             and missing transverse momentum in proton-proton collisions
             at sqrt[s] = 7 TeV. The measurement is based on 4.7 fb(-1)
             of data collected with the ATLAS detector at the LHC. Each
             top squark is assumed to decay to a top quark and the
             lightest supersymmetric particle (LSP). The data are found
             to be consistent with standard model expectations. Top
             squark masses between 230 GeV and 440 GeV are excluded with
             95% confidence for massless LSPs, and top squark masses
             around 400 GeV are excluded for LSP masses up to 125
             GeV.},
   Doi = {10.1103/physrevlett.109.211803},
   Key = {fds309059}
}

@article{fds309060,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Measurements of the top-quark mass and the tt cross section
             in the hadronic τ+jets decay channel at sqrt[s] = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {19},
   Pages = {192001},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.109.192001},
   Abstract = {We present the first direct measurement of the top-quark
             mass using tt events decaying in the hadronic τ+jets decay
             channel. Using data corresponding to an integrated
             luminosity of 2.2 fb(-1) collected by the CDF II detector in
             pp collisions at sqrt[s] = 1.96 TeV at the Fermilab
             Tevatron, we measure the tt cross section, σ(tt), and the
             top-quark mass, M(top). We extract M(top) from a likelihood
             based on per-event probabilities calculated with
             leading-order signal and background matrix elements. We
             measure σ(tt) = 8.8 ± 3.3(stat) ± 2.2(syst) pb and M(top)
             = 172.7 ± 9.3(stat) ± 3.7(syst) GeV/c(2).},
   Doi = {10.1103/physrevlett.109.192001},
   Key = {fds309060}
}

@article{fds309064,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Connors, J and Convery, ME and Conway,
             J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
             M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
             B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
             P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
             A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
             E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
             X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
             YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
             C and Zucchelli, S and CDF Collaboration},
   Title = {Search for the standard model Higgs Boson produced in
             association with top quarks using the full CDF data
             set.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {18},
   Pages = {181802},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.109.181802},
   Abstract = {A search is presented for the standard model Higgs boson
             produced in association with top quarks using the full Run
             II proton-antiproton collision data set, corresponding to
             9.45 fb(-1), collected by the Collider Detector at Fermilab.
             No significant excess over the expected background is
             observed, and 95% credibility-level upper bounds are placed
             on the cross section σ(ttH → lepton + missing transverse
             energy+jets). For a Higgs boson mass of 125 GeV/c(2), we
             expect to set a limit of 12.6 and observe a limit of 20.5
             times the standard model rate. This represents the most
             sensitive search for a standard model Higgs boson in this
             channel to date.},
   Doi = {10.1103/physrevlett.109.181802},
   Key = {fds309064}
}

@article{fds309070,
   Author = {Mu2e collaboration},
   Title = {Mu2e Conceptual Design Report},
   Journal = {arXiv:1211.7019},
   Year = {2012},
   Month = {November},
   Key = {fds309070}
}

@article{fds310549,
   Author = {Collaboration, AVKWATLAS},
   Title = {Search for high-mass resonances decaying to dilepton final
             states in pp collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {JHEP},
   Volume = {11},
   Number = {11},
   Pages = {138},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2012)138},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for highmass resonances decaying to an
             electron-positron pair or a muon-antimuon pair. The search
             is sensitive to heavy neutral Z′ gauge bosons,
             Randall-Sundrum gravitons, Z* bosons, techni-mesons,
             Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion
             models. Results are presented based on an analysis of pp
             collisions at a center-of-mass energy of 7 TeV corresponding
             to an integrated luminosity of 4.9 fb-1 in the e +e- channel
             and 5.0 fb-1 in the μ+μ- channel. A Z′ boson with
             Standard Model-like couplings is excluded at 95% confidence
             level for masses below 2.22 TeV. A Randall-Sundrum graviton
             with coupling k /M̄Pl = 0.1 is excluded at 95% confidence
             level for masses below 2.16 TeV. Limits on the other models
             are also presented, including Technicolor and Minimal Z′
             Models. Copyright CERN.},
   Doi = {10.1007/JHEP11(2012)138},
   Key = {fds310549}
}

@article{fds309063,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Further search for supersymmetry at √s=7TeV in final
             states with jets, missing transverse momentum, and isolated
             leptons with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.092002},
   Abstract = {This work presents a new inclusive search for supersymmetry
             (SUSY) by the ATLAS experiment at the LHC in proton-proton
             collisions at a center-of-mass energy √s=7TeV in final
             states with jets, missing transverse momentum and one or
             more isolated electrons and/or muons. The search is based on
             data from the full 2011 data-taking period, corresponding to
             an integrated luminosity of 4.7fb-1. Single-lepton and
             multilepton channels are treated together in one analysis.
             An increase in sensitivity is obtained by simultaneously
             fitting the number of events in statistically independent
             signal regions, and the shapes of distributions within those
             regions. A dedicated signal region is introduced to be
             sensitive to decay cascades of SUSY particles with small
             mass differences ("compressed SUSY"). Background
             uncertainties are constrained by fitting to the
             jet-multiplicity distribution in background control regions.
             Observations are consistent with Standard Model
             expectations, and limits are set or extended on a number of
             SUSY models. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.86.092002},
   Key = {fds309063}
}

@article{fds309087,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
             S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori,
             L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett,
             K},
   Title = {Combination of the top-quark mass measurements from the
             Tevatron collider},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Pages = {092003},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.092003},
   Abstract = {The top quark is the heaviest known elementary particle,
             with a mass about 40 times larger than the mass of its
             isospin partner, the bottom quark. It decays almost 100% of
             the time to a W boson and a bottom quark. Using top-antitop
             pairs at the Tevatron proton-antiproton collider, the CDF
             and D0 Collaborations have measured the top quark's mass in
             different final states for integrated luminosities of up to
             5.8fb-1. This paper reports on a combination of these
             measurements that results in a more precise value of the
             mass than any individual decay channel can provide. It
             describes the treatment of the systematic uncertainties and
             their correlations. The mass value determined is
             173.18±0.56(stat)±0.75(syst)GeV or 173.18±0.94GeV, which
             has a precision of ±0.54%, making this the most precise
             determination of the top-quark mass. © 2012 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.86.092003},
   Key = {fds309087}
}

@article{fds309062,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Lvarez
             González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
             S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
             JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
             SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
             M and Buescher, V and Bunichev, V and Burdin, S},
   Title = {Search for neutral Higgs bosons in events with multiple
             bottom quarks at the Tevatron},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.091101},
   Abstract = {The combination of searches performed by the CDF and D0
             collaborations at the Fermilab Tevatron Collider for neutral
             Higgs bosons produced in association with b quarks is
             reported. The data, corresponding to 2.6fb -1 of integrated
             luminosity at CDF and 5.2fb -1 at D0, have been collected in
             final states containing three or more b jets. Upper limits
             are set on the cross section multiplied by the branching
             ratio varying between 44 pb and 0.7 pb in the Higgs boson
             mass range 90 to 300 GeV, assuming production of a narrow
             scalar boson. Significant enhancements to the production of
             Higgs bosons can be found in theories beyond the standard
             model, for example, in supersymmetry. The results are
             interpreted as upper limits in the parameter space of the
             minimal supersymmetric standard model in a benchmark
             scenario favoring this decay mode. © 2012 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.86.091101},
   Key = {fds309062}
}

@article{fds309061,
   Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Erratum: Novel inclusive search for the Higgs boson in the
             four-lepton final state at CDF (Physical Review D (2012) 86
             (072012) DOI:10.1103/PhysRevD. 86.072012)},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.099902},
   Doi = {10.1103/PhysRevD.86.099902},
   Key = {fds309061}
}

@article{fds309067,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Saavedra, JAA and Agustoni, M and Aharrouche,
             M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Spiers, SEA and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik,
             E},
   Title = {Search for supersymmetry in events with large missing
             transverse momentum, jets, and at least one tau lepton in 7
             TeV proton-proton collision data with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2215-7},
   Abstract = {A search for supersymmetry (SUSY) in events with large
             missing transverse momentum, jets, and at least one
             hadronically decaying τ lepton, with zero or one additional
             light lepton (e/μ), has been performed using 4.7 fb−1of
             proton-proton collision data at √s = 7 TeV recorded with
             the ATLAS detector at the Large Hadron Collider. No excess
             above the Standard Model background expectation is observed
             and a 95 % confidence level visible cross-section upper
             limit for new phenomena is set. In the framework of
             gauge-mediated SUSY-breaking models, lower limits on the
             mass scale Λ are set at 54 TeV in the regions where the
             τ1is the next-to-lightest SUSY particle (tanβ > 20). These
             limits provide the most stringent tests to date of GMSB
             models in a large part of the parameter space
             considered.},
   Doi = {10.1140/epjc/s10052-012-2215-7},
   Key = {fds309067}
}

@article{fds309068,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G},
   Title = {Measurement of event shapes at large momentum transfer with
             the ATLAS detector in pp collisions at √s =7
             TeV},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2211-y},
   Abstract = {A measurement of event shape variables is presented for
             large momentum transfer proton-proton collisions using the
             ATLAS detector at the Large Hadron Collider. Six event shape
             variables calculated using hadronic jets are studied in
             inclusive multi-jet events in 35 pb<sup>-1</sup> of
             integrated luminosity at a center-of-mass energy of √s = 7
             TeV. These measurements are compared to predictions by three
             Monte Carlo event generators containing leading-logarithmic
             parton showers matched to leading order matrix elements for
             2→2 and 2→n (n = 2, …, 6) scattering. Measurements of
             the third-jet resolution parameter, aplanarity, thrust,
             sphericity, and transverse sphericity are generally well
             described. The mean value of each event shape variable is
             evaluated as a function of the average momentum of the two
             leading jets p<inf>T,1</inf> and p<inf>T,2</inf>, with a
             mean pT approaching 1 TeV.},
   Doi = {10.1140/epjc/s10052-012-2211-y},
   Key = {fds309068}
}

@article{fds309057,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ},
   Title = {Search for resonant top quark plus jet production in
             tt̄+jets events with the ATLAS detector in pp collisions at
             √s=7TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.091103},
   Abstract = {This paper presents a search for a new heavy particle
             produced in association with a top or antitop quark. Two
             models in which the new heavy particle is a color singlet or
             a color triplet are considered, decaying, respectively, to
             t̄q or tq, leading to a resonance within the tt̄+jets
             signature. The full 2011 ATLAS pp collision data set from
             the LHC (4.7fb -1) is used to search for tt̄ events
             produced in association with jets, in which one of the W
             bosons from the top quarks decays leptonically and the other
             decays hadronically. The data are consistent with the
             Standard Model expectation, and a new particle with mass
             below 430 Gev for both W ′ boson and color triplet models
             is excluded at 95% confidence level, assuming unit
             right-handed coupling. © 2012 CERN.},
   Doi = {10.1103/PhysRevD.86.091103},
   Key = {fds309057}
}

@article{fds309046,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
             R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J},
   Title = {Search for magnetic monopoles in sqrt[s]=7  TeV pp
             collisions with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {109},
   Number = {26},
   Pages = {261803},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.109.261803},
   Abstract = {This Letter presents a search for magnetic monopoles with
             the ATLAS detector at the CERN Large Hadron Collider using
             an integrated luminosity of 2.0  fb(-1) of pp collisions
             recorded at a center-of-mass energy of sqrt[s]=7  TeV.
             No event is found in the signal region, leading to an upper
             limit on the production cross section at 95% confidence
             level of 1.6/ϵ  fb for Dirac magnetic monopoles with
             the minimum unit magnetic charge and with mass between 200
             GeV and 1500 GeV, where ϵ is the monopole reconstruction
             efficiency. The efficiency ϵ is high and uniform in the
             fiducial region given by pseudorapidity |η|<1.37 and
             transverse kinetic energy 600-700<E(kin)sinθ<1400  GeV.
             The minimum value of 700 GeV is for monopoles of mass 200
             GeV, whereas the minimum value of 600 GeV is applicable for
             higher mass monopoles. Therefore, the upper limit on the
             production cross section at 95% confidence level is 2 fb in
             this fiducial region. Assuming the kinematic distributions
             from Drell-Yan pair production of spin-1/2 Dirac magnetic
             monopoles, the efficiency is in the range 1%-10%, leading to
             an upper limit on the cross section at 95% confidence level
             that varies from 145 fb to 16 fb for monopoles with mass
             between 200 GeV and 1200 GeV. This limit is weaker than the
             fiducial limit because most of these monopoles lie outside
             the fiducial region.},
   Doi = {10.1103/physrevlett.109.261803},
   Key = {fds309046}
}

@article{fds309056,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for R-parity-violating supersymmetry in events with
             four or more leptons in √s =7 TeV pp collisions with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2012},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2012)124},
   Abstract = {A search for new phenomena in final states with four or more
             leptons (electrons or muons) is presented. The analysis is
             based on 4.7 fb-1 of √s =7 TeV proton-proton collisions
             delivered by the Large Hadron Collider and recorded with the
             ATLAS detector. Observations are consistent with Standard
             Model expectations in two signal regions: one that requires
             moderate values of missing transverse momentum and another
             that requires large effective mass. The results are
             interpreted in a simplified model of R-parity-violating
             supersymmetry in which a 95% CL exclusion region is set for
             charged wino masses up to 540 GeV. In an R-parity-violating
             MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are
             excluded for 10 < tan β < 40. © 2012 Cern for the benefit
             of the ATLAS collaboration.},
   Doi = {10.1007/JHEP12(2012)124},
   Key = {fds309056}
}

@article{fds313368,
   Author = {ATLAS Collaboration},
   Title = {A particle consistent with the Higgs boson observed with the
             ATLAS detector at the Large Hadron Collider.},
   Journal = {Science (New York, N.Y.)},
   Volume = {338},
   Number = {6114},
   Pages = {1576-1582},
   Publisher = {American Association for the Advancement of Science
             (AAAS)},
   Year = {2012},
   Month = {December},
   ISSN = {0036-8075},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000312533100043&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {Nearly 50 years ago, theoretical physicists proposed that a
             field permeates the universe and gives energy to the vacuum.
             This field was required to explain why some, but not all,
             fundamental particles have mass. Numerous precision
             measurements during recent decades have provided indirect
             support for the existence of this field, but one crucial
             prediction of this theory has remained unconfirmed despite
             30 years of experimental searches: the existence of a
             massive particle, the standard model Higgs boson. The ATLAS
             experiment at the Large Hadron Collider at CERN has now
             observed the production of a new particle with a mass of 126
             giga-electron volts and decay signatures consistent with
             those expected for the Higgs particle. This result is strong
             support for the standard model of particle physics,
             including the presence of this vacuum field. The existence
             and properties of the newly discovered particle may also
             have consequences beyond the standard model
             itself.},
   Doi = {10.1126/science.1232005},
   Key = {fds313368}
}

@article{fds309054,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for doubly charged Higgs bosons in like-sign dilepton
             final states at √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {72},
   Number = {12},
   Publisher = {Springer Nature},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2244-2},
   Abstract = {A search for doubly charged Higgs bosons decaying to pairs
             of electrons and/or muons is presented. The search is
             performed using a data sample corresponding to an integrated
             luminosity of 4.7 fb−1of pp collisions at √s = 7 TeV
             collected by the ATLAS detector at the LHC. Pairs of prompt,
             isolated, high-pT leptons with the same electric charge
             (e±e±, e±μ±, μ±μ±) are selected, and their
             invariant mass distribution is searched for a narrow
             resonance. No significant excess over Standard Model
             background expectations is observed, and limits are placed
             on the cross section times branching ratio for pair
             production of doubly charged Higgs bosons. The masses of
             doubly charged Higgs bosons are constrained depending on the
             branching ratio into these leptonic final states. Assuming
             pair production, coupling to left-handed fermions, and a
             branching ratio of 100% for each final state, masses below
             409 GeV, 375 GeV, and 398 GeV are excluded for e±e±,
             e±μ±, and μ±μ±, respectively.},
   Doi = {10.1140/epjc/s10052-012-2244-2},
   Key = {fds309054}
}

@article{fds309047,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and A°kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for diphoton events with large missing transverse
             momentum in 7 TeV proton-proton collision data with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {718},
   Number = {2},
   Pages = {411-430},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.10.069},
   Abstract = {A search for diphoton events with large missing transverse
             momentum has been performed using proton-proton collision
             data at s=7 TeV recorded with the ATLAS detector,
             corresponding to an integrated luminosity of 4.8 fb-1. No
             excess of events was observed above the Standard Model
             prediction and model-dependent 95% confidence level
             exclusion limits are set. In the context of a generalised
             model of gauge-mediated supersymmetry breaking with a
             bino-like lightest neutralino of mass above 50 GeV, gluinos
             (squarks) below 1.07 TeV (0.87 TeV) are excluded, while a
             breaking scale Λ below 196 TeV is excluded for a minimal
             model of gauge-mediated supersymmetry breaking. For a
             specific model with one universal extra dimension,
             compactification scales 1/R<1.40 TeV are excluded. These
             limits provide the most stringent tests of these models to
             date. © 2012 CERN.},
   Doi = {10.1016/j.physletb.2012.10.069},
   Key = {fds309047}
}

@article{fds309048,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for the Higgs boson in the H→WW→ℓνjj decay
             channel at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {718},
   Number = {2},
   Pages = {391-410},
   Publisher = {Elsevier BV},
   Year = {2012},
   Month = {December},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.10.066},
   Abstract = {A search for the Standard Model Higgs boson has been
             performed in the H→WW→ℓνjj channel using 4.7 fb−1
             of pp collision data recorded at a centre-of-mass energy of
             s=7 TeV with the ATLAS detector at the Large Hadron
             Collider. Higgs boson candidates produced in association
             with zero, one or two jets are included in the analysis to
             maximize the acceptance for both gluon fusion and weak boson
             fusion Higgs boson production processes. No significant
             excess of events is observed over the expected background
             and limits on the Higgs boson production cross section are
             derived for a Higgs boson mass in the range 300 GeV<mH<600
             GeV. The best sensitivity is reached for mH=400 GeV, where
             the observed (expected) 95% confidence level upper bound on
             the cross section for H→WW produced in association with
             zero or one jet is 2.2 pb (1.9 pb), corresponding to 1.9
             (1.6) times the Standard Model prediction. In the Higgs
             boson plus two jets channel, which is more sensitive to the
             weak boson fusion process, the observed (expected) 95%
             confidence level upper bound on the cross section for H→WW
             production with mH=400 GeV is 0.7 pb (0.6 pb), corresponding
             to 7.9 (6.5) times the Standard Model prediction.},
   Doi = {10.1016/j.physletb.2012.10.066},
   Key = {fds309048}
}

@article{fds309050,
   Author = {Aaltonen, T and Adelman, J and Lvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
             Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
             F},
   Title = {Search for a heavy vector boson decaying to two gluons in
             pp̄ collisions at √s=1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {86},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2012},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.86.112002},
   Abstract = {We present a search for a new heavy vector boson Z′ that
             decays to gluons. Decays to on-shell gluons are suppressed,
             leading to a dominant decay mode of Z′→g*g. We study the
             case where the off-shell gluon g* converts to a pair of top
             quarks, leading to a final state of tt̄g. In a sample of
             events with exactly one charged lepton, large missing
             transverse momentum and at least five jets, corresponding to
             an integrated luminosity of 8.7fb-1 collected by the CDF II
             detector, we find the data to be consistent with the
             standard model. We set upper limits on the production cross
             section times branching ratio of this chromophilic Z′ at
             95% confidence level from 300 to 40 fb for Z′ masses
             ranging from 400 to 1000GeV/c2, respectively. © 2012
             American Physical Society.},
   Doi = {10.1103/PhysRevD.86.112002},
   Key = {fds309050}
}

@article{fds309013,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, L and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos,
             S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JJB and Badescu, E and Bagnaia, P and Bahinipati,
             S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio,
             EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Harpaz,
             SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni,
             A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
             AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
             G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
             V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
   Title = {Search for supersymmetry in events with photons, bottom
             quarks, and missing transverse momentum in proton-proton
             collisions at a centre-of-mass energy of 7 TeV with the
             ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {261-279},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.041},
   Abstract = {© 2013 CERN A search has been performed for the
             experimental signature of an isolated photon with high
             transverse momentum, at least one jet identified as
             originating from a bottom quark, and high missing transverse
             momentum. Such a final state may originate from
             supersymmetric models with gauge-mediated supersymmetry
             breaking in events in which one of a pair of higgsino-like
             neutralinos decays into a photon and a gravitino while the
             other decays into a Higgs boson and a gravitino. The search
             is performed using the full dataset of 7 TeV proton–proton
             collisions recorded with the ATLAS detector at the LHC in
             2011, corresponding to an integrated luminosity of 4.7
             fb−1. A total of 7 candidate events are observed while
             7.5±2.2 events are expected from the Standard Model
             background. The results of the search are interpreted in the
             context of general gauge mediation to exclude certain
             regions of a benchmark plane for higgsino-like neutralino
             production.},
   Doi = {10.1016/j.physletb.2013.01.041},
   Key = {fds309013}
}

@article{fds309014,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, R and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
             A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, R and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Gimenez, VC and Castro,
             NF and Cataldi, G and Catastini, R and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, R and Citron, ZH and Citterio, M and Ciubancan, M and Clark,
             A},
   Title = {A search for high-mass resonances decaying to
             τ+τ- in pp collisions at
             √s=7 TeV with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {242-260},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.040},
   Abstract = {© 2012 CERN This Letter presents a search for high-mass
             resonances decaying into τ+τ− final states using
             proton-proton collisions at s=7 TeV produced by the Large
             Hadron Collider. The data were recorded with the ATLAS
             detector and correspond to an integrated luminosity of 4.6
             fb−1. No statistically significant excess above the
             Standard Model expectation is observed; 95% credibility
             upper limits are set on the cross section times branching
             fraction of Z′ resonances decaying into τ+τ− pairs as
             a function of the resonance mass. As a result, Z′ bosons
             of the Sequential Standard Model with masses less than 1.40
             TeV are excluded at 95% credibility.},
   Doi = {10.1016/j.physletb.2013.01.040},
   Key = {fds309014}
}

@article{fds309015,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung,
             C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker,
             S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
             NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, E and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
             J},
   Title = {A search for prompt lepton-jets in pp collisions at
             √s=7 TeV with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {299-317},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.034},
   Abstract = {© 2013 CERN We present a search for a light (mass <2GeV)
             boson predicted by Hidden Valley supersymmetric models that
             decays into a final state consisting of collimated muons or
             electrons, denoted “lepton-jets”. The analysis uses
             5fb−1 of s=7TeV proton–proton collision data recorded by
             the ATLAS detector at the Large Hadron Collider to search
             for the following signatures: single lepton-jets with at
             least four muons; pairs of lepton-jets, each with two or
             more muons; and pairs of lepton-jets with two or more
             electrons. This study finds no statistically significant
             deviation from the Standard Model prediction and places 95%
             confidence-level exclusion limits on the production cross
             section times branching ratio of light bosons for several
             parameter sets of a Hidden Valley model.},
   Doi = {10.1016/j.physletb.2013.01.034},
   Key = {fds309015}
}

@article{fds309016,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, R and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, E and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, R and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
             M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
             PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
             M and Belloni, A and Belaboradova, O and Belotiskiy, K and Beltramello,
             O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Nocioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Bensalma, K and Bentvelsen, S and Berge,
             D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitnec, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boviea, A and Boyd, J and Boyka, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, E and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Carbreara Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capau, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, E and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, E and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
             JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
             NJ and Collins-Tooth, C and Collot, J},
   Title = {Measurement of the jet radius and transverse momentum
             dependence of inclusive jet suppression in lead-lead
             collisions at √SNN=2.76 TeV with the
             ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {719},
   Number = {4-5},
   Pages = {220-241},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.024},
   Abstract = {Measurements of inclusive jet suppression in heavy ion
             collisions at the LHC provide direct sensitivity to the
             physics of jet quenching. In a sample of lead–lead
             collisions at sNN=2.76 TeV corresponding to an integrated
             luminosity of approximately 7 μb−1, ATLAS has measured
             jets with a calorimeter system over the pseudorapidity
             interval |η|<2.1 and over the transverse momentum range
             38<pT<210 GeV. Jets were reconstructed using the anti-kt
             algorithm with values for the distance parameter that
             determines the nominal jet radius of R=0.2, 0.3, 0.4 and
             0.5. The centrality dependence of the jet yield is
             characterized by the jet “central-to-peripheral ratio,”
             RCP. Jet production is found to be suppressed by
             approximately a factor of two in the 10% most central
             collisions relative to peripheral collisions. RCP varies
             smoothly with centrality as characterized by the number of
             participating nucleons. The observed suppression is only
             weakly dependent on jet radius and transverse momentum.
             These results provide the first direct measurement of
             inclusive jet suppression in heavy ion collisions and
             complement previous measurements of dijet transverse energy
             imbalance at the LHC.},
   Doi = {10.1016/j.physletb.2013.01.024},
   Key = {fds309016}
}

@article{fds309022,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
             Costa, JJBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Bege, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Busey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, JJ and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas,
             CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, JJ and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
   Title = {Search for pair production of heavy top-like quarks decaying
             to a high-pT W boson and a b
             quark in the lepton plus jets final state at √s=7
             TeV with the ATLAS detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {4-5},
   Pages = {1284-1302},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.071},
   Abstract = {© 2012 CERN A search is presented for production of a heavy
             up-type quark (t′) together with its antiparticle,
             assuming a significant branching ratio for subsequent decay
             into a W boson and a b quark. The search is based on 4.7
             fb−1 of pp collisions at s=7 TeV recorded in 2011 with the
             ATLAS detector at the CERN Large Hadron Collider. Data are
             analyzed in the lepton + jets final state, characterized by
             a high-transverse-momentum isolated electron or muon, large
             missing transverse momentum and at least three jets. The
             analysis strategy relies on the substantial boost of the W
             bosons in the t′t¯′ signal when mt′≳400 GeV. No
             significant excess of events above the Standard Model
             expectation is observed and the result of the search is
             interpreted in the context of fourth-generation and
             vector-like quark models. Under the assumption of a
             branching ratio BR(t′→Wb)=1, a fourth-generation t′
             quark with mass lower than 656 GeV is excluded at 95%
             confidence level. In addition, in light of the recent
             discovery of a new boson of mass ∼126 GeV at the LHC,
             upper limits are derived in the two-dimensional plane of
             BR(t′→Wb) versus BR(t′→Ht), where H is the Standard
             Model Higgs boson, for vector-like quarks of various
             masses.},
   Doi = {10.1016/j.physletb.2012.11.071},
   Key = {fds309022}
}

@article{fds309026,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arika, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, R and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
             Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans,
             RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
             MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
             M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
             VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas,
             CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
             L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M},
   Title = {Search for new phenomena in the WW → |v|′v′ final
             state in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {3},
   Pages = {860-878},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.040},
   Abstract = {This Letter reports a search for a heavy particle that
             decays to WW using events produced in pp collisions at
             s=7TeV. The data were recorded in 2011 by the ATLAS detector
             and correspond to an integrated luminosity of 4.7 fb-1.
             WW→ℓνℓ'ν'(ℓ, ℓ'=e or μ) final states are
             considered and the distribution of the transverse mass of
             the WW candidates is found to be consistent with Standard
             Model expectations. Upper limits on the production cross
             section times branching ratio into W boson pairs are set for
             Randall-Sundrum and bulk Randall-Sundrum gravitons, which
             result in observed 95% CL lower limits on the masses of the
             two particles of 1.23 TeV and 0.84 TeV, respectively. ©
             2012 CERN.},
   Doi = {10.1016/j.physletb.2012.11.040},
   Key = {fds309026}
}

@article{fds309027,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, R and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansi, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Da Costa and JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Be, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, E and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
             J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
             C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
             J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki,
             J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, JJ and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Buanes, T and Buat, QQ and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov,
             O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans, RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, JJ and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
             AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
             G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Io, MAC and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and El
             Moursli, RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, R and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C},
   Title = {Search for direct slepton and gaugino production in final
             states with two leptons and missing transverse momentum with
             the ATLAS detector in pp collisions at √s=7
             TeV},
   Journal = {PHYSICS LETTERS B},
   Volume = {718},
   Number = {3},
   Pages = {879-901},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.058},
   Abstract = {A search for the electroweak pair production of charged
             sleptons and weak gauginos decaying into final states with
             two leptons is performed using 4.7 fb-1 of proton-proton
             collision data at s=7 TeV recorded with the ATLAS experiment
             at the Large Hadron Collider. No significant excesses are
             observed with respect to the prediction from Standard Model
             processes. In the scenario of direct slepton production, if
             the sleptons decay directly into the lightest neutralino,
             left-handed slepton masses between 85 and 195 GeV are
             excluded at 95% confidence level for a 20 GeV neutralino.
             Chargino masses between 110 and 340 GeV are excluded in the
             scenario of direct production of wino-like chargino pairs
             decaying into the lightest neutralino via an intermediate
             on-shell charged slepton for a 10 GeV neutralino. The
             results are also interpreted in the framework of the
             phenomenological minimal supersymmetric Standard Model. ©
             2012 CERN.},
   Doi = {10.1016/j.physletb.2012.11.058},
   Key = {fds309027}
}

@article{fds309036,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
             VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
             M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
             AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes,
             JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey,
             DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, JB and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
             AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans,
             RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
             A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
             SL and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
             BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu,
             ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca,
             D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
             ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN and Clemens, JC},
   Title = {Dynamics of isolated-photon plus jet production in pp
             collisions at s=7 TeV with the ATLAS detector},
   Journal = {Nuclear Physics B},
   Volume = {875},
   Number = {3},
   Pages = {483-535},
   Publisher = {Elsevier BV},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2013.07.025},
   Abstract = {The dynamics of isolated-photon plus jet production in pp
             collisions at a centre-of-mass energy of 7 TeV has been
             studied with the ATLAS detector at the LHC using an
             integrated luminosity of 37 pb-1. Measurements of
             isolated-photon plus jet bin-averaged cross sections are
             presented as functions of photon transverse energy, jet
             transverse momentum and jet rapidity. In addition, the
             bin-averaged cross sections as functions of the difference
             between the azimuthal angles of the photon and the jet, the
             photon-jet invariant mass and the scattering angle in the
             photon-jet centre-of-mass frame have been measured.
             Next-to-leading-order QCD calculations are compared to the
             measurements and provide a good description of the data,
             except for the case of the azimuthal opening angle. © 2013
             CERN.},
   Doi = {10.1016/j.nuclphysb.2013.07.025},
   Key = {fds309036}
}

@article{fds309044,
   Author = {Kang, SB and Han, SJ and Nam, SB and Nam, IS and Cho, BK and Kim, CH and Oh,
             SH},
   Title = {Effect of aging atmosphere on thermal sintering of modern
             commercial TWCs},
   Journal = {Topics in Catalysis},
   Volume = {56},
   Number = {1-8},
   Pages = {298-305},
   Year = {2013},
   url = {http://dx.doi.org/10.1007/s11244-013-9970-z},
   Abstract = {The effect of aging atmosphere on the sintering behavior of
             commercial Pd and Rh catalysts as well as the TWC
             performance thereof has been investigated under straight
             oxidizing, reducing and periodic cycling aging conditions,
             in search of useful guidance in the optimum design of
             thermally durable TWCs for advanced gasoline engines
             equipped with the deceleration fuel cutoff technology. Pd
             and Rh catalysts individually exhibit an opposite trend in
             the thermal sintering behavior with respect to the aging
             atmosphere. Under oxidizing conditions, the Pd catalyst
             becomes more resistant to sintering in higher O 2
             concentrations, whereas the Rh catalyst reveals the opposite
             behavior, regardless of the aging temperature.
             Physicochemical characterizations by using TGA and CO
             chemisorption have indicated that the state of Pd (PdO vs.
             Pd0) and Rh (Rh2O3 vs. Rh0) on the catalyst surface formed
             during the thermal aging plays an important role for
             determining the trend of thermal sintering; the positive
             effect of the O 2 concentration on Pd sintering is
             attributable primarily to the formation of PdO, while the
             main cause for severe deactivation of the Rh catalyst under
             oxidizing conditions is the diffusion of Rh2O 3 into the
             support along with the agglomeration of Rh particles. ©
             2013 Springer Science+Business Media New
             York.},
   Doi = {10.1007/s11244-013-9970-z},
   Key = {fds309044}
}

@article{fds309045,
   Author = {Kim, PS and Kim, MK and Cho, BK and Nam, IS and Oh, SH},
   Title = {Effect of H2 on deNOx performance of
             HC-SCR over Ag/Al2O3: Morphological,
             chemical, and kinetic changes},
   Journal = {Journal of Catalysis},
   Volume = {301},
   Pages = {65-76},
   Year = {2013},
   url = {http://dx.doi.org/10.1016/j.jcat.2013.01.026},
   Abstract = {The enhanced deNOx performance of the Ag/Al2O 3 catalyst by
             addition of H2 was investigated for HC-SCR using a mixture
             of simulated diesel and ethanol as the reductant. As H 2
             concentration increased in the feed-gas stream, the
             low-temperature NOx reduction activity was remarkably
             enhanced. Addition of H 2 promoted the oxidation of both NO
             and hydrocarbons, resulting in an increased formation of
             nitrates, enolic, and isocyanate species regarded as
             reaction intermediates. Results of the UV-vis indicated that
             H2 promoted the transformation of Ag+ to Agnδ+ and Ag0 on
             the surface of Ag/Al2O3 catalyst, while those of H 2-TPR,
             O2-TPD, in situ FTIR, and TGA revealed the formation of
             highly mobile and reactive oxygen species under the (O2 +
             H2) flow. A reaction mechanism is proposed to elucidate the
             role of H2 in the enhancement of deNOx performance of HC-SCR
             in view of morphological, chemical, and kinetic changes of
             the Ag/Al 2O3 catalytic system. © 2013 Elsevier Inc. All
             rights reserved.},
   Doi = {10.1016/j.jcat.2013.01.026},
   Key = {fds309045}
}

@article{fds309073,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and Barbaro,
             PD and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Canto,
             AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Ramos, JPF and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Garfinkel, AF and Garosi,
             P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and López, OG and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare,
             M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
             A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Fernández, IR and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov,
             A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
   Title = {Measurement of the mass difference between top and antitop
             quarks},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Pages = {052013},
   Year = {2013},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052013},
   Abstract = {We present a measurement of the mass difference between top
             (t) and antitop (t̄) quarks using tt̄ candidate events
             reconstructed in the final state with one lepton and
             multiple jets. We use the full data set of Tevatron
             √s=1.96 TeV proton-antiproton collisions recorded by the
             CDF II detector, corresponding to an integrated luminosity
             of 8.7 fb-1. We estimate event by event the mass difference
             to construct templates for top pair signal events and
             background events. The resulting mass difference
             distribution in data compared to signal and background
             templates using a likelihood fit yields ΔMtop=Mt-Mt̄=-1.95±1.11(stat)
             ±0.59(syst) GeV/c2 and is in agreement with the standard
             model prediction of no mass difference. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.87.052013},
   Key = {fds309073}
}

@article{fds221238,
   Author = {S. Oh and ATLAS collaboration},
   Title = {Search for WH production with a light Higgs boson decaying
             to prompt electron-jets in proton-proton collisions at √s
             = 7 TeV with the ATLAS detector},
   Journal = {New J. Phys. 15 (2013) 043009},
   Year = {2013},
   Key = {fds221238}
}

@article{fds221239,
   Author = {S. Oh and ATLAS collaboration},
   Title = {Search for heavy resonance decaying to WW or WZ in the lvjj
             and lvJ (boosted) final states.},
   Journal = {Phys. Rev. D 87, 112006 (2013)},
   Year = {2013},
   Key = {fds221239}
}

@article{fds221240,
   Author = {S. Oh and ATLAS collaboration},
   Title = {Measurements of Higgs production and couplings using diboson
             final states with the ATLAS detector at the
             LHC},
   Journal = {Phys. Lett. B 726 (2013), pp. 88-119},
   Year = {2013},
   Key = {fds221240}
}

@article{fds221235,
   Author = {S. Oh and T. Aaltonen et al},
   Title = {Search for Pair Production of Strongly Interacting Particles
             Decaying to Pairs of Jets in p pbar Collisions at sqrt (s) =
             1.96 TeV},
   Journal = {Phys. Rev. Lett. 111, 031802 (2013). arXiv:
             1303.2699},
   Year = {2013},
   Key = {fds221235}
}

@article{fds221236,
   Author = {S. Oh and T. Aaltonen et al},
   Title = {Production Properties of Ks, K* and phi in MB Events and Ks
             and Lambda in Jets},
   Journal = {PRD, 2013},
   Year = {2013},
   Key = {fds221236}
}

@article{fds308948,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for charginos nearly mass degenerate with the
             lightest neutralino based on a disappearing-track signature
             in pp collisions at √(s) = 8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {11},
   Pages = {112006-1-112006-23},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.112006},
   Abstract = {A search is presented for direct chargino production based
             on a disappearing-track signature using 20:3 fb-1 of
             proton-proton collisions at √s = 8 TeV collected with the
             ATLAS experiment at the LHC. In anomaly-mediated
             supersymmetry breaking (AMSB) models, the lightest chargino
             is nearly mass degenerate with the lightest neutralino and
             its lifetime is long enough to be detected in the tracking
             detectors by identifying decays that result in tracks with
             no associated hits in the outer region of the tracking
             system. Some models with supersymmetry also predict
             charginos with a significant lifetime. This analysis attains
             sensitivity for charginos with a lifetime between 0.1 and 10
             ns, and significantly surpasses the reach of the LEP
             experiments. No significant excess above the background
             expectation is observed for candidate tracks with large
             transverse momentum, and constraints on chargino properties
             are obtained. In the AMSB scenarios, a chargino mass below
             270 GeV is excluded at 95% confidence level.},
   Doi = {10.1103/PhysRevD.88.112006},
   Key = {fds308948}
}

@article{fds308950,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for long-lived stopped R-hadrons decaying out of time
             with pp collisions using the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {11},
   Pages = {112003-1-112003-30},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.112003},
   Abstract = {An updated search is performed for gluino, top squark, or
             bottom squark R-hadrons that have come to rest within the
             ATLAS calorimeter, and decay at some later time to hadronic
             jets and a neutralino, using 5.0 and 22:9 fb-1 of pp
             collisions at 7 and 8 TeV, respectively. Candidate decay
             events are triggered in selected empty bunch crossings of
             the LHC in order to remove pp collision backgrounds.
             Selections based on jet shape and muon system activity are
             applied to discriminate signal events from cosmic ray and
             beam-halo muon backgrounds. In the absence of an excess of
             events, improved limits are set on gluino, stop, and sbottom
             masses for different decays, lifetimes, and neutralino
             masses. With a neutralino of mass 100 GeV, the analysis
             excludes gluinos with mass below 832 GeV (with an expected
             lower limit of 731 GeV), for a gluino lifetime between 10
             μs and 1000 s in the generic R-hadron model with equal
             branching ratios for decays to (formula presented) and
             (formula presented). Under the same assumptions for the
             neutralino mass and squark lifetime, top squarks and bottom
             squarks in the Regge R-hadron model are excluded with masses
             below 379 and 344 GeV, respectively.},
   Doi = {10.1103/PhysRevD.88.112003},
   Key = {fds308950}
}

@article{fds310543,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson,
             TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand,
             S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Measurement of the top quark charge in pp collisions at √s
             = 7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2013)031},
   Abstract = {A measurement of the top quark electric charge is carried
             out in the ATLAS experiment at the Large Hadron Collider
             using 2.05 fb-1 of data at a centre-of-mass energy of 7TeV.
             In units of the elementary electric charge, the top quark
             charge is determined to be 0.64 ± 0.02 (stat.) ± 0.08
             (syst.) from the charges of the top quark decay products in
             single lepton tt̄ candidate events. This excludes models
             that propose a heavy quark of electric charge -4/3, instead
             of the Standard Model top quark, with a significance of more
             than 8σ. Copyright CERN.},
   Doi = {10.1007/JHEP11(2013)031},
   Key = {fds310543}
}

@article{fds308962,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Measurement of the differential cross-section of B+ meson
             production in pp collisions at √s = 7 TeV at
             ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {10},
   Pages = {1-37},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP10(2013)042},
   Abstract = {The production cross-section of B+ mesons is measured as a
             function of transverse momentum pT and rapidity y in
             proton-proton collisions at centre-of-mass energy √s = 7
             TeV, using 2.4 fb-1 of data recorded with the ATLAS detector
             at the Large Hadron Collider. The differential production
             cross-sections, determined in the range 9 GeV < pT < 120 GeV
             and |y| < 2:25, are compared to next-to-leading-order
             theoretical predictions. Copyright CERN.},
   Doi = {10.1007/JHEP10(2013)042},
   Key = {fds308962}
}

@article{fds308978,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, KM and Blair,
             RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
             J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
             S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A},
   Title = {Measurement of the inclusive jet cross-section in pp
             collisions at [Formula: see text] and comparison to the
             inclusive jet cross-section at [Formula: see text] using the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {8},
   Pages = {2509},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2509-4},
   Abstract = {The inclusive jet cross-section has been measured in
             proton-proton collisions at [Formula: see text] in a dataset
             corresponding to an integrated luminosity of [Formula: see
             text] collected with the ATLAS detector at the Large Hadron
             Collider in 2011. Jets are identified using the
             anti-<i>k</i><sub><i>t</i></sub> algorithm with two radius
             parameters of 0.4 and 0.6. The inclusive jet
             double-differential cross-section is presented as a function
             of the jet transverse momentum <i>p</i><sub>T</sub> and jet
             rapidity <i>y</i>, covering a range of 20≤<i>p</i><sub>T</sub><430 GeV
             and |<i>y</i>|<4.4. The ratio of the cross-section to the
             inclusive jet cross-section measurement at [Formula: see
             text], published by the ATLAS Collaboration, is calculated
             as a function of both transverse momentum and the
             dimensionless quantity [Formula: see text], in bins of jet
             rapidity. The systematic uncertainties on the ratios are
             significantly reduced due to the cancellation of correlated
             uncertainties in the two measurements. Results are compared
             to the prediction from next-to-leading order perturbative
             QCD calculations corrected for non-perturbative effects, and
             next-to-leading order Monte Carlo simulation. Furthermore,
             the ATLAS jet cross-section measurements at [Formula: see
             text] and [Formula: see text] are analysed within a
             framework of next-to-leading order perturbative QCD
             calculations to determine parton distribution functions of
             the proton, taking into account the correlations between the
             measurements.},
   Doi = {10.1140/epjc/s10052-013-2509-4},
   Key = {fds308978}
}

@article{fds308979,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
             R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
             V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
             A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
   Title = {Improved luminosity determination in pp collisions at
             [Formula: see text] using the ATLAS detector at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {8},
   Pages = {2518},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2518-3},
   Abstract = {The luminosity calibration for the ATLAS detector at the LHC
             during <i>pp</i> collisions at [Formula: see text] in 2010
             and 2011 is presented. Evaluation of the luminosity scale is
             performed using several luminosity-sensitive detectors, and
             comparisons are made of the long-term stability and accuracy
             of this calibration applied to the <i>pp</i> collisions at
             [Formula: see text]. A luminosity uncertainty of [Formula:
             see text] is obtained for the 47 pb<sup>-1</sup> of data
             delivered to ATLAS in 2010, and an uncertainty of [Formula:
             see text] is obtained for the 5.5 fb<sup>-1</sup> delivered
             in 2011.},
   Doi = {10.1140/epjc/s10052-013-2518-3},
   Key = {fds308979}
}

@article{fds308980,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for tt̄ resonances in the lepton plus jets final
             state with ATLAS using 4.7 fb–1of pp collisions
             at √s = 7 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.012004},
   Abstract = {A search for new particles that decay into top quark pairs
             (tt) is performed with the ATLAS experiment at the LHC using
             an integrated luminosity of 4.7 fb–1of proton–proton
             (pp) collision data collected at a center-of-mass energy
             √s = 7 TeV. In the tt̄→ WbWb decay, the lepton plus
             jets final state is used, where one W boson decays
             leptonically and the other hadronically. The tt̄system is
             reconstructed using both small-radius and large-radius jets,
             the latter being supplemented by a jet substructure
             analysis. A search for local excesses in the number of data
             events compared to the Standard Model expectation in the
             tt̄invariant mass spectrum is performed. No evidence for a
             tt̄resonance is found and 95% credibility-level limits on
             the production rate are determined for massive states
             predicted in two benchmark models. The upper limits on the
             cross section times branching ratio of a narrow Z′
             resonance range from 5.1 pb for a boson mass of 0.5 TeV to
             0.03 pb for a mass of 3 TeV. A narrow leptophobic topcolor
             Z′ resonance with a mass below 1.74 TeV is excluded.
             Limits are also derived for a broad color-octet resonance
             with Γ/m = 15.3%. A Kaluza–Klein excitation of the gluon
             in a Randall–Sundrum model is excluded for masses below
             2.07 TeV.},
   Doi = {10.1103/PhysRevD.88.012004},
   Key = {fds308980}
}

@article{fds308985,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for resonant diboson production in the WW/WZ →
             ℓvjj decay channels with the ATLAS detector at √s = 7
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.112006},
   Abstract = {A search for resonant diboson production using a data sample
             corresponding to 4:7 fb–1of integrated luminosity
             collected by the ATLAS experiment at the Large Hadron
             Collider in pp collisions at √s = 7 TeV is presented. The
             search for a narrow resonance in the WW or WZ mass
             distribution is conducted in a final state with an electron
             or a muon, missing transverse momentum, and at least two
             jets. No significant excess is observed and limits are set
             using three benchmark models: WW resonance masses below 940
             and 710 GeV are excluded at 95% confidence level for spin-2
             Randall–Sundrum and bulk Randall–Sundrum gravitons,
             respectively; WZ resonance masses below 950 GeV are excluded
             at 95% confidence level for a spin-1 extended gauge model
             W′ boson.},
   Doi = {10.1103/PhysRevD.87.112006},
   Key = {fds308985}
}

@article{fds308990,
   Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
             E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
             J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y},
   Title = {Search for a light charged Higgs boson in the decay channel
             [Formula: see text] in [Formula: see text] events using
             pp collisions at [Formula: see text] with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {6},
   Pages = {2465},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2465-z},
   Abstract = {A search for a charged Higgs boson (<i>H</i><sup>+</sup>) in
             [Formula: see text] decays is presented, where one of the
             top quarks decays via <i>t</i>→<i>H</i><sup>+</sup><i>b</i>,
             followed by <i>H</i><sup>+</sup>→ two jets ([Formula: see
             text]). The other top quark decays to <i>Wb</i>, where the
             <i>W</i> boson then decays into a lepton
             (<i>e</i>/<i>μ</i>) and a neutrino. The data were recorded
             in <i>pp</i> collisions at [Formula: see text] by the ATLAS
             detector at the LHC in 2011, and correspond to an integrated
             luminosity of 4.7 fb<sup>-1</sup>. With no observation of a
             signal, 95 % confidence level (CL) upper limits are set on
             the decay branching ratio of top quarks to charged Higgs
             bosons varying between 5 % and 1 % for
             <i>H</i><sup>+</sup> masses between 90 GeV and 150 GeV,
             assuming [Formula: see text].},
   Doi = {10.1140/epjc/s10052-013-2465-z},
   Key = {fds308990}
}

@article{fds308994,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach,
             B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
             F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
             J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
             V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C},
   Title = {Measurement of kT splitting scales in
             Wℓν events at [Formula: see text] with
             the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {5},
   Pages = {2432},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2432-8},
   Abstract = {A measurement of splitting scales, as defined by the
             <i>k</i><sub>T</sub> clustering algorithm, is presented for
             final states containing a <i>W</i> boson produced in
             proton-proton collisions at a centre-of-mass energy of
             7 TeV. The measurement is based on the full 2010 data
             sample corresponding to an integrated luminosity of
             36 pb<sup>-1</sup> which was collected using the ATLAS
             detector at the CERN Large Hadron Collider. Cluster
             splitting scales are measured in events containing <i>W</i>
             bosons decaying to electrons or muons. The measurement
             comprises the four hardest splitting scales in a
             <i>k</i><sub>T</sub> cluster sequence of the hadronic
             activity accompanying the <i>W</i> boson, and ratios of
             these splitting scales. Backgrounds such as multi-jet and
             top-quark-pair production are subtracted and the results are
             corrected for detector effects. Predictions from various
             Monte Carlo event generators at particle level are compared
             to the data. Overall, reasonable agreement is found with all
             generators, but larger deviations between the predictions
             and the data are evident in the soft regions of the
             splitting scales.},
   Doi = {10.1140/epjc/s10052-013-2432-8},
   Key = {fds308994}
}

@article{fds309005,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
             MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
             R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
             J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
             F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans
             Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo
             Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
             D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
             AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
             B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG},
   Title = {Jet energy resolution in proton-proton collisions at
             [Formula: see text] recorded in 2010 with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {3},
   Pages = {2306},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2306-0},
   Abstract = {The measurement of the jet energy resolution is presented
             using data recorded with the ATLAS detector in proton-proton
             collisions at [Formula: see text]. The sample corresponds to
             an integrated luminosity of 35 pb<sup>-1</sup>. Jets are
             reconstructed from energy deposits measured by the
             calorimeters and calibrated using different jet calibration
             schemes. The jet energy resolution is measured with two
             different in situ methods which are found to be in agreement
             within uncertainties. The total uncertainties on these
             measurements range from 20 % to 10 % for jets within
             |<i>y</i>|<2.8 and with transverse momenta increasing
             from 30 GeV to 500 GeV. Overall, the Monte Carlo
             simulation of the jet energy resolution agrees with the data
             within 10 %.},
   Doi = {10.1140/epjc/s10052-013-2306-0},
   Key = {fds309005}
}

@article{fds309006,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio,
             EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas,
             CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
   Title = {Measurement of the [Formula: see text] production cross
             section in the tau + jets channel using the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {3},
   Pages = {2328},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2328-7},
   Abstract = {A measurement of the top quark pair production cross section
             in the final state with a hadronically decaying tau lepton
             and jets is presented. The analysis is based on
             proton-proton collision data recorded by the ATLAS
             experiment at the LHC, with a centre-of-mass energy of
             7 TeV. The data sample corresponds to an integrated
             luminosity of 1.67 fb<sup>-1</sup>. The cross section is
             measured to be [Formula: see text] and is in agreement with
             other measurements and with the Standard Model
             prediction.},
   Doi = {10.1140/epjc/s10052-013-2328-7},
   Key = {fds309006}
}

@article{fds309009,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
             OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer,
             F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
             D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
             E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
             T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Multi-channel search for squarks and gluinos in [Formula:
             see text]pp collisions with the ATLAS detector at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {3},
   Pages = {2362},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2362-5},
   Abstract = {A search for supersymmetric particles in final states with
             zero, one, and two leptons, with and without jets identified
             as originating from <i>b</i>-quarks, in 4.7 fb<sup>-1</sup>
             of [Formula: see text]<i>pp</i> collisions produced by the
             Large Hadron Collider and recorded by the ATLAS detector is
             presented. The search uses a set of variables carrying
             information on the event kinematics transverse and parallel
             to the beam line that are sensitive to several topologies
             expected in supersymmetry. Mutually exclusive final states
             are defined, allowing a combination of all channels to
             increase the search sensitivity. No deviation from the
             Standard Model expectation is observed. Upper limits at
             95 % confidence level on visible cross-sections for the
             production of new particles are extracted. Results are
             interpreted in the context of the constrained minimal
             supersymmetric extension to the Standard Model and in
             supersymmetry-inspired models with diverse,
             high-multiplicity final states.},
   Doi = {10.1140/epjc/s10052-013-2362-5},
   Key = {fds309009}
}

@article{fds309011,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
             JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnault, C and Artamonov, A},
   Title = {Jet energy measurement with the ATLAS detector in
             proton-proton collisions at √s =7 TeV},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2304-2},
   Abstract = {The jet energy scale and its systematic uncertainty are
             determined for jets measured with the ATLAS detector at the
             LHC in proton-proton collision data at a centre-of-mass
             energy of √ s = 7 TeV corresponding to an integrated
             luminosity of 38 pb-1. Jets are reconstructed with the
             anti-kt algorithm with distance parameters R = 0.4 or R =
             0.6. Jet energy and angle corrections are determined from
             Monte Carlo simulations to calibrate jets with transverse
             momenta pT ≥ 20 GeV and pseudorapidities |η| < 4.5. The
             jet energy systematic uncertainty is estimated using the
             single isolated hadron response measured in situ and in
             test-beams, exploiting the transverse momentum balance
             between central and forward jets in events with dijet
             topologies and studying systematic variations in Monte Carlo
             simulations. The jet energy uncertainty is less than 2.5 %
             in the central calorimeter region (|η| < 0.8) for jets with
             60 ≤ pT < 800 GeV, and is maximally 14 % for pT ≤ 30 GeV
             in the most forward region 3.2 ≤ |η| < 4.5. The jet
             energy is validated for jet transverse momenta up to 1 TeV
             to the level of a few percent using several in situ
             techniques by comparing a well-known reference such as the
             recoiling photon pT, the sum of the transverse momenta of
             tracks associated to the jet, or a system of low-pT jets
             recoiling against a high-pT jet. More sophisticated jet
             calibration schemes are presented based on calorimeter cell
             energy density weighting or hadronic properties of jets,
             aiming for an improved jet energy resolution and a reduced
             flavour dependence of the jet response. The systematic
             uncertainty of the jet energy determined from a combination
             of in situ techniques is consistent with the one derived
             from single hadron response measurements over a wide
             kinematic range. The nominal corrections and uncertainties
             are derived for isolated jets in an inclusive sample of
             high-pT jets. Special cases such as event topologies with
             close-by jets, or selections of samples with an enhanced
             content of jets originating from light quarks, heavy quarks
             or gluons are also discussed and the corresponding
             uncertainties are determined.},
   Doi = {10.1140/epjc/s10052-013-2304-2},
   Key = {fds309011}
}

@article{fds309020,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for the neutral Higgs bosons of the minimal
             supersymmetric standard model in pp collisions at √s = 7
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {2},
   Pages = {1-46},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP02(2013)095},
   Abstract = {A search for neutral Higgs bosons of the Minimal
             Supersymmetric Standard Model (MSSM) is reported. The
             analysis is based on a sample of proton-proton collisions at
             a centre-of-mass energy of 7TeV recorded with the ATLAS
             detector at the Large Hadron Collider. The data were
             recorded in 2011 and correspond to an integrated luminosity
             of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into
             oppositely-charged muon or τ lepton pairs are considered
             for final states requiring either the presence or absence of
             b-jets. No statistically significant excess over the
             expected background is observed and exclusion limits at the
             95% confidence level are derived. The exclusion limits are
             for the production cross-section of a generic neutral Higgs
             boson, φ, as a function of the Higgs boson mass and for
             h/A/H production in the MSSM as a function of the parameters
             mA and tan β in the mhmax scenario for mA in the range of
             90GeV to 500 GeV. Copyright CERN.},
   Doi = {10.1007/JHEP02(2013)095},
   Key = {fds309020}
}

@article{fds309025,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
             C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
             U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland,
             W},
   Title = {Measurement of Z boson production in Pb-Pb collisions at
             sqrt[s(NN)]=2.76  TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {2},
   Pages = {022301},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.110.022301},
   Abstract = {The ATLAS experiment has observed 1995 Z boson candidates in
             data corresponding to 0.15  nb(-1) of integrated
             luminosity obtained in the 2011 LHC Pb+Pb run at
             sqrt[s(NN)]=2.76  TeV. The Z bosons are reconstructed
             via dielectron and dimuon decay channels, with a background
             contamination of less than 3%. Results from the two channels
             are consistent and are combined. Within the statistical and
             systematic uncertainties, the per-event Z boson yield is
             proportional to the number of binary collisions estimated by
             the Glauber model. The elliptic anisotropy of the azimuthal
             distribution of the Z boson with respect to the event plane
             is found to be consistent with zero.},
   Doi = {10.1103/physrevlett.110.022301},
   Key = {fds309025}
}

@article{fds309030,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
             E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
             V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
             P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates,
             RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
             Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
             O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
             Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
             JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
             G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC},
   Title = {Search for dark matter candidates and large extra dimensions
             in events with a photon and missing transverse momentum in
             pp collision data at sqrt[s]=7 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {1},
   Pages = {011802},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.110.011802},
   Abstract = {Results of a search for new phenomena in events with an
             energetic photon and large missing transverse momentum in
             proton-proton collisions at sqrt[s] = 7 TeV are reported.
             Data collected by the ATLAS experiment at the LHC
             corresponding to an integrated luminosity of 4.6 fb(-1) are
             used. Good agreement is observed between the data and the
             standard model predictions. The results are translated into
             exclusion limits on models with large extra spatial
             dimensions and on pair production of weakly interacting dark
             matter candidates.},
   Doi = {10.1103/physrevlett.110.011802},
   Key = {fds309030}
}

@article{fds309032,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
             DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
             AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
             V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN},
   Title = {Measurement of jet shapes in top-quark pair events at
             [Formula: see text] using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {73},
   Number = {12},
   Pages = {2676},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2676-3},
   Abstract = {A measurement of jet shapes in top-quark pair events using
             1.8 fb<sup>-1</sup> of [Formula: see text]<i>pp</i>
             collision data recorded by the ATLAS detector at the LHC is
             presented. Samples of top-quark pair events are selected in
             both the single-lepton and dilepton final states. The
             differential and integrated shapes of the jets initiated by
             bottom-quarks from the top-quark decays are compared with
             those of the jets originated by light-quarks from the
             hadronic <i>W</i>-boson decays [Formula: see text] in the
             single-lepton channel. The light-quark jets are found to
             have a narrower distribution of the momentum flow inside the
             jet area than <i>b</i>-quark jets.},
   Doi = {10.1140/epjc/s10052-013-2676-3},
   Key = {fds309032}
}

@article{fds309035,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of isolated-photon pair production in pp
             collisions at √s=7TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)086},
   Abstract = {The ATLAS experiment at the LHC has measured the production
             cross section of events with two isolated photons in the
             final state, in proton-proton collisions at √s=7TeV . The
             full data set collected in 2011, corresponding to an
             integrated luminosity of 4.9 fb-1, is used. The amount of
             background, from hadronic jets and isolated electrons, is
             estimated with data-driven techniques and subtracted. The
             total cross section, for two isolated photons with
             transverse energies above 25 GeV and 22 GeV respectively, in
             the acceptance of the electromagnetic calorimeter (|η| <
             1.37 and 1.52 < |η| < 2.37) and with an angular separation
             ΔR > 0.4, is 44.0-4.2+3.2 pb. The differential cross
             sections as a function of the di-photon invariant mass,
             transverse momentum, azimuthal separation, and cosine of the
             polar angle of the largest transverse energy photon in the
             Collins-Soper di-photon rest frame are also measured. The
             results are compared to the prediction of leading-order
             parton-shower and next-to-leading-order and
             next-to-next-to-leading-order parton-level
             generators.[Figure not available: see fulltext.] © 2013
             CERN for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP01(2013)086},
   Key = {fds309035}
}

@article{fds309040,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E and Arik, M and Armbruster, AJ},
   Title = {Measurement of the production cross section of jets in
             association with a Z boson in pp collisions at √s=7 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP07(2013)032},
   Abstract = {Measurements of the production of jets of particles in
             association with a Z boson in pp collisions at √s=7 TeV
             are presented, using data corresponding to an integrated
             luminosity of 4.6 fb-1 collected by the ATLAS experiment at
             the Large Hadron Collider. Inclusive and differential jet
             cross sections in Z events, with Z decaying into electron or
             muon pairs, are measured for jets with transverse momentum p
             T > 30 GeV and rapidity |y| < 4.4. The results are compared
             to next-to-leading-order perturbative QCD calculations, and
             to predictions from different Monte Carlo generators based
             on leading-order and next-to-leading-order matrix elements
             supplemented by parton showers. [Figure not available: see
             fulltext.] © 2013 CERN for the benefit of the ATLAS
             collaboration.},
   Doi = {10.1007/JHEP07(2013)032},
   Key = {fds309040}
}

@article{fds309041,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
             VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Search for third generation scalar leptoquarks in pp
             collisions at √s=7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2013)033},
   Abstract = {A search for pair-produced third generation scalar
             leptoquarks is presented, using proton-proton collisions at
             s=7 TeV at the LHC. The data were recorded with the ATLAS
             detector and correspond to an integrated luminosity of 4.7
             fb-1. Each leptoquark is assumed to decay to a tau lepton
             and a b-quark with a branching fraction equal to 100%. No
             statistically significant excess above the Standard Model
             expectation is observed. Third generation leptoquarks are
             therefore excluded at 95% confidence level for masses less
             than 534GeV. [Figure not available: see fulltext.] © 2013
             Cern for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP06(2013)033},
   Key = {fds309041}
}

@article{fds309081,
   Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
             W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
             A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
             L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
             ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
   Title = {Search for the Higgs boson in the all-hadronic final state
             using the full CDF data set},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {2},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP02(2013)004},
   Abstract = {This paper reports the result of a search for the standard
             model Higgs boson in events containing four reconstructed
             jets associated with quarks. For masses below 135 GeV/c 2,
             the Higgs boson decays to bottom-antibottom quark pairs are
             dominant and result primarily in two hadronic jets. An
             additional two jets can be produced in the hadronic decay of
             a W or Z boson produced in association with the Higgs boson,
             or from the incoming quarks that produced the Higgs boson
             through the vector-boson fusion process. The search is
             performed using a sample of √s=1.96 TeV proton-antiproton
             collisions corresponding to an integrated luminosity of 9.45
             fb-1 recorded by the CDF II detector. The data are in
             agreement with the background model and 95% credibility
             level upper limits on Higgs boson production are set as a
             function of the Higgs boson mass. The median expected
             (observed) limit for a 125 GeV/c 2 Higgs boson is 11.0 (9.0)
             times the predicted standard model rate. © 2013
             SISSA.},
   Doi = {10.1007/JHEP02(2013)004},
   Key = {fds309081}
}

@article{fds316870,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Triggers for displaced decays of long-lived neutral
             particles in the ATLAS detector},
   Journal = {Journal of Instrumentation},
   Volume = {8},
   Number = {7},
   Pages = {P07015-P07015},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {January},
   ISSN = {1748-0221},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000322572900026&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {A set of three dedicated triggers designed to detect
             long-lived neutral particles decaying throughout the ATLAS
             detector to a pair of hadronic jets is described. The
             efficiencies of the triggers for selecting displaced decays
             as a function of the decay position are presented for
             simulated events. The effect of pile-up interactions on the
             trigger efficiencies and the dependence of the trigger rate
             on instantaneous luminosity during the 2012 data-taking
             period at the LHC are discussed.},
   Doi = {10.1088/1748-0221/8/07/P07015},
   Key = {fds316870}
}

@article{fds321462,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {ATLAS search for new phenomena in dijet mass and angular
             distributions using pp collisions at √s = 7
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)029},
   Abstract = {Mass and angular distributions of dijets produced in LHC
             proton-proton collisions at a centre-of-mass energy √s =
             7TeV have been studied with the ATLAS detector using the
             full 2011 data set with an integrated luminosity of 4.8
             fb-1. Dijet masses up to ~ 4.0TeV have been probed. No
             resonance-like features have been observed in the dijet mass
             spectrum, and all angular distributions are consistent with
             the predictions of QCD. Exclusion limits on six hypotheses
             of new phenomena have been set at 95% CL in terms of mass or
             energy scale, as appropriate. These hypotheses include
             excited quarks below 2.83 TeV, colour octet scalars below
             1.86TeV, heavy W bosons below 1.68 TeV, string resonances
             below 3.61 TeV, quantum black holes with six extra
             space-time dimensions for quantum gravity scales below 4.11
             TeV, and quark contact interactions below a compositeness
             scale of 7.6 TeV in a destructive interference
             scenario.},
   Doi = {10.1007/JHEP01(2013)029},
   Key = {fds321462}
}

@article{fds316869,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S},
   Title = {Characterisation and mitigation of beam-induced backgrounds
             observed in the ATLAS detector during the 2011 proton-proton
             run},
   Journal = {Journal of Instrumentation},
   Volume = {8},
   Number = {7},
   Pages = {P07004-P07004},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {January},
   ISSN = {1748-0221},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000322572900015&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {This paper presents a summary of beam-induced backgrounds
             observed in the ATLAS detector and discusses methods to tag
             and remove background contaminated events in data.
             Triggerrate based monitoring of beam-related backgrounds is
             presented. The correlations of backgrounds with machine
             conditions, such as residual pressure in the beam-pipe, are
             discussed. Results from dedicated beam-background
             simulations are shown, and their qualitative agreement with
             data is evaluated. Data taken during the passage of
             unpaired, i.e. non-colliding, proton bunches is used to
             obtain background-enriched data samples. These are used to
             identify characteristic features of beam-induced
             backgrounds, which then are exploited to develop dedicated
             background tagging tools. These tools, based on observables
             in the Pixel detector, the muon spectrometer and the
             calorimeters, are described in detail and their efficiencies
             are evaluated. Finally an example of an application of these
             techniques to a monojet analysis is given, which
             demonstrates the importance of such event cleaning
             techniques for some new physics searches.},
   Doi = {10.1088/1748-0221/8/07/P07004},
   Key = {fds316869}
}

@article{fds309031,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {Measurement of the Bc-meson lifetime in the decay
             Bc-→J/ψπ},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.011101},
   Abstract = {The lifetime of the Bc- meson is measured using 272
             exclusive Bc-→J/ψ(→μ+μ-)π- decays reconstructed in
             data from proton-antiproton collisions corresponding to an
             integrated luminosity of 6.7 fb-1 recorded by the CDF II
             detector at the Fermilab Tevatron. The lifetime of the Bc-
             meson is measured to be τ(Bc-)=0.452±0.048(stat)±0.027(syst)
             ps. This is the first measurement of the Bc- meson lifetime
             in a fully reconstructed hadronic channel, and it agrees
             with previous results and has comparable precision. © 2013
             American Physical Society.},
   Doi = {10.1103/PhysRevD.87.011101},
   Key = {fds309031}
}

@article{fds309029,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for contact interactions and large extra dimensions
             in dilepton events from pp collisions at √s=7 TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.015010},
   Abstract = {A search for nonresonant new phenomena, originating from
             either contact interactions or large extra spatial
             dimensions, has been carried out using events with two
             isolated electrons or muons. These events, produced at the
             LHC in proton-proton collisions at √s=7 TeV, were recorded
             by the ATLAS detector. The data sample, collected throughout
             2011, corresponds to an integrated luminosity of 4.9 and 5.0
             fb-1 in the e+e - and μ+μ- channels, respectively. No
             significant deviations from the Standard Model expectation
             are observed. Using a Bayesian approach, 95% confidence
             level lower limits ranging from 9.0 to 13.9 TeV are placed
             on the energy scale of ℓℓqq contact interactions in the
             left-left isoscalar model. Lower limits ranging from 2.4 to
             3.9 TeV are also set on the string scale in large extra
             dimension models. After combining these limits with results
             from a similar search in the diphoton channel, slightly more
             stringent limits are obtained.},
   Doi = {10.1103/PhysRevD.87.015010},
   Key = {fds309029}
}

@article{fds309028,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ},
   Title = {Search for direct production of charginos and neutralinos in
             events with three leptons and missing transverse momentum in
             √s=7 TeV pp collisions with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {718},
   Number = {3},
   Pages = {841-859},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2012.11.039},
   Abstract = {A search for the direct production of charginos and
             neutralinos in final states with three electrons or muons
             and missing transverse momentum is presented. The analysis
             is based on 4.7 fb−1 of s=7 TeV proton–proton collision
             data delivered by the Large Hadron Collider and recorded
             with the ATLAS detector. Observations are consistent with
             Standard Model expectations in three signal regions that are
             either depleted or enriched in Z-boson decays. Upper limits
             at 95% confidence level are set in R-parity conserving
             phenomenological minimal supersymmetric models and in
             simplified models, significantly extending previous
             results.},
   Doi = {10.1016/j.physletb.2012.11.039},
   Key = {fds309028}
}

@article{fds309038,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurements of top quark pair relative differential
             cross-sections with ATLAS in pp collisions at √s = 7
             TeV},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {1},
   Pages = {1-28},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2261-1},
   Abstract = {Measurements are presented of differential crosss√ ections
             for top quark pair production in pp collisions at s = 7 TeV
             relative to the total inclusive top quark pair production
             cross-section. A data sample of 2.05 fb<sup>−1</sup>
             recorded by the ATLAS detector at the Large Hadron Collider
             is used. Relative differential cross-sections are derived as
             a function of the invariant mass, the transverse momentum
             and the rapidity of the top quark pair system. Events are
             selected in the lepton (electron or muon) + jets channel.
             The backgroundsubtracted differential distributions are
             corrected for detector effects, normalized to the total
             inclusive top quark pair production cross-section and
             compared to theoretical predictions. The measurement
             uncertainties range typically between 10 % and 20 % and are
             generally dominated by systematic effects. No significant
             deviations from the Standard Model expectations are
             observed.},
   Doi = {10.1140/epjc/s10052-012-2261-1},
   Key = {fds309038}
}

@article{fds309039,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim,
             A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Search for pair-produced massive coloured scalars in
             four-jet final states with the ATLAS detector in
             proton–proton collisions at √s =7 TeV},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {1},
   Pages = {1-20},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-012-2263-z},
   Abstract = {A search for pair-produced massive coloured scalar particles
             decaying to a four-jet final state is performed by the ATLAS
             experiment at the LHC in proton–proton collisions at √s
             = 7 TeV. The analysed data sample corresponds to an
             integrated luminosity of 4.6 fb<sup>−1</sup>. No deviation
             from the Standard Model is observed in the invariant mass
             spectrum of the two-jet pairs. A limit on the scalar gluon
             pair production cross section of 70 pb (10 pb) is obtained
             at the 95 % confidence level for a scalar gluon mass of 150
             GeV (350 GeV). Interpreting these results as mass limits on
             scalar gluons, masses ranging from 150 GeV to 287 GeV are
             excluded at the 95 % confidence level.},
   Doi = {10.1140/epjc/s10052-012-2263-z},
   Key = {fds309039}
}

@article{fds309023,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for squarks and gluinos with the ATLAS detector in
             final states with jets and missing transverse momentum using
             4.7 fb-1 of √s=7 TeV proton-proton collision
             data},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.012008},
   Abstract = {A search for squarks and gluinos in final states containing
             jets, missing transverse momentum and no high-pT electrons
             or muons is presented. The data represent the complete
             sample recorded in 2011 by the ATLAS experiment in 7 TeV
             proton-proton collisions at the Large Hadron Collider, with
             a total integrated luminosity of 4.7 fb-1. No excess above
             the Standard Model background expectation is observed.
             Gluino masses below 860 GeV and squark masses below 1320 GeV
             are excluded at the 95% confidence level in simplified
             models containing only squarks of the first two generations,
             a gluino octet and a massless neutralino, for squark or
             gluino masses below 2 TeV, respectively. Squarks and gluinos
             with equal masses below 1410 GeV are excluded. In minimal
             supergravity/constrained minimal supersymmetric Standard
             Model models with tanâ-¡β=10, A0=0 and μ>0, squarks and
             gluinos of equal mass are excluded for masses below 1360
             GeV. Constraints are also placed on the parameter space of
             supersymmetric models with compressed spectra. These limits
             considerably extend the region of supersymmetric parameter
             space excluded by previous measurements with the ATLAS
             detector.},
   Doi = {10.1103/PhysRevD.87.012008},
   Key = {fds309023}
}

@article{fds309018,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chou, JP and Chokheli,
             D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Funakoshi, Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hopkins, W and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
             KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leone, S and Lewis, JD and Limosani, A and Lipeles,
             E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
             J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty,
             R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki,
             D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore,
             R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini,
             M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
             E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
             A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi,
             G and Wagner, P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams,
             HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers,
             S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato,
             D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Observation of the production of a W boson in association
             with a single charm quark.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {7},
   Pages = {071801},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.110.071801},
   Abstract = {The first observation of the production of a W boson with a
             single charm quark (c) jet in pp[over ¯] collisions at
             √s=1.96  TeV is reported. The analysis uses data
             corresponding to 4.3  fb(-1), recorded with the CDF II
             detector at the Fermilab Tevatron. Charm quark candidates
             are selected through the identification of an electron or
             muon from charm-hadron semileptonic decay within a hadronic
             jet, and a Wc signal is observed with a significance of 5.7
             standard deviations. The production cross section
             σ(Wc)(p(Tc)>20  GeV/c,|η(c)|<1.5)×B(W→ℓν) is
             measured to be 13.6(-3.1)(+3.4)  pb and is in agreement
             with theoretical expectations. From this result the
             magnitude of the quark-mixing matrix element V(cs) is
             derived, |V(cs)|=1.08±0.16 along with a lower limit of
             |V(cs)|>0.71 at the 95% confidence level, assuming that the
             Wc production through c to s quark coupling is
             dominant.},
   Doi = {10.1103/physrevlett.110.071801},
   Key = {fds309018}
}

@article{fds309019,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the Λb0 lifetime and mass in the ATLAS
             experiment},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.032002},
   Abstract = {A measurement of the Λb0 lifetime and mass in the decay
             channel Λb0→J/ψ(μ+μ-)Λ0(pπ -) is presented. The
             analysis uses a signal sample of about 2200 Λb0 and Λ̄b0
             decays that are reconstructed in 4.9 fb -1 of ATLAS pp
             collision data collected in 2011 at the LHC center-of-mass
             energy of 7 TeV. A simultaneous mass and decay time maximum
             likelihood fit is used to extract the Λb0 lifetime and
             mass. They are measured to be τΛb=1.449±0.036(stat)
             ±0.017(syst) ps and mΛb=5619.7±0. 7(stat)±1.1(syst)
             MeV.},
   Doi = {10.1103/PhysRevD.87.032002},
   Key = {fds309019}
}

@article{fds309021,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
             N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M},
   Title = {Measurement of the flavour composition of dijet events in pp
             collisions at √s = 7 TeV with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {2},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2301-5},
   Abstract = {This paper describes a measurement of the flavour
             composition of dijet events produced in pp collisions at
             √s = 7 TeV using the ATLAS detector. The measurement uses
             the full 2010 data sample, corresponding to an integrated
             luminosity of 39 pb<sup>−1</sup>. Six possible
             combinations of light, charm and bottom jets are identified
             in the dijet events, where the jet flavour is defined by the
             presence of bottom, charm or solely light flavour hadrons in
             the jet. Kinematic variables, based on the properties of
             displaced decay vertices and optimised for jet flavour
             identification, are used in a multidimensional template fit
             to measure the fractions of these dijet flavour states as
             functions of the leading jet transverse momentum in the
             range 40 GeV to 500 GeV and jet rapidity |y| < 2.1. The fit
             results agree with the predictions of leading- and
             next-to-leading-order calculations, with the exception of
             the dijet fraction composed of bottom and light flavour
             jets, which is underestimated by all models at large
             transverse jet momenta. The ability to identify jets
             containing two b-hadrons, originating from e.g. gluon
             splitting, is demonstrated. The difference between bottom
             jet production rates in leading and subleading jets is
             consistent with the next-to-leading-order
             predictions.},
   Doi = {10.1140/epjc/s10052-013-2301-5},
   Key = {fds309021}
}

@article{fds309033,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Search for direct chargino production in anomaly-mediated
             supersymmetry breaking models based on a disappearing-track
             signature in pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)131},
   Abstract = {A search for direct chargino production in anomaly-mediated
             supersymmetry breaking scenarios is performed in pp
             collisions at √s=7TeV using 4.7 fb-1 of data collected
             with the ATLAS experiment at the LHC. In these models, the
             lightest chargino is predicted to have a lifetime long
             enough to be detected in the tracking detectors of collider
             experiments. This analysis explores such models by searching
             for chargino decays that result in tracks with few
             associated hits in the outer region of the tracking system.
             The transverse-momentum spectrum of candidate tracks is
             found to be consistent with the expectation from the
             Standard Model background processes and constraints on
             chargino properties are obtained. © 2013 CERN for the
             benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP01(2013)131},
   Key = {fds309033}
}

@article{fds309034,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for resonances decaying into top-quark pairs using
             fully hadronic decays in pp collisions with ATLAS at √s=7
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP01(2013)116},
   Abstract = {A search for resonances produced in 7 TeV proton-proton
             collisions and decaying into top-quark pairs is described.
             In this Letter events where the top-quark decay produces two
             massive jets with large transverse momenta recorded with the
             ATLAS detector at the Large Hadron Collider are considered.
             Two techniques that rely on jet substructure are used to
             separate top-quark jets from those arising from light quarks
             and gluons. In addition, each massive jet is required to
             have evidence of an associated bottom-quark decay. The data
             are consistent with the Standard Model, and limits can be
             set on the production cross section times branching fraction
             of a Z′ boson and a Kaluza-Klein gluon resonance. These
             limits exclude, at the 95% credibility level, Z′ bosons
             with masses 0.70-1.00 TeV as well as 1.28-1.32 TeV and
             Kaluza-Klein gluons with masses 0.70-1.62 TeV. © 2013 Cern
             for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP01(2013)116},
   Key = {fds309034}
}

@article{fds309017,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of W-boson polarization in top-quark decay using
             the full CDF Run II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.031104},
   Abstract = {We measure the polarization of W bosons from top-quark (t)
             decays into final states with a charged lepton and jets,
             tt̄→W+bW -b̄→ℓνbqq̄′b̄, using the full Run II
             data set collected by the CDF II detector, corresponding to
             an integrated luminosity of 8.7 fb-1. A model-independent
             method simultaneously determines the fraction of
             longitudinal (f0) and right-handed (f+) W bosons to yield
             f0=0.726±0. 066(stat)±0.067(syst) and f+=-0.045±0.044(stat)
             ±0.058(syst) with a correlation coefficient of -0.69.
             Additional results are presented under various standard
             model assumptions. No significant discrepancies with the
             standard model are observed. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.87.031104},
   Key = {fds309017}
}

@article{fds309012,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Search for long-lived, heavy particles in final states with
             a muon and multi-track displaced vertex in proton-proton
             collisions at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {719},
   Number = {4-5},
   Pages = {280-298},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.042},
   Abstract = {Many extensions of the Standard Model posit the existence of
             heavy particles with long lifetimes. In this Letter, results
             are presented of a search for events containing one or more
             such particles, which decay at a significant distance from
             their production point, using a final state containing
             charged hadrons and an associated muon. This analysis uses a
             data sample of proton-proton collisions at s=7TeV
             corresponding to an integrated luminosity of 4.4 fb−1
             collected in 2011 by the ATLAS detector operating at the
             Large Hadron Collider. Results are interpreted in the
             context of R-parity violating supersymmetric scenarios. No
             events in the signal region are observed and limits are set
             on the production cross section for pair production of
             supersymmetric particles, multiplied by the square of the
             branching fraction for a neutralino to decay to charged
             hadrons and a muon, based on the scenario where both of the
             produced supersymmetric particles give rise to neutralinos
             that decay in this way. However, since the search strategy
             is based on triggering on and reconstructing the decay
             products of individual long-lived particles, irrespective of
             the rest of the event, these limits can easily be
             reinterpreted in scenarios with different numbers of
             long-lived particles per event. The limits are presented as
             a function of neutralino lifetime, and for a range of squark
             and neutralino masses.},
   Doi = {10.1016/j.physletb.2013.01.042},
   Key = {fds309012}
}

@article{fds308998,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
             C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
             L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
             C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
             K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for resonant top-antitop production in the lepton
             plus jets decay mode using the full CDF data
             set.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {12},
   Pages = {121802},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.110.121802},
   Abstract = {This Letter reports a search for a narrow resonant state
             decaying into two W bosons and two b quarks where one W
             boson decays leptonically and the other decays into a
             quark-antiquark pair. The search is particularly sensitive
             to top-antitop resonant production. We use the full data
             sample of proton-antiproton collisions at a center-of-mass
             energy of 1.96 TeV collected by the CDF II detector at the
             Fermilab Tevatron, corresponding to an integrated luminosity
             of 9.45 fb(-1). No evidence for resonant production is
             found, and upper limits on the production cross section
             times branching ratio for a narrow resonant state are
             extracted. Within a specific benchmark model, we exclude a
             Z' boson with mass, M(Z'), below 915 GeV/c(2) decaying into
             a top-antitop pair at the 95% credibility level assuming a
             Z' boson decay width of Γ(Z') = 0.012 M(Z'). This is the
             most sensitive search for a narrow qq-initiated tt resonance
             in the mass region below 750 GeV/c(2).},
   Doi = {10.1103/physrevlett.110.121802},
   Key = {fds308998}
}

@article{fds308999,
   Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
             G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
             W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
             M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
             A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
             RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
             M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
             D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Johnstone, A and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
             T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
             Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
             Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Truong, A and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
             AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Search for a two-Higgs-boson doublet using a simplified
             model in pp collisions at sqrt[s] = 1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {12},
   Pages = {121801},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.110.121801},
   Abstract = {We present a search for new particles in an extension to the
             standard model that includes a heavy Higgs boson (H(0)), a
             lighter charged Higgs boson (H(±)), and an even lighter
             Higgs boson h(0), with decays leading to a W-boson pair and
             a bottom-antibottom quark pair in the final state. We use
             events with exactly one lepton, missing transverse momentum,
             and at least four jets in data corresponding to an
             integrated luminosity of 8.7 fb(-1) collected by the CDF II
             detector in proton-antiproton collisions at sqrt[s]= 1.96
             TeV. We find the data to be consistent with standard model
             predictions and report the results in terms of a simplified
             Higgs-cascade-decay model, setting 95% confidence level
             upper limits on the product of cross section and branching
             fraction from 1.3 pb to 15 fb as a function of H(0) and
             H(±) masses for m(h)(0) = 126 GeV/c(2).},
   Doi = {10.1103/physrevlett.110.121801},
   Key = {fds308999}
}

@article{fds309002,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
             EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
             A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Riddick, T and Rimondi,
             F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani,
             M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu,
             V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song,
             H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the cross section for prompt isolated
             diphoton production using the full CDF run II data
             sample.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {10},
   Pages = {101801},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.110.101801},
   Abstract = {This Letter reports a measurement of the cross section for
             producing pairs of central prompt isolated photons in
             proton-antiproton collisions at a total energy sqrt[s] =
             1.96 TeV using data corresponding to 9.5 fb(-1) integrated
             luminosity collected with the CDF II detector at the
             Fermilab Tevatron. The measured differential cross section
             is compared to three calculations derived from the theory of
             strong interactions. These include a prediction based on a
             leading order matrix element calculation merged with a
             parton shower model, a next-to-leading order calculation,
             and a next-to-next-to-leading order calculation. The first
             and last calculations reproduce most aspects of the data,
             thus showing the importance of higher-order contributions
             for understanding the theory of strong interaction and
             improving measurements of the Higgs boson and searches for
             new phenomena in diphoton final states.},
   Doi = {10.1103/physrevlett.110.101801},
   Key = {fds309002}
}

@article{fds309008,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of ZZ production in pp collisions at √ = 7 TeV
             and limits on anomalous ZZZ and ZZγ couplings with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2013)128},
   Abstract = {A measurement of the ZZ production cross section in
             proton-proton collisions at √ = 7 TeV using data recorded
             by the ATLAS experiment at the Large Hadron Collider is
             presented. In a data sample corresponding to an integrated
             luminosity of 4.6 fb-1 collected in 2011, events are
             selected that are consistent either with two Z bosons
             decaying to electrons or muons or with one Z boson decaying
             to electrons or muons and a second Z boson decaying to
             neutrinos. The ZZ → ℓ + ℓ - ℓ ′+ ℓ ′- and ZZ
             → ℓ + ℓ - ℓv̄v cross sections are measured in
             restricted phase-space regions. These results are then used
             to derive the total cross section for ZZ events produced
             with both Z bosons in the mass range 66 to 116 GeV, σZZtot
             = 6.7 ± 0.7 (stat.) -0.3+0.4 (stat.) ± 0.3 (lumi.) pb,
             which is consistent with the Standard Model prediction of
             5.89-0.18+0.22 pb calculated at next-to-leading order in
             QCD. The normalized differential cross sections in bins of
             various kinematic variables are presented. Finally, the
             differential event yield as a function of the transverse
             momentum of the leading Z boson is used to set limits on
             anomalous neutral triple gauge boson couplings in ZZ
             production. © 2013 Cern for the benefit of the ATLAS
             collaboration.},
   Doi = {10.1007/JHEP03(2013)128},
   Key = {fds309008}
}

@article{fds309010,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
             A and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
             T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
             MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
             M and Armbruster, AJ and Arnaez, O},
   Title = {Single hadron response measurement and calorimeter jet
             energy scale uncertainty with the ATLAS detector at the
             LHC},
   Journal = {European Physical Journal C},
   Volume = {73},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1140/epjc/s10052-013-2305-1},
   Abstract = {The uncertainty on the calorimeter energy response to jets
             of particles is derived for the ATLAS experiment at the
             Large Hadron Collider (LHC). First, the calorimeter response
             to single isolated charged hadrons is measured and compared
             to the Monte Carlo simulation using proton-proton collisions
             at centre-of-mass energies of √s = 900 GeV and 7 TeV
             collected during 2009 and 2010. Then, using the decay of
             K<inf>s</inf> and Λ particles, the calorimeter response to
             specific types of particles (positively and negatively
             charged pions, protons, and anti-protons) is measured and
             compared to the Monte Carlo predictions. Finally, the jet
             energy scale uncertainty is determined by propagating the
             response uncertainty for single charged and neutral
             particles to jets. The response uncertainty is 2–5 % for
             central isolated hadrons and 1–3 % for the final
             calorimeter jet energy scale.},
   Doi = {10.1140/epjc/s10052-013-2305-1},
   Key = {fds309010}
}

@article{fds309003,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for new phenomena in events with three charged
             leptons at √s=7 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052002},
   Abstract = {A generic search for anomalous production of events with at
             least three charged leptons is presented. The search uses a
             pp-collision data sample at a center-of-mass energy of
             √s=7 TeV corresponding to 4.6 fb-1 of integrated
             luminosity collected in 2011 by the ATLAS detector at the
             CERN Large Hadron Collider. Events are required to contain
             at least two electrons or muons, while the third lepton may
             either be an additional electron or muon, or a hadronically
             decaying tau lepton. Events are categorized by the presence
             or absence of a reconstructed tau-lepton or Z-boson
             candidate decaying to leptons. No significant excess above
             backgrounds expected from Standard Model processes is
             observed. Results are presented as upper limits on event
             yields from non-Standard-Model processes producing at least
             three prompt, isolated leptons, given as functions of lower
             bounds on several kinematic variables. Fiducial efficiencies
             for model testing are also provided. The use of the results
             is illustrated by setting upper limits on the production of
             doubly charged Higgs bosons decaying to same-sign lepton
             pairs.},
   Doi = {10.1103/PhysRevD.87.052002},
   Key = {fds309003}
}

@article{fds309004,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of upsilon production in 7 TeV pp collisions at
             ATLAS},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052004},
   Abstract = {Using 1.8 fb-1 of pp collisions at a center-of-mass energy
             of 7 TeV recorded by the ATLAS detector at the Large Hadron
             Collider, we present measurements of the production cross
             sections of Υ(1S,2S,3S) mesons. Υ mesons are reconstructed
             using the dimuon decay mode. Total production cross sections
             for pT<70 GeV and in the rapidity interval |yΥ|<2.25 are
             measured to be, 8.01±0.02±0.36±0.31 nb,
             2.05±0.01±0.12±0.08 nb, and 0.92±0.01±0. 07±0.04 nb,
             respectively, with uncertainties separated into statistical,
             systematic, and luminosity measurement effects. In addition,
             differential cross section times dimuon branching fractions
             for Υ(1S), Υ(2S), and Υ(3S) as a function of Υ
             transverse momentum pT and rapidity are presented. These
             cross sections are obtained assuming unpolarized production.
             If the production polarization is fully transverse or
             longitudinal with no azimuthal dependence in the helicity
             frame, the cross section may vary by approximately ±20%. If
             a nontrivial azimuthal dependence is considered, integrated
             cross sections may be significantly enhanced by a factor of
             2 or more. We compare our results to several theoretical
             models of Υ meson production, finding that none provide an
             accurate description of our data over the full range of Υ
             transverse momenta accessible with this data
             set.},
   Doi = {10.1103/PhysRevD.87.052004},
   Key = {fds309004}
}

@article{fds309024,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Updated search for the standard model Higgs boson in events
             with jets and missing transverse energy using the full CDF
             data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.052008},
   Abstract = {We present an updated search for the Higgs boson produced in
             association with a vector boson in the final state with
             missing transverse energy and two jets. We use the full CDF
             data set corresponding to an integrated luminosity of 9.45
             fb-1 at a proton-antiproton center-of-mass energy of
             √s=1.96 TeV. New to this analysis is the inclusion of a
             b-jet identification algorithm specifically optimized for
             H→bb̄ searches. Across the Higgs boson mass range
             90≤mH≤150 GeV/c2, the expected 95% credibility level
             upper limits on the VH production cross section times the
             H→bb̄ branching fraction are improved by an average of
             14% relative to the previous analysis. At a Higgs boson mass
             of 125 GeV/c2, the observed (expected) limit is 3.06 (3.33)
             times the standard model prediction, corresponding to one of
             the most sensitive searches to date in this final state. ©
             2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.87.052008},
   Key = {fds309024}
}

@article{fds309000,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for light top squark pair production in final states
             with leptons and b-jets with the ATLAS detector in √s=7
             TeV proton–proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {720},
   Number = {1-3},
   Pages = {13-31},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.049},
   Abstract = {The results of a search for pair production of light top
             squarks are presented, using 4.7 fb−1 of s=7 TeV
             proton–proton collisions collected with the ATLAS detector
             at the Large Hadron Collider. This search targets top
             squarks with masses similar to, or lighter than, the top
             quark mass. Final states containing exclusively one or two
             leptons (e,μ), large missing transverse momentum,
             light-flavour jets and b-jets are used to reconstruct the
             top squark pair system. Event-based mass scale variables are
             used to separate the signal from a large tt¯ background. No
             excess over the Standard Model expectations is found. The
             results are interpreted in the framework of the Minimal
             Supersymmetric Standard Model, assuming the top squark
             decays exclusively to a chargino and a b-quark, while
             requiring different mass relationships between the
             Supersymmetric particles in the decay chain. Light top
             squarks with masses between 123–167 GeV are excluded for
             neutralino masses around 55 GeV.},
   Doi = {10.1016/j.physletb.2013.01.049},
   Key = {fds309000}
}

@article{fds309001,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of angular correlations in Drell–Yan lepton
             pairs to probe Z/γ boson transverse momentum
             at √s=7 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {720},
   Number = {1-3},
   Pages = {32-51},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.01.054},
   Abstract = {A measurement of angular correlations in Drell–Yan lepton
             pairs via the ϕη⁎ observable is presented. This variable
             probes the same physics as the Z/γ⁎ boson transverse
             momentum with a better experimental resolution. The
             Z/γ⁎→e+e− and Z/γ⁎→μ+μ− decays produced in
             proton–proton collisions at a centre-of-mass energy of
             sqrts=7 TeV are used. The data were collected with the ATLAS
             detector at the LHC and correspond to an integrated
             luminosity of 4.6 fb−1. Normalised differential cross
             sections as a function of ϕη⁎ are measured separately
             for electron and muon decay channels. These channels are
             then combined for improved accuracy. The cross section is
             also measured double differentially as a function of ϕη⁎
             for three independent bins of the Z boson rapidity. The
             results are compared to QCD calculations and to predictions
             from different Monte Carlo event generators. The data are
             reasonably well described, in all measured Z boson rapidity
             regions, by resummed QCD predictions combined with
             fixed-order perturbative QCD calculations or by some Monte
             Carlo event generators. The measurement precision is
             typically better by one order of magnitude than present
             theoretical uncertainties.},
   Doi = {10.1016/j.physletb.2013.01.054},
   Key = {fds309001}
}

@article{fds321461,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Ochoa, MI and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurement of hard double-parton interactions in W(→ lν)
             + 2-jet events at √s = 7 TeV with the ATLAS
             detector},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {3},
   Pages = {033038-033038},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1088/1367-2630/15/3/033038},
   Abstract = {The production of W bosons in association with two jets in
             proton-proton collisions at a centre-of-mass energy of √ s
             = 7 TeV has been analysed for the presence of double-parton
             interactions using data corresponding to an integrated
             luminosity of 36 pb-1, collected with the ATLAS detector at
             the Large Hadron Collider. The fraction of events arising
             from double-parton interactions, f(D)DP, has been measured
             through the pT balance between the two jets and amounts to
             f(D)DP = 0.08 ±0.01 (stat.)±0.02 (sys.) for jets with
             transverse momentum pT > 20 GeV and rapidity |y| < 2.8. This
             corresponds to a measurement of the effective area parameter
             for hard double-parton interactions of σeff = 15 ± 3
             (stat.) +5-3 (sys.) mb.},
   Doi = {10.1088/1367-2630/15/3/033038},
   Key = {fds321461}
}

@article{fds333008,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Searches for heavy long-lived sleptons and R-hadrons with
             the ATLAS detector in pp collisions at √s=7
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {720},
   Number = {4-5},
   Pages = {277-308},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.02.015},
   Abstract = {A search for long-lived particles is performed using a data
             sample of 4.7 fb−1 from proton–proton collisions at a
             centre-of-mass energy s=7 TeV collected by the ATLAS
             detector at the LHC. No excess is observed above the
             estimated background and lower limits, at 95% confidence
             level, are set on the mass of the long-lived particles in
             different scenarios, based on their possible interactions in
             the inner detector, the calorimeters and the muon
             spectrometer. Long-lived staus in gauge-mediated
             SUSY-breaking models are excluded up to a mass of 300 GeV
             for tanβ=5–20. Directly produced long-lived sleptons are
             excluded up to a mass of 278 GeV. R-hadrons, composites of
             gluino (stop, sbottom) and light quarks, are excluded up to
             a mass of 985 GeV (683 GeV, 612 GeV) when using a generic
             interaction model. Additionally two sets of limits on
             R-hadrons are obtained that are less sensitive to the
             interaction model for R-hadrons. One set of limits is
             obtained using only the inner detector and calorimeter
             observables, and a second set of limits is obtained based on
             the inner detector alone.},
   Doi = {10.1016/j.physletb.2013.02.015},
   Key = {fds333008}
}

@article{fds308995,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Search for WH production with a light Higgs boson decaying
             to prompt electron-jets in proton-proton collisions at
             √s=7 TeV with the ATLAS detector},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {4},
   Pages = {043009-043009},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1367-2630/15/4/043009},
   Abstract = {A search is performed for WH production with a light Higgs
             boson decaying to hidden-sector particles resulting in
             clusters of collimated electrons, known as electron-jets.
             The search is performed with 2.04 fb-1 of data collected in
             2011 with the ATLAS detector at the Large Hadron Collider in
             proton-proton collisions at . One event satisfying the
             signal selection criteria is observed, which is consistent
             with the expected background rate. Limits on the product of
             the WH production cross section and the branching ratio of a
             Higgs boson decaying to prompt electron-jets are calculated
             as a function of a Higgs boson mass in the range from 100 to
             140 GeV. © CERN 2013 for the benefit of the ATLAS
             Collaboration, published under the terms of the Creative
             Commons Attribution 3.0 licence by IOP Publishing Ltd and
             Deutsche Physikalische Gesellschaft. Any further
             distribution of this work must maintain attribution to the
             author(s) and the published article's title, journal
             citation and DOI.},
   Doi = {10.1088/1367-2630/15/4/043009},
   Key = {fds308995}
}

@article{fds308996,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for extra dimensions in diphoton events from
             proton-proton collisions at √s= 7 TeV in the ATLAS
             detector at the LHC},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {4},
   Pages = {043007-043007},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1367-2630/15/4/043007},
   Abstract = {The large difference between the Planck scale and the
             electroweak scale, known as the hierarchy problem, is
             addressed in certain models through the postulate of extra
             spatial dimensions. A search for evidence of extra spatial
             dimensions in the diphoton channel has been performed using
             the full set of proton-proton collisions at √s = 7 TeV
             recorded in 2011 with the ATLAS detector at the CERN Large
             Hadron Collider. This dataset corresponds to an integrated
             luminosity of 4.9 fb1. The diphoton invariant mass spectrum
             is observed to be in good agreement with the Standard Model
             expectation. In the context of the model proposed by
             Arkani-Hamed, Dimopoulos and Dvali, 95% confidence level
             lower limits of between 2.52 and 3.92 TeV are set on the
             ultraviolet cutoff scale MS depending on the number of extra
             dimensions and the theoretical formalism used. In the
             context of the Randall-Sundrum model, a lower limit of 2.06
             (1.00) TeV at 95% confidence level is set on the mass of the
             lightest graviton for couplings of k/MPl = 0.1(0.01).
             Combining with the ATLAS dilepton searches based on the 2011
             data, the 95% confidence level lower limit on the
             Randall-Sundrum graviton mass is further tightened to 2.23
             (1.03) TeV for k/ MPl= 0.1(0.01).© CERN 2013 for the
             benefit of the ATLAS Collaboration.},
   Doi = {10.1088/1367-2630/15/4/043007},
   Key = {fds308996}
}

@article{fds308997,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Search for Bs0→μ+μ- and
             B0→μ+μ- decays with the full CDF
             Run II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.072003},
   Abstract = {We report on a search for Bs0→μ+μ- and B0→μ+μ-
             decays using proton-antiproton collision data at √s=1.96
             TeV corresponding to 10 fb-1 of integrated luminosity
             collected by the CDF II detector at the Fermilab Tevatron
             collider. The observed number of B0 candidates is consistent
             with background-only expectations and yields an upper limit
             on the branching fraction of B(B0→μ+μ-)<4.6×10-9 at 95%
             confidence level. We observe an excess of Bs0 candidates.
             The probability that the background processes alone could
             produce such an excess or larger is 0.94%. The probability
             that the combination of background and the expected standard
             model rate of Bs0→μ+μ- could produce such an excess or
             larger is 6.8%. These data are used to determine a branching
             fraction B(Bs0→μ+μ-)=(1.3-0.7+0.9) ×10-8 and provide an
             upper limit of B(Bs0→μ +μ-)<3.1×10-8 at 95% confidence
             level. © 2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.87.072003},
   Key = {fds308997}
}

@article{fds310548,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
   Title = {Search for displaced muonic lepton jets from light Higgs
             boson decay in proton–proton collisions at √s = 7 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {721},
   Number = {1-3},
   Pages = {32-50},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.02.058},
   Abstract = {A search is performed for collimated muon pairs displaced
             from the primary vertex produced in the decay of long-lived
             neutral particles in proton–proton collisions at s=7 TeV
             centre-of-mass energy, with the ATLAS detector at the LHC.
             In a 1.9 fb−1event sample collected during 2011, the
             observed data are consistent with the Standard Model
             background expectations. Limits on the product of the
             production cross section and the branching ratio of a Higgs
             boson decaying to hidden-sector neutral long-lived particles
             are derived as a function of the particlesʼ mean
             lifetime.},
   Doi = {10.1016/j.physletb.2013.02.058},
   Key = {fds310548}
}

@article{fds309007,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Joffe, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S and Arik, E and Arik, M},
   Title = {Search for charged Higgs bosons through the violation of
             lepton universality in tt events using pp collision data at
             √S=7 TeV with the ATLAS experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP03(2013)076},
   Abstract = {In several extensions of the Standard Model, the top quark
             can decay into a bottom quark and a light charged Higgs
             boson H +, t → bH +, in addition to the Standard Model
             decay t → bW. Since W bosons decay to the three lepton
             generations equally, while H + maypredominantlydecayinto
             τν, charged Higgs bosons can be searched for using the
             violation of lepton universality in top quark decays. The
             analysis in this paper is based on 4.6 fb-1 of proton-proton
             collision data at √s=7 TeV collected by the ATLAS
             experiment at the Large Hadron Collider. Signatures
             containing leptons (e or μ) and/or a hadronically decaying
             τ (τ had) are used. Event yield ratios between e + τ had
             and e + μ, as well as between μ + τ had andμ + e, final
             states are measured in the data and compared to predictions
             from simulations. This ratio-based method reduces the impact
             of systematic uncertainties in the analysis. No significant
             deviation from the Standard Model predictions is observed.
             With the assumption that the branching fraction ℬ (H + →
             τν) is 100%, upper limits in the range 3.2%-4.4% can be
             placed on the branching fraction ℬ (t → bH +) for
             charged Higgs boson masses m H+ in the range 90-140 GeV.
             After combination with results from a search for charged
             Higgs bosons in t\overline{t} decays using the τ had + jets
             final state, upper limits on ℬ (t → bH +) can be set in
             the range 0.8%-3.4%, for m H+ in the range 90-160
             GeV.[Figure not available: see fulltext.] © 2013 Cern for
             the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP03(2013)076},
   Key = {fds309007}
}

@article{fds309042,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim,
             A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for dark matter candidates and large extra dimensions
             in events with a jet and missing transverse momentum with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2013)075},
   Abstract = {A search for new phenomena in events with a high-energy jet
             and large missing transverse momentum is performed using
             data from proton-proton collisions at √s=7 TeV with the
             ATLAS experiment at the Large Hadron Collider. Four
             kinematic regions are explored using a dataset corresponding
             to an integrated luminosity of 4.7 fb-1. No excess of events
             beyond expectations from Standard Model processes is
             observed, and limits are set on large extra dimensions and
             the pair production of dark matter particles. © 2013 CERN,
             for the benefit of the ATLAS collaboration.},
   Doi = {10.1007/JHEP04(2013)075},
   Key = {fds309042}
}

@article{fds333007,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Ochoa, MI and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for single b-quark production with the
             ATLAS detector at √s=7 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {721},
   Number = {4-5},
   Pages = {171-189},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.03.016},
   Abstract = {The results of a search for an excited bottom-quark b⁎ in
             pp collisions at s=7 TeV, using 4.7 fb−1 of data collected
             by the ATLAS detector at the LHC are presented. In the model
             studied, a single b⁎-quark is produced through a
             chromomagnetic interaction and subsequently decays to a W
             boson and a top quark. The search is performed in the
             dilepton and lepton + jets final states, which are combined
             to set limits on b⁎-quark couplings for a range of
             b⁎-quark masses. For a benchmark with unit size
             chromomagnetic and Standard Model-like electroweak b⁎
             couplings, b⁎ quarks with masses less than 870 GeV are
             excluded at the 95% credibility level.},
   Doi = {10.1016/j.physletb.2013.03.016},
   Key = {fds333007}
}

@article{fds308992,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
             E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee,
             P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
             S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
             D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
             P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
             V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou,
             Y},
   Title = {Observation of associated near-side and away-side long-range
             correlations in sqrt[s(NN)]=5.02 TeV proton-lead collisions
             with the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {18},
   Pages = {182302},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.110.182302},
   Abstract = {Two-particle correlations in relative azimuthal angle (Δø)
             and pseudorapidity (Δη) are measured in sqrt[s(NN)] = 5.02
             TeV p+Pb collisions using the ATLAS detector at the LHC. The
             measurements are performed using approximately 1 μb(-1) of
             data as a function of transverse momentum (p(T)) and the
             transverse energy (ΣE(T)(Pb)) summed over 3.1 < η < 4.9 in
             the direction of the Pb beam. The correlation function,
             constructed from charged particles, exhibits a long-range (2
             < |Δ η | < 5) "near-side" (Δø ~ 0) correlation that
             grows rapidly with increasing ΣE(T)(Pb). A long-range
             "away-side" (Δø ~ π) correlation, obtained by subtracting
             the expected contributions from recoiling dijets and other
             sources estimated using events with small ΣE(T)(Pb), is
             found to match the near-side correlation in magnitude, shape
             (in Δη and Δø) and ΣE(T)(Pb) dependence. The resultant
             Δø correlation is approximately symmetric about π/2, and
             is consistent with a dominant cos2Δø modulation for all
             ΣE(T)(Pb) ranges and particle p(T).},
   Doi = {10.1103/physrevlett.110.182302},
   Key = {fds308992}
}

@article{fds309043,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for supersymmetry with like-sign lepton-tau events at
             CDF.},
   Journal = {Physical review letters},
   Volume = {110},
   Number = {20},
   Pages = {201802},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.110.201802},
   Abstract = {We present a search for chargino-neutralino associated
             production using like electric charge dilepton events
             collected by the CDF II detector at the Fermilab Tevatron in
             proton-antiproton collisions at sqrt[s] = 1.96 TeV. One
             lepton is identified as the hadronic decay of a tau lepton,
             while the other is an electron or muon. In data
             corresponding to 6.0 fb(-1) of integrated luminosity, we
             obtain good agreement with standard model predictions and
             set limits on the chargino-neutralino production cross
             section for simplified gravity- and gauge-mediated models.
             As an example, assuming that the chargino and neutralino
             decays to taus dominate, in the simplified gauge-mediated
             model we exclude cross sections greater than 300 fb at 95%
             credibility level for chargino and neutralino masses of 225
             GeV/c(2). This analysis is the first to extend the LHC
             searches for electroweak supersymmetric production of
             gauginos to high tanβ and slepton next-to-lightest
             supersymmetric particle scenarios.},
   Doi = {10.1103/physrevlett.110.201802},
   Key = {fds309043}
}

@article{fds308993,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of the top quark forward-backward production
             asymmetry and its dependence on event kinematic
             properties},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.092002},
   Abstract = {We present new measurements of the inclusive
             forward-backward tt̄ production asymmetry, AFB, and its
             dependence on several properties of the tt̄ system. The
             measurements are performed with the full Tevatron data set
             recorded with the CDF II detector during pp̄ collisions at
             √s=1.96 TeV, corresponding to an integrated luminosity of
             9.4 fb -1. We measure the asymmetry using the rapidity
             difference Δy=yt-yt̄. Parton-level results are derived,
             yielding an inclusive asymmetry of 0.164±0.047(stat+syst).
             We establish an approximately linear dependence of AFB on
             the top-quark pair mass Mtt̄ and the rapidity difference
             |Δy| at detector and parton levels. Assuming the standard
             model, the probabilities to observe the measured values or
             larger for the detector-level dependencies are 7.4×10-3 and
             2.2×10-3 for Mtt̄ and |Δy| respectively. Lastly, we study
             the dependence of the asymmetry on the transverse momentum
             of the tt̄ system at the detector level. These results are
             consistent with previous lower-precision measurements and
             provide additional quantification of the functional
             dependencies of the asymmetry. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.87.092002},
   Key = {fds308993}
}

@article{fds332095,
   Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
             JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
             D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
             B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
             B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
             V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
             K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
             F and D'Errico, M},
   Title = {W-boson polarization measurement in the tt- dilepton channel
             using the CDF II detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {722},
   Number = {1-3},
   Pages = {48-54},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.03.032},
   Abstract = {We present a measurement of the W-boson polarization in
             top-quark decays in tt- events with decays to dilepton final
             states using data corresponding to 5.1 fb-1 of integrated
             luminosity in pp- collisions collected by the CDF II
             detector at the Tevatron. Assuming a top-quark mass of 172.5
             GeV/c2, a simultaneous measurement of the fractions of
             longitudinal ( f0) and right-handed ( f+) W-bosons yields
             the results f0 = 0.70-0.17+0.18 (stat) ± 0.06(syst) and f+
             =-0.09 ± 0.09(stat) ± 0.03(syst). Combining this
             measurement with our previous measurement based on
             single-lepton final states, we obtain f0 = 0.84 ±
             0.09(stat) ± 0.05(syst) and f+ =-0.16 ± 0.05(stat) ±
             0.04(syst). The results are consistent with the standard
             model expectation.},
   Doi = {10.1016/j.physletb.2013.03.032},
   Key = {fds332095}
}

@article{fds333006,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
             ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S and Arik, E and Arik, M},
   Title = {Search for long-lived, multi-charged particles in pp
             collisions at √s=7 TeV using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {722},
   Number = {4-5},
   Pages = {305-323},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.04.036},
   Abstract = {A search for highly ionising, penetrating particles with
             electric charges from |q|=2e to 6e is performed using the
             ATLAS detector at the CERN Large Hadron Collider.
             Proton-proton collision data taken at s=7 TeV during the
             2011 running period, corresponding to an integrated
             luminosity of 4.4 fb−1, are analysed. No signal candidates
             are observed, and 95% confidence level cross-section upper
             limits are interpreted as mass-exclusion lower limits for a
             simplified Drell–Yan production model. In this model,
             masses are excluded from 50 GeV up to 430, 480, 490, 470 and
             420 GeV for charges 2e, 3e, 4e, 5e and 6e,
             respectively.},
   Doi = {10.1016/j.physletb.2013.04.036},
   Key = {fds333006}
}

@article{fds308988,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
             Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
             ATH and Arfaoui, S and Arguin, JF and Arik, E},
   Title = {Measurement of W+W- production in pp
             collisions at √s=7 TeV with the ATLAS detector and limits
             on anomalous WWZ and WWγ couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.112001},
   Abstract = {This paper presents a measurement of the W+W- production
             cross section in pp collisions at √s=7 TeV. The leptonic
             decay channels are analyzed using data corresponding to an
             integrated luminosity of 4.6 fb-1 collected with the ATLAS
             detector at the Large Hadron Collider. The W+W- production
             cross section σ(pp→W+W-+X) is measured to be
             51.9±2.0(stat)±3.9(syst)±2.0(lumi) pb, compatible with
             the Standard Model prediction of 44.7-1.9+2.1 pb. A
             measurement of the normalized fiducial cross section as a
             function of the leading lepton transverse momentum is also
             presented. The reconstructed transverse momentum
             distribution of the leading lepton is used to extract limits
             on anomalous WWZ and WWγ couplings.},
   Doi = {10.1103/PhysRevD.87.112001},
   Key = {fds308988}
}

@article{fds310547,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of R=B(t→Wb)/B(t→Wq) in top-quark-pair
             decays using lepton+jets events and the full CDF run II
             dataset},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.111101},
   Abstract = {We present a measurement of the ratio of the top-quark
             branching fractions R=B(t→Wb)/B(t→Wq), where q
             represents quarks of type b, s, or d, in the final state
             with a lepton and hadronic jets. The measurement uses
             √s=1.96 TeV proton-antiproton collision data from 8.7 fb-1
             of integrated luminosity collected with the Collider
             Detector at Fermilab during Run II of the Tevatron. We
             simultaneously measure R=0.94±0.09 (stat+syst) and the tt̄
             production cross section σtt̄=7. 5±1.0 (stat+syst) pb.
             The magnitude of the Cabibbo-Kobayashi-Maskawa matrix
             element, |Vtb|=0.97±0.05 (stat+syst) is extracted assuming
             three generations of quarks, and a lower limit of |V
             tb|>0.89 at 95% credibility level is set. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.87.111101},
   Key = {fds310547}
}

@article{fds308987,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Measurements of Wγ and Zγ production in pp collisions at
             √s=7 TeV with the ATLAS detector at the
             LHC},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {87},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.87.112003},
   Abstract = {The integrated and differential fiducial cross sections for
             the production of a W or Z boson in association with a
             high-energy photon are measured using pp collisions at
             √s=7 TeV. The analyses use a data sample with an
             integrated luminosity of 4.6 fb-1 collected by the ATLAS
             detector during the 2011 LHC data-taking period. Events are
             selected using leptonic decays of the W and Z bosons
             [W(eν,μν) and Z(e+e-, μ+μ-,νν¯)] with the
             requirement of an associated isolated photon. The data are
             used to test the electroweak sector of the Standard Model
             and search for evidence for new phenomena. The measurements
             are used to probe the anomalous WWγ, ZZγ, and Zγγ
             triple-gauge-boson couplings and to search for the
             production of vector resonances decaying to Zγ and Wγ. No
             deviations from Standard Model predictions are observed and
             limits are placed on anomalous triple-gauge-boson couplings
             and on the production of new vector meson
             resonances.},
   Doi = {10.1103/PhysRevD.87.112003},
   Key = {fds308987}
}

@article{fds333005,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
   Title = {Search for a heavy narrow resonance decaying to eμ eτ or
             μτ with the ATLAS detector in √s=7 TeV pp collisions at
             the LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {723},
   Number = {1-3},
   Pages = {15-32},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {June},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.04.035},
   Abstract = {This Letter presents the results of a search for a heavy
             particle decaying into an e±μ∓, e±τ∓, or μ±τ∓
             final state in pp collisions at s=7 TeV. The data were
             recorded with the ATLAS detector at the LHC during 2011 and
             correspond to an integrated luminosity of 4.6 fb−1. No
             significant excess above the Standard Model expectation is
             observed, and exclusions at 95% confidence level are placed
             on the cross section times branching ratio for the
             production of an R-parity-violating supersymmetric tau
             sneutrino. For a sneutrino mass of 500 (2000) GeV, the
             observed limits on the production cross section times
             branching ratio are 3.2 (1.4) fb, 42 (17) fb, and 40 (18) fb
             for the eμ eτ and μτ modes, respectively. These results
             considerably extend constraints from Tevatron
             experiments.},
   Doi = {10.1016/j.physletb.2013.04.035},
   Key = {fds333005}
}

@article{fds308981,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Search for nonpointing photons in the diphoton and ETmiss
             final state in √s=7 TeV proton-proton collisions using the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.012001},
   Abstract = {A search has been performed for photons originating in the
             decay of a neutral long-lived particle, exploiting the
             capabilities of the ATLAS electromagnetic calorimeter to
             make precise measurements of the flight direction of
             photons, as well as the calorimeter's excellent time
             resolution. The search has been made in the diphoton plus
             missing transverse energy final state, using the full data
             sample of 4.8 fb-1 of 7 TeV proton-proton collisions
             collected in 2011 with the ATLAS detector at the LHC. No
             excess is observed above the background expected from
             Standard Model processes. The results are used to set
             exclusion limits in the context of gauge mediated
             supersymmetry breaking models, with the lightest neutralino
             being the next-to-lightest supersymmetric particle and
             decaying with a lifetime in excess of 0.25 ns into a photon
             and a gravitino. © 2013 CERN.},
   Doi = {10.1103/PhysRevD.88.012001},
   Key = {fds308981}
}

@article{fds308982,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Top-quark mass measurement in events with jets and missing
             transverse energy using the full CDF data
             set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.011101},
   Abstract = {We present a measurement of the top-quark mass using the
             full data set of Tevatron √s=1.96 TeV proton-antiproton
             collisions recorded by the CDF II detector, corresponding to
             an integrated luminosity of 8.7 fb-1. The analysis uses
             events with one semileptonic t or t̄ decay, but without
             detection of the electron or muon. We select events with
             significant missing transverse energy and multiple jets. We
             veto events containing identified electrons or muons. We
             obtain distributions of the top-quark masses and the
             invariant mass of the two jets from W-boson decays from data
             and compare these to templates derived from signal and
             background samples to extract the top-quark mass and the
             energy scale of the calorimeter jets with in situ
             calibration. A likelihood fit of the templates from signal
             and background events to the data yields the top-quark mass,
             Mtop=173.93±1.64(stat)±0. 87(syst) GeV/c2. This result is
             the most precise measurement to date of the mass of the top
             quark in this event topology. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.011101},
   Key = {fds308982}
}

@article{fds308983,
   Author = {Aaltonen, T and Albin, E and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
             A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
             F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
             C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
             L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
             C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
             K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
             JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for pair production of strongly interacting particles
             decaying to pairs of jets in pp collisions at √s=1.96
             TeV.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {3},
   Pages = {031802},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.111.031802},
   Abstract = {We present a search for the pair production of a narrow
             nonstandard-model strongly interacting particle that decays
             to a pair of quarks or gluons, leading to a final state with
             four hadronic jets. We consider both nonresonant production
             via an intermediate gluon as well as resonant production via
             a distinct nonstandard-model intermediate strongly
             interacting particle. We use data collected by the CDF
             experiment in proton-antiproton collisions at √[s]=1.96
             TeV corresponding to an integrated luminosity of 6.6 fb(-1).
             We find the data to be consistent with nonresonant
             production. We report limits on σ(pp[over ¯]→jjjj) as a
             function of the masses of the hypothetical intermediate
             particles. Upper limits on the production cross sections for
             nonstandard-model particles in several resonant and
             nonresonant processes are also derived.},
   Doi = {10.1103/physrevlett.111.031802},
   Key = {fds308983}
}

@article{fds308984,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
             N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
             YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the cross section for direct-photon
             production in association with a heavy quark in pp[over ¯]
             collisions at sqrt[s]=1.96  TeV.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {4},
   Pages = {042003},
   Year = {2013},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.111.042003},
   Abstract = {We report on a measurement of the cross section for
             direct-photon production in association with a heavy quark
             using the full data set of sqrt[s]=1.96  TeV
             proton-antiproton collisions corresponding to 9.1  fb-1
             of integrated luminosity collected by the CDF II detector at
             the Fermilab Tevatron. The measurements are performed as a
             function of the photon transverse momentum, covering a
             photon transverse momentum between 30 and 300 GeV, photon
             rapidities |yγ|<1.0, a heavy-quark-jet transverse momentum
             pTjet>20  GeV, and jet rapidities |yjet|<1.5. The
             results are compared with several theoretical
             predictions.},
   Doi = {10.1103/physrevlett.111.042003},
   Key = {fds308984}
}

@article{fds308977,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar,
             R},
   Title = {Exclusion of exotic top-like quarks with -4/3 electric
             charge using jet-charge tagging in single-lepton tt̄ events
             at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {3},
   Pages = {032003},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.032003},
   Abstract = {We report on a measurement of the top-quark electric charge
             in tt̄ events in which one W boson originating from the
             top-quark pair decays into leptons and the other into
             hadrons. The event sample was collected by the CDF II
             detector in √s=1.96 TeV proton-antiproton collisions and
             corresponds to 5.6 fb-1. We find the data to be consistent
             with the standard model and exclude the existence of an
             exotic quark with -4/3 electric charge and mass of the
             conventional top quark at the 99% confidence level. © 2013
             American Physical Society.},
   Doi = {10.1103/PhysRevD.88.032003},
   Key = {fds308977}
}

@article{fds308976,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
             PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of charged-particle event shape variables in
             inclusive √(s)=7 TeV proton-proton interactions with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.032004},
   Abstract = {The measurement of charged-particle event shape variables is
             presented in inclusive inelastic pp collisions at a
             center-of-mass energy of 7 TeV using the ATLAS detector at
             the LHC. The observables studied are the transverse thrust,
             thrust minor, and transverse sphericity, each defined using
             the final-state charged particles' momentum components
             perpendicular to the beam direction. Events with at least
             six charged particles are selected by a minimum-bias
             trigger. In addition to the differential distributions, the
             evolution of each event shape variable as a function of the
             leading charged-particle transverse momentum,
             charged-particle multiplicity, and summed transverse
             momentum is presented. Predictions from several Monte Carlo
             models show significant deviations from data. © 2013 CERN.
             Published by the American Physical Society.},
   Doi = {10.1103/PhysRevD.88.032004},
   Key = {fds308976}
}

@article{fds309632,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Measurement with the ATLAS detector of multi-particle
             azimuthal correlations in p + Pb collisions at
             √sNN= 5.02 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {725},
   Number = {1-3},
   Pages = {60-78},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.06.057},
   Abstract = {In order to study further the long-range correlations
             ("ridge") observed recently in p + Pb collisions at √sNN=
             5.02 TeV, the second-order azimuthal anisotropy parameter of
             charged particles, v2, has been measured with the cumulant
             method using the ATLAS detector at the LHC. In a data sample
             corresponding to an integrated luminosity of approximately 1
             μb-1, the parameter v2has been obtained using two- and
             four-particle cumulants over the pseudorapidity range
             |η|<2.5. The results are presented as a function of
             transverse momentum and the event activity, defined in terms
             of the transverse energy summed over 3.1 < η <4.9 in the
             direction of the Pb beam. They show features characteristic
             of collective anisotropic flow, similar to that observed in
             Pb + Pb collisions. A comparison is made to results obtained
             using two-particle correlation methods, and to predictions
             from hydrodynamic models of p +Pb collisions. Despite the
             small transverse spatial extent of the p + Pb collision
             system, the large magnitude of v2and its similarity to
             hydrodynamic predictions provide additional evidence for the
             importance of final-state effects in p + Pb reactions. ©
             2013 CERN. Published by Elsevier B.V.},
   Doi = {10.1016/j.physletb.2013.06.057},
   Key = {fds309632}
}

@article{fds308975,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Signature-based search for delayed photons in exclusive
             photon plus missing transverse energy events from pp̄
             collisions with √s=1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {3},
   Pages = {031103},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.031103},
   Abstract = {We present the first signature-based search for delayed
             photons using an exclusive photon plus missing transverse
             energy final state. Events are reconstructed in a data
             sample from the CDF II detector corresponding to 6.3 fb-1 of
             integrated luminosity from √s=1.96 TeV proton-antiproton
             collisions. Candidate events are selected if they contain a
             photon with an arrival time in the detector larger than
             expected from a promptly produced photon. The mean number of
             events from standard model sources predicted by the
             data-driven background model based on the photon timing
             distribution is 286±24. A total of 322 events are observed.
             A p value of 12% is obtained, showing consistency of the
             data with standard model predictions. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.88.031103},
   Key = {fds308975}
}

@article{fds308974,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and AlvarezGonzalez, B and Alviggi, MG and Amako, K and AmaralCoutinho, Y and Amelung, C and Ammosov, VV and AmorDosSantos, SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and AperioBella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
             M},
   Title = {Evidence for the spin-0 nature of the Higgs boson using
             ATLAS data},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {726},
   Number = {1-3},
   Pages = {120-144},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.08.026},
   Abstract = {Studies of the spin and parity quantum numbers of the Higgs
             boson are presented, based on proton-proton collision data
             collected by the ATLAS experiment at the LHC. The Standard
             Model spin-parity JP=0+ hypothesis is compared with
             alternative hypotheses using the Higgs boson decays
             H→γγ, H→ZZ*→4ℓ and H→WW*→ℓνℓν, as well
             as the combination of these channels. The analysed dataset
             corresponds to an integrated luminosity of 20.7 fb-1
             collected at a centre-of-mass energy of s=8TeV. For the
             H→ZZ*→4ℓ decay mode the dataset corresponding to an
             integrated luminosity of 4.6 fb-1 collected at s=7TeV is
             included. The data are compatible with the Standard Model
             JP=0+ quantum numbers for the Higgs boson, whereas all
             alternative hypotheses studied in this Letter, namely some
             specific JP=0-, 1+, 1-, 2+ models, are excluded at
             confidence levels above 97.8%. This exclusion holds
             independently of the assumptions on the coupling strengths
             to the Standard Model particles and in the case of the JP=2+
             model, of the relative fractions of gluon-fusion and
             quark-antiquark production of the spin-2 particle. The data
             thus provide evidence for the spin-0 nature of the Higgs
             boson, with positive parity being strongly preferred. ©
             2013 CERN.},
   Doi = {10.1016/j.physletb.2013.08.026},
   Key = {fds308974}
}

@article{fds308967,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
   Title = {Performance of jet substructure techniques for large-R jets
             in proton-proton collisions at √s=7 TeV using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2013)076},
   Abstract = {This paper presents the application of a variety of
             techniques to study jet substructure. The performance of
             various modified jet algorithms, or jet grooming techniques,
             for several jet types and event topologies is investigated
             for jets with transverse momentum larger than 300 GeV.
             Properties of jets subjected to the mass-drop filtering,
             trimming, and pruning algorithms are found to have a reduced
             sensitivity to multiple proton-proton interactions, are more
             stable at high luminosity and improve the physics potential
             of searches for heavy boosted objects. Studies of the
             expected discrimination power of jet mass and jet
             substructure observables in searches for new physics are
             also presented. Event samples enriched in boosted W and Z
             bosons and top-quark pairs are used to study both the
             individual jet invariant mass scales and the efficacy of
             algorithms to tag boosted hadronic objects. The analyses
             presented use the full 2011 ATLAS dataset, corresponding to
             an integrated luminosity of 4.7 ± 0.1 fb-1 from
             proton-proton collisions produced by the Large Hadron
             Collider at a centre-of-mass energy of √s=7 TeV. [Figure
             not available: see fulltext.] © 2013 Cern for the benefit
             of the ATLAS collaboration.},
   Doi = {10.1007/JHEP09(2013)076},
   Key = {fds308967}
}

@article{fds308972,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for excited electrons and muons in √s=8 TeV
             proton-proton collisions with the ATLAS detector},
   Journal = {New Journal of Physics},
   Volume = {15},
   Number = {9},
   Pages = {093011-093011},
   Publisher = {IOP Publishing},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1088/1367-2630/15/9/093011},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for excited electrons and excited muons in the
             channel pp → ℓℓ* → ℓℓγ, assuming that excited
             leptons are produced via contact interactions. The analysis
             is based on 13 fb-1 of pp collisions at a centre-of-mass
             energy of 8 TeV. No evidence for excited leptons is found,
             and a limit is set at the 95% credibility level on the cross
             section times branching ratio as a function of the
             excited-lepton mass mℓ*. For mℓ* 0.8 TeV, the respective
             upper limits on σB(ℓ* → ℓγ) are 0.75 and 0.90 fb for
             the e* and μ* searches. Limits on σB are converted into
             lower bounds on the compositeness scale Λ. In the special
             case where Λ = m ℓ*, excited-electron and excited-muon
             masses below 2.2 TeV are excluded. © CERN
             2013.},
   Doi = {10.1088/1367-2630/15/9/093011},
   Key = {fds308972}
}

@article{fds308973,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
             M},
   Title = {Measurements of Higgs boson production and couplings in
             diboson final states with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {726},
   Number = {1-3},
   Pages = {88-119},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.08.010},
   Abstract = {Measurements are presented of production properties and
             couplings of the recently discovered Higgs boson using the
             decays into boson pairs, H→γγ, H→ZZ*→4ℓ and
             H→WW*→ℓνℓν. The results are based on the complete
             pp collision data sample recorded by the ATLAS experiment at
             the CERN Large Hadron Collider at centre-of-mass energies of
             s=7 TeV and s=8 TeV, corresponding to an integrated
             luminosity of about 25 fb-1. Evidence for Higgs boson
             production through vector-boson fusion is reported. Results
             of combined fits probing Higgs boson couplings to fermions
             and bosons, as well as anomalous contributions to
             loop-induced production and decay modes, are presented. All
             measurements are consistent with expectations for the
             Standard Model Higgs boson. © 2013 CERN.},
   Doi = {10.1016/j.physletb.2013.08.010},
   Key = {fds308973}
}

@article{fds308969,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
             A},
   Title = {Higgs boson studies at the Tevatron},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052014},
   Abstract = {We combine searches by the CDF and D0 Collaborations for the
             standard model Higgs boson with mass in the range 90-200
             GeV/c2 produced in the gluon-gluon fusion, WH, ZH, tt̄H,
             and vector boson fusion processes, and decaying in the
             H→bb̄, H→W+W-, H→ZZ, H→τ+τ-, and H→γγ modes.
             The data correspond to integrated luminosities of up to 10
             fb-1 and were collected at the Fermilab Tevatron in pp̄
             collisions at √s=1.96 TeV. The searches are also
             interpreted in the context of fermiophobic and fourth
             generation models. We observe a significant excess of events
             in the mass range between 115 and 140 GeV/c2. The local
             significance corresponds to 3.0 standard deviations at
             mH=125 GeV/c2, consistent with the mass of the Higgs boson
             observed at the LHC, and we expect a local significance of
             1.9 standard deviations. We separately combine searches for
             H→bb̄, H→W +W-, H→τ+τ-, and H→γγ. The observed
             signal strengths in all channels are consistent with the
             presence of a standard model Higgs boson with a mass of 125
             GeV/c2. © 2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.88.052014},
   Key = {fds308969}
}

@article{fds308970,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bertoli, G and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
             S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci, MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina,
             K},
   Title = {Searches for the Higgs boson decaying to W+W
             -→ℓ+νℓ-ν̄ with the
             CDF II detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052012},
   Abstract = {We present a search for a standard model Higgs boson
             decaying to two W bosons that decay to leptons using the
             full data set collected with the CDF II detector in
             √s=1.96 TeV pp̄ collisions at the Fermilab Tevatron,
             corresponding to an integrated luminosity of 9.7 fb-1. We
             obtain no evidence for production of a standard model Higgs
             boson with mass between 110 and 200 GeV/c2, and place upper
             limits on the production cross section within this range. We
             exclude standard model Higgs boson production at the 95%
             confidence level in the mass range between 149 and 172
             GeV/c2, while expecting to exclude, in the absence of
             signal, the range between 155 and 175 GeV/c2. We also
             interpret the search in terms of standard model Higgs boson
             production in the presence of a fourth generation of
             fermions and within the context of a fermiophobic Higgs
             boson model. For the specific case of a standard-model-like
             Higgs boson in the presence of fourth-generation fermions,
             we exclude at the 95% confidence level Higgs boson
             production in the mass range between 124 and 200 GeV/c2,
             while expecting to exclude, in the absence of signal, the
             range between 124 and 221 GeV/c2. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.052012},
   Key = {fds308970}
}

@article{fds308971,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
             M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Combination of searches for the Higgs boson using the full
             CDF data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052013},
   Abstract = {We present a combination of searches for the standard model
             Higgs boson using the full CDF run II data set, which
             corresponds to an integrated luminosity of 9.45-10.0 fb-1
             collected from √s=1.96 TeV pp̄ collisions at the Fermilab
             Tevatron. The searches consider Higgs boson production from
             gluon-gluon fusion, vector-boson fusion, and associated
             production with either a W or Z boson or a tt̄ pair.
             Depending on the production mode, Higgs boson decays to
             W+W-, ZZ, bb̄, τ+τ-, and γγ are examined. We search for
             a Higgs boson with masses (mH) in the range 90-200 GeV/c2.
             In the absence of a signal, we expect based on combined
             search sensitivity to exclude at the 95% credibility level
             the mass regions 90<mH<94 GeV/c2, 96<mH<106 GeV/c2, and
             153<mH<175 GeV/c2. The observed exclusion regions are
             90<mH<102 GeV/c2 and 149<mH<172 GeV/c2. A moderate excess of
             signal-like events relative to the background expectation at
             the level of 2.0 standard deviations is present in the data
             for the mH=125 GeV/c2 search hypothesis. We also present
             interpretations of the data within the context of a
             fermiophobic model and an alternative standard model
             incorporating a fourth generation of fermions. Finally, for
             the hypothesis of a new particle with mass 125 GeV/c2, we
             constrain the coupling strengths of the new particle to W±
             bosons, Z bosons, and fermions. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.052013},
   Key = {fds308971}
}

@article{fds308968,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Beecher, D and Begalli, M and Behari, S and Bellantoni,
             L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon,
             M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti,
             A and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Boudreau, J and Boveia,
             A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg,
             C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd,
             HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P},
   Title = {Combination of CDF and D0 W-Boson mass measurements},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {5},
   Pages = {052018},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.052018},
   Abstract = {We summarize and combine direct measurements of the mass of
             the W boson in √s=1.96 TeV proton-antiproton collision
             data collected by CDF and D0 experiments at the Fermilab
             Tevatron Collider. Earlier measurements from CDF and D0 are
             combined with the two latest, more precise measurements: a
             CDF measurement in the electron and muon channels using data
             corresponding to 2.2 fb-1 of integrated luminosity, and a D0
             measurement in the electron channel using data corresponding
             to 4.3 fb-1 of integrated luminosity. The resulting Tevatron
             average for the mass of the W boson is M W=80387±16 MeV.
             Including measurements obtained in electron-positron
             collisions at LEP yields the most precise value of M
             W=80385±15 MeV. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.052018},
   Key = {fds308968}
}

@article{fds308960,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
             M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
             M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
             OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
             M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
             G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
             FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
             R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN},
   Title = {Measurement of the azimuthal angle dependence of inclusive
             jet yields in Pb+Pb collisions at √(sNN)=2.76 TeV with the
             ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {15},
   Pages = {152301},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.111.152301},
   Abstract = {Measurements of the variation of inclusive jet suppression
             as a function of relative azimuthal angle, Δφ, with
             respect to the elliptic event plane provide insight into the
             path-length dependence of jet quenching. ATLAS has measured
             the Δφ dependence of jet yields in 0.14 nb(-1) of
             √(s(NN))=2.76 TeV Pb+Pb collisions at the LHC for jet
             transverse momenta p(T)>45 GeV in different collision
             centrality bins using an underlying event subtraction
             procedure that accounts for elliptic flow. The variation of
             the jet yield with Δφ was characterized by the parameter,
             v(2)(jet), and the ratio of out-of-plane (Δφ~π/2) to
             in-plane (Δφ~0) yields. Nonzero v(2)(jet) values were
             measured in all centrality bins for p(T)<160 GeV. The jet
             yields are observed to vary by as much as 20% between
             in-plane and out-of-plane directions.},
   Doi = {10.1103/physrevlett.111.152301},
   Key = {fds308960}
}

@article{fds308964,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Search for microscopic black holes in a like-sign dimuon
             final state using large track multiplicity with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.072001},
   Abstract = {A search is presented for microscopic black holes in a
             like-sign dimuon final state in proton-proton collisions at
             √s=8 TeV. The data were collected with the ATLAS detector
             at the Large Hadron Collider in 2012 and correspond to an
             integrated luminosity of 20.3 fb-1. Using a high track
             multiplicity requirement, 0.6±0.2 background events from
             Standard Model processes are predicted and none observed.
             This result is interpreted in the context of low-scale
             gravity models and 95% C.L. lower limits on microscopic
             black hole masses are set for different model assumptions.
             © 2013 CERN. Published by the American Physical Society
             under the terms of the Creative Commons Attribution 3.0
             License. Further distribution of this work must maintain
             attribution to the author(s) and the published article's
             title, journal citation, and DOI.},
   Doi = {10.1103/PhysRevD.88.072001},
   Key = {fds308964}
}

@article{fds308965,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger,
             J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
             YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz,
             D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Evidence for a bottom baryon resonance Λb*0 in CDF
             data},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Pages = {071101},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.071101},
   Abstract = {Using data from proton-antiproton collisions at √s=1.96
             TeV recorded by the CDF II detector at the Fermilab
             Tevatron, evidence for the excited resonance state Λb*0 is
             presented in its Λb0π -π+ decay followed by the Λb0→Λ
             c+π- and Λc+→pK-π+ decays. The analysis is based on a
             data sample corresponding to an integrated luminosity of 9.6
             fb-1 collected by an online event selection based on
             charged-particle tracks displaced from the proton-antiproton
             interaction point. The significance of the observed signal
             is 3.5σ. The mass of the observed state is found to be
             5919.22±0.76 MeV/c2 in agreement with similar findings in
             proton-proton collision experiments. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.88.071101},
   Key = {fds308965}
}

@article{fds309037,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Measurement of the high-mass Drell–Yan differential
             cross-section in pp collisions at √s=7TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {725},
   Number = {4-5},
   Pages = {223-242},
   Publisher = {Elsevier BV},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.07.049},
   Abstract = {This Letter reports a measurement of the high-mass
             Drell–Yan differential cross-section in proton–proton
             collisions at a centre-of-mass energy of 7 TeV at the LHC.
             Based on an integrated luminosity of 4.9 fb−1, the
             differential cross-section in the Z/γ⁎→e+e− channel
             is measured with the ATLAS detector as a function of the
             invariant mass, mee, in the range 116 <mee <1500 GeV, for a
             fiducial region in which both the electron and the positron
             have transverse momentum pT >25 GeV and pseudorapidity |η|
             <2.5. A comparison is made to various event generators and
             to the predictions of perturbative QCD calculations at
             next-to-next-to-leading order.},
   Doi = {10.1016/j.physletb.2013.07.049},
   Key = {fds309037}
}

@article{fds310544,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Search for new phenomena in final states with large jet
             multiplicities and missing transverse momentum at √s = 8
             TeV proton-proton collisions using the ATLAS
             experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {10},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1007/JHEP10(2013)130},
   Abstract = {A search is presented for new particles decaying to large
             numbers (7 or more) of jets, with missing transverse
             momentum and no isolated electrons or muons. This analysis
             uses 20:3 fb-1 of pp collision data at √s = 8 TeV
             collected by the ATLAS experiment at the Large Hadron
             Collider. The sensitivity of the search is enhanced by
             considering the number of b-tagged jets and the scalar sum
             of masses of large-radius jets in an event. No evidence is
             found for physics beyond the Standard Model. The results are
             interpreted in the context of various simplified
             supersymmetry-inspired models where gluinos are pair
             produced, as well as an mSUGRA/CMSSM model. © SISSA
             2013.},
   Doi = {10.1007/JHEP10(2013)130},
   Key = {fds310544}
}

@article{fds308963,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Indirect measurement of sin2θw (MW)
             using e+e- pairs in the Z-boson region
             with p̄p collisions at a center-of-momentum energy of 1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.072002},
   Abstract = {Drell-Yan lepton pairs are produced in the process p̄p→e
             +e-+X through an intermediate γ*/Z boson. The lepton
             angular distributions are used to provide information on the
             electroweak-mixing parameter sin2θw via its observable
             effective-leptonic sin2θw, or sinâ¡2θefflept. A new
             method to infer sin 2θw or, equivalently, the W-boson mass
             MW in the on-shell scheme, is developed and tested using a
             previous CDF Run II measurement of angular distributions
             from electron pairs in a sample corresponding to 2.1 fb-1 of
             integrated luminosity from p̄p collisions at a
             center-of-momentum energy of 1.96 TeV. The value of
             sinâ¡2θefflept is found to be 0.2328±0.0011. Within a
             specified context of the standard model, this results in sin
             2θw=0.2246±0.0011, which corresponds to a W-boson mass of
             80.297±0.055 GeV/c2, in agreement with previous
             determinations in electron-position collisions and at the
             Tevatron collider. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.072002},
   Key = {fds308963}
}

@article{fds308961,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Measurement of the leptonic asymmetry in tt̄ events
             produced in pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.072003},
   Abstract = {We measure the asymmetry in the charge-weighted rapidity
             qyℓ of the lepton in semileptonic tt̄ decays recorded
             with the CDF II detector using the full Tevatron Run II
             sample, corresponding to an integrated luminosity of 9.4
             fb-1. A parametrization of the asymmetry as a function of
             qyℓ is used to correct for the finite acceptance of the
             detector and recover the production-level asymmetry. The
             result of AFBℓ=0.094-0.029+0.032 is to be compared to the
             standard model next-to-leading-order prediction of
             AFBℓ=0.038±0.003. © 2013 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.88.072003},
   Key = {fds308961}
}

@article{fds308959,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Erratum: Indirect measurement of sin-W
             (MW) using e+e - pairs in
             the Z-boson region with pp̄ collisions at a
             center-of-momentum energy of 1.96 TeV (Physical Review D
             (2013) 88 (072002))},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.079905},
   Doi = {10.1103/PhysRevD.88.079905},
   Key = {fds308959}
}

@article{fds308956,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Measurement of the distributions of event-by-event flow
             harmonics in lead-lead collisions at √SNN =
             2.76 TeV with the ATLAS detector at the LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2013},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2013)183},
   Abstract = {The distributions of event-by-event harmonic flow
             coefficients υn for n = 2-4 are measured in √sNN =
             2.76TeV Pb+Pb collisions using the ATLAS detector at the
             LHC. The measurements are performed using charged particles
             with transverse momentum pT > 0.5GeV and in the
             pseudorapidity range |η| < 2.5 in a dataset of
             approximately 7 μb-1 recorded in 2010. The shapes of the
             υn distributions suggest that the associated flow vectors
             are described by a two-dimensional Gaussian function in
             central collisions for υ2 and over most of the measured
             centrality range for υ3 and υ4. Significant deviations
             from this function are observed for υ2 in mid-central and
             peripheral collisions, and a small deviation is observed for
             υ3 in mid-central collisions. In order to be sensitive to
             these deviations, it is shown that the commonly used
             multi-particle cumulants, involving four particles or more,
             need to be measured with a precision better than a few
             percent. The υn distributions are also measured
             independently for charged particles with 0.5 < pT < 1 GeV
             and pT > 1 GeV. When these distributions are rescaled to the
             same mean values, the adjusted shapes are found to be nearly
             the same for these two pT ranges. The υn distributions are
             compared with the eccentricity distributions from two models
             for the initial collision geometry: a Glauber model and a
             model that includes corrections to the initial geometry due
             to gluon saturation effects. Both models fail to describe
             the experimental data consistently over most of the measured
             centrality range. Copyright CERN.},
   Doi = {10.1007/JHEP11(2013)183},
   Key = {fds308956}
}

@article{fds308958,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Direct measurement of the total decay width of the top
             quark.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {20},
   Pages = {202001},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.111.202001},
   Abstract = {We present a measurement of the total decay width of the top
             quark using events with top-antitop quark pair candidates
             reconstructed in the final state with one charged lepton and
             four or more hadronic jets. We use the full Tevatron run II
             data set of sqrt[s]=1.96  TeV proton-antiproton
             collisions recorded by the CDF II detector. The top quark
             mass and the mass of the hadronically decaying W boson are
             reconstructed for each event and compared with distributions
             derived from simulated signal and background samples to
             extract the top quark width (Γtop) and the energy scale of
             the calorimeter jets with in situ calibration. For a top
             quark mass Mtop=172.5  GeV/c2, we find
             1.10<Γtop<4.05  GeV at 68% confidence level, which is
             in agreement with the standard model expectation of 1.3 GeV
             and is the most precise direct measurement of the top quark
             width to date.},
   Doi = {10.1103/physrevlett.111.202001},
   Key = {fds308958}
}

@article{fds308986,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Measurement of the differential cross section
             dσ/d(cosθ(t)) for Top-Quark Pair Production in pp
             Collisions at sqrt[s] = 1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {18},
   Pages = {182002},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.111.182002},
   Abstract = {We report a measurement of the differential cross section
             dσ/d(cosθ(t)) for top-quark pair production as a function
             of the top-quark production angle in proton-antiproton
             collisions at sqrt[s] = 1.96 TeV. This measurement is
             performed using data collected with the CDF II detector at
             the Tevatron, corresponding to an integrated luminosity of
             9.4 fb(-1). We employ the Legendre polynomials to
             characterize the shape of the differential cross section at
             the parton level. The observed Legendre coefficients are in
             good agreement with the prediction of the
             next-to-leading-order standard-model calculation, with the
             exception of an excess linear-term coefficient a(1) = 0.40
             ± 0.12, compared to the standard-model prediction of
             a(1)=0.15(-0.03)(+0.07).},
   Doi = {10.1103/physrevlett.111.182002},
   Key = {fds308986}
}

@article{fds308955,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
             MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
             Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
             F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
   Title = {Measurement of the top-quark pair-production cross section
             in events with two leptons and bottom-quark jets using the
             full CDF data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.091103},
   Abstract = {We present a measurement of the top-quark pair production
             cross section in proton-antiproton collisions at √s=1.96
             TeV. The data were collected at the Fermilab Tevatron by the
             CDF II detector and correspond to an integrated luminosity
             of 8.8 fb-1, representing the complete CDF Run II data set.
             We select events consistent with the production of top-quark
             pairs by requiring the presence of two reconstructed
             leptons, an imbalance in the total event transverse
             momentum, and jets. At least one jet is required to be
             identified as consistent with the fragmentation of a bottom
             quark using a secondary-vertex-finding algorithm. The 246
             candidate events are estimated to have a signal purity of
             91%. We measure a cross section of σ tt̄=7.09±0.84 pb,
             assuming a top-quark mass of 172.5 GeV/c2. The results are
             consistent with the standard model as predicted by
             next-to-leading-order calculations. Published by the
             American Physical Society.},
   Doi = {10.1103/PhysRevD.88.091103},
   Key = {fds308955}
}

@article{fds308954,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Search for the production of ZW and ZZ boson pairs decaying
             into charged leptons and jets in pp̄ collisions at
             √s=1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Pages = {092002},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.092002},
   Abstract = {We present a measurement of the production cross section for
             ZW and ZZ boson pairs in final states with a pair of charged
             leptons, from the decay of a Z boson, and at least two jets,
             from the decay of a W or Z boson, using the full sample of
             proton-antiproton collisions recorded with the CDF II
             detector at the Tevatron, corresponding to 8.9 fb-1 of
             integrated luminosity. We increase the sensitivity to
             vector-boson decays into pairs of quarks using a
             neural-network discriminant that exploits the differences
             between the spatial spread of energy depositions and
             charged-particle momenta contained within the jet of
             particles originating from quarks and gluons. Additionally,
             we employ new jet energy corrections to Monte Carlo
             simulations that account for differences in the observed
             energy scales for quark and gluon jets. The number of signal
             events is extracted through a simultaneous fit to the dijet
             mass spectrum in three classes of events: events likely to
             contain jets with a heavy-quark decay, events likely to
             contain jets originating from light quarks, and events that
             fail these identification criteria. We determine the
             production cross section to be σZW+ZZ=2.5-1.0+2.0 pb (<6.1
             pb at the 95% confidence level), consistent with the
             standard model prediction of 5.1 pb. © 2013 American
             Physical Society.},
   Doi = {10.1103/PhysRevD.88.092002},
   Key = {fds308954}
}

@article{fds308953,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Search for a dijet resonance in events with jets and missing
             transverse energy in pp̄ collisions at √s=1.96
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.092004},
   Abstract = {We report on a search for a dijet resonance in events with
             only two or three jets and a large imbalance in the total
             event transverse momentum. This search is sensitive to the
             possible production of a new particle in association with a
             W or Z boson, where the boson decays leptonically with one
             or more neutrinos in the final state. We use the full data
             set collected by the CDF II detector at the Tevatron
             collider at a proton-antiproton center-of-mass energy of
             1.96 TeV. These data correspond to an integrated luminosity
             of 9.1 fb -1. We study the invariant mass distribution of
             the two jets with highest transverse energy. We find good
             agreement between data and standard model background
             expectations and measure the combined cross section for WW,
             WZ, and ZZ production to be 13.8-2.7+3.0 pb. No significant
             anomalies are observed in the mass spectrum, and 95%
             credibility level upper limits are set on the production
             rates of a potential new particle in association with a W or
             Z boson. © 2013 American Physical Society.},
   Doi = {10.1103/PhysRevD.88.092004},
   Key = {fds308953}
}

@article{fds310542,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Production of KS0, K*(892) and φ0(1020) in minimum bias
             events and KS0 and Λ0 in jets in pp̄ collisions at
             √s=1.96 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {88},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2013},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.092005},
   Abstract = {We report measurements of the inclusive transverse momentum
             (pT) distribution of centrally produced KS0, K±(892), and
             φ0(1020) mesons up to pT=10 GeV/c in minimum bias events,
             and KS0 and Λ0 particles up to pT=20 GeV/c in jets with
             transverse energy between 25 and 160 GeV in pp̄ collisions.
             The data were taken with the CDF II detector at the Fermilab
             Tevatron at √s=1.96 TeV. We find that as pT increases, the
             pT slopes of the three mesons (KS0, K±, and φ) are
             similar. And using our previous Λ0 results from minimum
             bias events, we show that the ratio of Λ0 to KS0 as a
             function of pT in minimum bias events becomes similar to the
             fairly constant ratio in jets at pT∼5 GeV/c. This suggests
             that the particles with pTâ‰35 GeV/c in minimum bias
             events are from "soft" jets, and that the pT slope of
             particles in jets is insensitive to light quark flavor (u,
             d, or s) and to the number of valence quarks. We also find
             that for pT≠24 GeV relatively more Λ0 baryons are
             produced in minimum bias events than in jets. © 2013
             American Physical Society.},
   Doi = {10.1103/PhysRevD.88.092005},
   Key = {fds310542}
}

@article{fds308949,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
             A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith,
             L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay,
             NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
             AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
             BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
             FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
   Title = {Measurement of top quark polarization in top-antitop events
             from proton-proton collisions at √s=7  TeV using the
             ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {23},
   Pages = {232002},
   Year = {2013},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.111.232002},
   Abstract = {This Letter presents measurements of the polarization of the
             top quark in top-antitop quark pair events, using
             4.7  fb(-1) of proton-proton collision data recorded
             with the ATLAS detector at the Large Hadron Collider at
             √s=7  TeV. Final states containing one or two isolated
             leptons (electrons or muons) and jets are considered. Two
             measurements of α(ℓ)P, the product of the leptonic
             spin-analyzing power and the top quark polarization, are
             performed assuming that the polarization is introduced by
             either a CP conserving or a maximally CP violating
             production process. The measurements obtained,
             α(ℓ)P(CPC)=-0.035±0.014(stat)±0.037(syst) and
             α(ℓ)P(CPV)=0.020±0.016(stat)(-0.017)(+0.013)(syst), are
             in good agreement with the standard model prediction of
             negligible top quark polarization.},
   Doi = {10.1103/physrevlett.111.232002},
   Key = {fds308949}
}

@article{fds308951,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kulkarni, N and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
             L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
             A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
             A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
             E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
             Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
   Title = {Observation of D⁰-D¯⁰ mixing using the CDF II
             detector.},
   Journal = {Physical review letters},
   Volume = {111},
   Number = {23},
   Pages = {231802},
   Year = {2013},
   Month = {December},
   url = {http://dx.doi.org/10.1103/physrevlett.111.231802},
   Abstract = {We measure the time dependence of the ratio of decay rates
             for D0→K(+)π(-) to the Cabibbo-favored decay
             D(0)→K(-)π(+). The charge conjugate decays are included.
             A signal of 3.3×10(4) D(*+)→π(+)D(0), D(0)→K(+)π(-)
             decays is obtained with D0 proper decay times between 0.75
             and 10 mean D0 lifetimes. The data were recorded with the
             CDF II detector at the Fermilab Tevatron and correspond to
             an integrated luminosity of 9.6  fb(-1) for pp¯
             collisions at √s=1.96  TeV. Assuming CP conservation,
             we search for D0-D¯0 mixing and measure the mixing
             parameters to be R(D)=(3.51±0.35)×10(-3),
             y'=(4.3±4.3)×10(-3), and x'2=(0.08±0.18)×10(-3). We
             report Bayesian probability intervals in the x'2-y' plane
             and find that the significance of excluding the no-mixing
             hypothesis is equivalent to 6.1 Gaussian standard
             deviations, providing the second observation of D0-D¯0
             mixing from a single experiment.},
   Doi = {10.1103/physrevlett.111.231802},
   Key = {fds308951}
}

@article{fds325316,
   Author = {The ATLAS collaboration and A and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for supersymmetry in events with large missing
             transverse momentum, jets, and at least one tau lepton in 20
             fb−1 of √s= 8 TeV proton-proton collision data with the
             ATLAS detector},
   Journal = {Social Psychiatry and Psychiatric Epidemiology},
   Volume = {2014},
   Number = {9},
   Publisher = {Dr. Dietrich Steinkopff Verlag GmbH and Co.
             KG},
   Year = {2014},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)103},
   Abstract = {A search for supersymmetry (SUSY) in events with large
             missing transverse momentum, jets, at least one hadronically
             decaying tau lepton and zero or one additional light leptons
             (electron/muon), has been performed using 20.3fb−1of
             proton-proton collision data at √ s= 8 TeV recorded with
             the ATLAS detector at the Large Hadron Collider. No excess
             above the Standard Model background expectation is observed
             in the various signal regions and 95% confidence level upper
             limits on the visible cross section for new phenomena are
             set. The results of the analysis are interpreted in several
             SUSY scenarios, significantly extending previous limits
             obtained in the same final states. In the framework of
             minimal gauge-mediated SUSY breaking models, values of the
             SUSY breaking scale Λ below 63 TeV are excluded,
             independently of tan β. Exclusion limits are also derived
             for an mSUGRA/CMSSM model, in both the R-parity-conserving
             and R-parity-violating case. A further interpretation is
             presented in a framework of natural gauge mediation, in
             which the gluino is assumed to be the only light coloured
             sparticle and gluino masses below 1090 GeV are
             excluded.},
   Doi = {10.1007/JHEP09(2014)103},
   Key = {fds325316}
}

@article{fds225675,
   Author = {ATLAS collaboration},
   Title = {Search for dark matter in events with a Z boson and missing
             transverse momentum in pp collisions at √s = 8 TeV with
             the ATLAS detector},
   Journal = {PRD 90, 012004},
   Year = {2014},
   Key = {fds225675}
}

@article{fds313372,
   Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek,
             S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J},
   Title = {Search for strong production of supersymmetric particles in
             final states with missing transverse momentum and at least
             three b-jets at (formula presented) TeV proton-proton
             collisions with the ATLAS detector},
   Journal = {Critical Ultrasound Journal},
   Volume = {2014},
   Number = {10},
   Year = {2014},
   Month = {January},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP10(2014)024},
   Abstract = {© 2014, The Author(s). Abstract: This paper reports the
             results of a search for strong production of supersymmetric
             particles in 20.1 fb−1 of proton-proton collisions at a
             centre-of-mass energy of 8 TeV using the ATLAS detector at
             the LHC. The search is performed separately in events with
             either zero or at least one high-pT lepton (electron or
             muon), large missing transverse momentum, high jet
             multiplicity and at least three jets identified as
             originated from the fragmentation of a b-quark. No excess is
             observed with respect to the Standard Model predictions. The
             results are interpreted in the context of several
             supersymmetric models involving gluinos and scalar top and
             bottom quarks, as well as a mSUGRA/CMSSM model. Gluino
             masses up to 1340 GeV are excluded, depending on the model,
             significantly extending the previous ATLAS
             limits.},
   Doi = {10.1007/JHEP10(2014)024},
   Key = {fds313372}
}

@article{fds308937,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
             VV and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {Measurement of the electroweak production of dijets in
             association with a Z-boson and distributions sensitive to
             vector boson fusion in proton-proton collisions at √s= 8
             TeV using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP04(2014)031},
   Doi = {10.1007/JHEP04(2014)031},
   Key = {fds308937}
}

@article{fds308938,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for direct production of charginos and neutralinos in
             events with three leptons and missing transverse momentum in
             pv s = 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {4},
   Pages = {1-52},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP04(2014)169},
   Abstract = {A search for the direct production of charginos and
             neutralinos in final states with three leptons and missing
             transverse momentum is presented. The analysis is based on
             20.3 fb-1 of vs = 8TeV proton-proton collision data
             delivered by the Large Hadron Collider and recorded with the
             ATLAS detector. Observations are consistent with the
             Standard Model expectations and limits are set in
             R-parity-conserving phenomenological Minimal Supersymmetric
             Standard Models and in simplified supersymmetric models,
             significantly extending previous results. For simplified
             supersymmetric models of direct chargino (∼X±1) and
             next-to-lightest neutralino (X∼02) production with decays
             to lightest neutralino (∼X01) via either all three
             generations of sleptons, staus only, gauge bosons, or Higgs
             bosons, ∼X± 1 and ∼X02 masses are excluded up to
             700GeV, 380GeV, 345GeV, or 148GeV respectively, for a
             massless ∼X01.},
   Doi = {10.1007/JHEP04(2014)169},
   Key = {fds308938}
}

@article{fds308943,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
             S},
   Title = {Measurement of the top quark pair production charge
             asymmetry in proton-proton collisions at √s = 7 TeV using
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {2},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP02(2014)107},
   Abstract = {This paper presents a measurement of the top quark pair
             (tt̄) production charge asymmetry AC using 4.7 fb-1 of
             proton-proton collisions at a centre-of-mass energy √s =
             7TeV collected by the ATLAS detector at the LHC. A
             tt̄-enriched sample of events with a single lepton
             (electron or muon), missing transverse momentum and at least
             four high transverse momentum jets, of which at least one is
             tagged as coming from a b-quark, is selected. A likelihood
             fit is used to reconstruct the tt̄ event kinematics. A
             Bayesian unfolding procedure is employed to estimate AC at
             the parton-level. The measured value of the tt̄ production
             charge asymmetry is AC = 0.006 ± 0.010, where the
             uncertainty includes both the statistical and the systematic
             components. Differential AC measurements as a function of
             the invariant mass, the rapidity and the transverse momentum
             of the tt̄- system are also presented. In addition, AC is
             measured for a subset of events with large tt̄ velocity,
             where physics beyond the Standard Model could contribute.
             All measurements are consistent with the Standard Model
             predictions.},
   Doi = {10.1007/JHEP02(2014)107},
   Key = {fds308943}
}

@article{fds308944,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
             K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
             IA and Budick, B and Buehrer, F and Bugge, L and Bulekov, O and Bundock,
             AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Chapman, JW and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov,
             A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
             BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
             J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
             ZH},
   Title = {Search for dark matter in events with a hadronically
             decaying W or Z boson and missing transverse momentum in pp
             collisions at √s=8  TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {4},
   Pages = {041802},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1103/physrevlett.112.041802},
   Abstract = {A search is presented for dark matter pair production in
             association with a W or Z boson in pp collisions
             representing 20.3  fb(-1) of integrated luminosity at
             √s=8  TeV using data recorded with the ATLAS detector
             at the Large Hadron Collider. Events with a hadronic jet
             with the jet mass consistent with a W or Z boson, and with
             large missing transverse momentum are analyzed. The data are
             consistent with the standard model expectations. Limits are
             set on the mass scale in effective field theories that
             describe the interaction of dark matter and standard model
             particles, and on the cross section of Higgs production and
             decay to invisible particles. In addition, cross section
             limits on the anomalous production of W or Z bosons with
             large missing transverse momentum are set in two fiducial
             regions.},
   Doi = {10.1103/physrevlett.112.041802},
   Key = {fds308944}
}

@article{fds308945,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Search for new phenomena in photon + jet events collected in
             proton-proton collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {728},
   Number = {1},
   Pages = {562-578},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.12.029},
   Abstract = {This Letter describes a model-independent search for the
             production of new resonances in photon + jet (γ + jet)
             events using 20 fb-1 of proton-proton LHC data recorded with
             the ATLAS detector at a centre-of-mass energy of √s = 8
             TeV. The γ + jet mass distribution is compared to a
             background model fit from data; no significant deviation
             from the background-only hypothesis is found. Limits are set
             at 95% credibility level on generic Gaussian-shaped signals
             and two benchmark phenomena beyond the Standard Model:
             non-thermal quantum black holes and excited quarks.
             Non-thermal quantum black holes are excluded below masses of
             4.6 TeV and excited quarks are excluded below masses of 3.5
             TeV. © 2013 The Authors. Published by Elsevier
             B.V.},
   Doi = {10.1016/j.physletb.2013.12.029},
   Key = {fds308945}
}

@article{fds308947,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Erratum: Search for new phenomena in final states with large
             jet multiplicities and missing transverse momentum at √s =
             8 TeV proton-proton collisions using the ATLAS experiment
             (Journal of High Energy Physics (2013) 10
             (130))},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2014)109},
   Doi = {10.1007/JHEP01(2014)109},
   Key = {fds308947}
}

@article{fds316866,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
             E},
   Title = {Standalone vertex finding in the ATLAS muon
             spectrometer},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {2},
   Pages = {P02001-P02001},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/9/02/P02001},
   Abstract = {A dedicated reconstruction algorithm to find decay vertices
             in the ATLAS muon spectrometer is presented. The algorithm
             searches the region just upstream of or inside the muon
             spectrometer volume for multi-particle vertices that
             originate from the decay of particles with long decay paths.
             The performance of the algorithm is evaluated using both a
             sample of simulated Higgs boson events, in which the Higgs
             boson decays to long-lived neutral particles that in turn
             decay to bb final states, and pp collision data at √s = 7
             TeV collected with the ATLAS detector at the LHC during
             2011.},
   Doi = {10.1088/1748-0221/9/02/P02001},
   Key = {fds316866}
}

@article{fds316867,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Operation and performance of the ATLAS semiconductor
             tracker},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {8},
   Pages = {P08009-P08009},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/9/08/P08009},
   Abstract = {The semiconductor tracker is a silicon microstrip detector
             forming part of the inner tracking system of the ATLAS
             experiment at the LHC. The operation and performance of the
             semiconductor tracker during the first years of LHC running
             are described. More than 99% of the detector modules were
             operational during this period, with an average intrinsic
             hit efficiency of (99.74±0.04)%. The evolution of the noise
             occupancy is discussed, and measurements of the Lorentz
             angle, d-ray production and energy loss presented. The
             alignment of the detector is found to be stable at the
             few-micron level over long periods of time. Radiation damage
             measurements, which include the evolution of detector
             leakage currents, are found to be consistent with
             predictions and are used in the verification of radiation
             background simulations.},
   Doi = {10.1088/1748-0221/9/08/P08009},
   Key = {fds316867}
}

@article{fds313373,
   Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J},
   Title = {Search for the direct production of charginos, neutralinos
             and staus in final states with at least two hadronically
             decaying taus and missing transverse momentum in pp
             collisions at √ $$ \sqrt{s}=8 $$ TeV with the ATLAS
             detector},
   Journal = {Critical Ultrasound Journal},
   Volume = {2014},
   Number = {10},
   Year = {2014},
   Month = {January},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP10(2014)096},
   Abstract = {© 2014, The Author(s).Abstract: Results of a search for the
             electroweak associated production of charginos and
             next-to-lightest neutralinos, pairs of charginos or pairs of
             tau sleptons are presented. These processes are
             characterised by final states with at least two hadronically
             decaying tau leptons, missing transverse momentum and low
             jet activity. The analysis is based on an integrated
             luminosity of 20.3 fb−1 of proton-proton collisions at
             (Formula presented) recorded with the ATLAS experiment at
             the Large Hadron Collider. No significant excess is observed
             with respect to the predictions from Standard Model
             processes. Limits are set at 95% confidence level on the
             masses of the lighter chargino and next-to-lightest
             neutralino for various hypotheses for the lightest
             neutralino mass in simplified models. In the scenario of
             direct production of chargino pairs, with each chargino
             decaying into the lightest neutralino via an intermediate
             tau slepton, chargino masses up to 345 GeV are excluded for
             a massless lightest neutralino. For associated production of
             mass-degenerate charginos and next-to-lightest neutralinos,
             both decaying into the lightest neutralino via an
             intermediate tau slepton, masses up to 410 GeV are excluded
             for a massless lightest neutralino.[Figure not available:
             see fulltext.]},
   Doi = {10.1007/JHEP10(2014)096},
   Key = {fds313373}
}

@article{fds310525,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
             JF},
   Title = {Measurement of dijet cross-sections in pp collisions at 7
             TeV centre-of-mass energy using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP05(2014)059},
   Abstract = {Double-differential dijet cross-sections measured in pp
             collisions at the LHC with a 7TeV centre-of-mass energy are
             presented as functions of dijet mass and half the rapidity
             separation of the two highest-pT jets. These measurements
             are obtained using data corresponding to an integrated
             luminosity of 4.5 fb−1, recorded by the ATLAS detector in
             2011. The data are corrected for detector effects so that
             cross-sections are presented at the particle level.
             Cross-sections are measured up to 5TeV dijet mass using jets
             reconstructed with the anti-kt algorithm for values of the
             jet radius parameter of 0.4 and 0.6. The cross-sections are
             compared with next-to-leading-order perturbative QCD
             calculations by NLOJet++ corrected to account for
             non-perturbative effects. Comparisons with POWHEG
             predictions, using a next-to-leading-order matrix element
             calculation interfaced to a partonshower Monte Carlo
             simulation, are also shown. Electroweak effects are
             accounted for in both cases. The quantitative comparison of
             data and theoretical predictions obtained using various
             parameterizations of the parton distribution functions is
             performed using a frequentist method. In general, good
             agreement with data is observed for the NLOJet++ theoretical
             predictions when using the CT10, NNPDF2.1 and MSTW 2008 PDF
             sets. Disagreement is observed when using the ABM11 and
             HERAPDF1.5 PDF sets for some ranges of dijet mass and half
             the rapidity separation. An example setting a lower limit on
             the compositeness scale for a model of contact interactions
             is presented, showing that the unfolded results can be used
             to constrain contributions to dijet production beyond that
             predicted by the Standard Model.},
   Doi = {10.1007/JHEP05(2014)059},
   Key = {fds310525}
}

@article{fds310491,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for long-lived neutral particles decaying into lepton
             jets in proton-proton collisions at √s= 8TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)088},
   Abstract = {Abstract: Several models of physics beyond the Standard
             Model predict neutral particles that decay into final states
             consisting of collimated jets of light leptons and hadrons
             (so-called “lepton jets”). These particles can also be
             long-lived with decay length comparable to, or even larger
             than, the LHC detectors’ linear dimensions. This paper
             presents the results of a search for lepton jets in
             proton-proton collisions at the centre-of-mass energy of
             √s= 8TeV in a sample of 20.3 fb−1 collected during 2012
             with the ATLAS detector at the LHC. Limits on models
             predicting Higgs boson decays to neutral long-lived lepton
             jets are derived as a function of the particle’s proper
             decay length.},
   Doi = {10.1007/JHEP11(2014)088},
   Key = {fds310491}
}

@article{fds310528,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Fiducial and differential cross sections of Higgs boson
             production measured in the four-lepton decay channel in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Pages = {234-253},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.09.054},
   Abstract = {Measurements of fiducial and differential cross sections of
             Higgs boson production in the H→ZZ*→4ℓ decay channel
             are presented. The cross sections are determined within a
             fiducial phase space and corrected for detection efficiency
             and resolution effects. They are based on 20.3fb-1 of pp
             collision data, produced at √s=8 TeV centre-of-mass energy
             at the LHC and recorded by the ATLAS detector. The
             differential measurements are performed in bins of
             transverse momentum and rapidity of the four-lepton system,
             the invariant mass of the subleading lepton pair and the
             decay angle of the leading lepton pair with respect to the
             beam line in the four-lepton rest frame, as well as the
             number of jets and the transverse momentum of the leading
             jet. The measured cross sections are compared to selected
             theoretical calculations of the Standard Model expectations.
             No significant deviation from any of the tested predictions
             is found.},
   Doi = {10.1016/j.physletb.2014.09.054},
   Key = {fds310528}
}

@article{fds313371,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of flow harmonics with multi-particle cumulants
             in Pb+Pb collisions at [Formula: see text] TeV with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {11},
   Pages = {3157},
   Year = {2014},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3157-z},
   Abstract = {ATLAS measurements of the azimuthal anisotropy in lead-lead
             collisions at [Formula: see text] TeV are shown using a
             dataset of approximately 7 [Formula: see text]b[Formula:
             see text] collected at the LHC in 2010. The measurements are
             performed for charged particles with transverse momenta
             [Formula: see text] GeV and in the pseudorapidity range
             [Formula: see text]. The anisotropy is characterized by the
             Fourier coefficients, [Formula: see text], of the
             charged-particle azimuthal angle distribution for [Formula:
             see text]-4. The Fourier coefficients are evaluated using
             multi-particle cumulants calculated with the generating
             function method. Results on the transverse momentum,
             pseudorapidity and centrality dependence of the [Formula:
             see text] coefficients are presented. The elliptic flow,
             [Formula: see text], is obtained from the two-, four-, six-
             and eight-particle cumulants while higher-order
             coefficients, [Formula: see text] and [Formula: see text],
             are determined with two- and four-particle cumulants. Flow
             harmonics [Formula: see text] measured with four-particle
             cumulants are significantly reduced compared to the
             measurement involving two-particle cumulants. A comparison
             to [Formula: see text] measurements obtained using different
             analysis methods and previously reported by the LHC
             experiments is also shown. Results of measurements of flow
             fluctuations evaluated with multi-particle cumulants are
             shown as a function of transverse momentum and the collision
             centrality. Models of the initial spatial geometry and its
             fluctuations fail to describe the flow fluctuations
             measurements.},
   Doi = {10.1140/epjc/s10052-014-3157-z},
   Key = {fds313371}
}

@article{fds310513,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for microscopic black holes and string balls in final
             states with leptons and jets with the ATLAS detector at √s
             = 8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP08(2014)103},
   Abstract = {A search for an excess of events with multiple high
             transverse momentum objects including charged leptons and
             jets is presented, using 20.3 fb -1 of proton-proton
             collision data recorded by the ATLAS detector at the Large
             Hadron Collider in 2012 at a centre-of-mass energy of √s =
             8 TeV. No excess of events beyond Standard Model
             expectations is observed. Using extra-dimensional models for
             black hole and string ball production and decay, exclusion
             contours are determined as a function of the mass threshold
             for production and the fundamental gravity scale for two,
             four and six extra dimensions. For six extra dimensions,
             mass thresholds of 4.8-6.2 TeV are excluded at 95 %
             confidence level, depending on the fundamental gravity scale
             and model assumptions. Upper limits on the fiducial
             cross-sections for non-Standard Model production of these
             final states are set. [Figure not available: see fulltext.]
             © 2014 The Author(s).},
   Doi = {10.1007/JHEP08(2014)103},
   Key = {fds310513}
}

@article{fds310520,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for direct top-squark pair production in final states
             with two leptons in pp collisions at √s = 8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)124},
   Abstract = {A search is presented for direct top-squark pair production
             in final states with two leptons (electrons or muons) of
             opposite charge using 20.3 fb -1 of pp collision data at
             √s = 8 TeV, collected by the ATLAS experiment at the Large
             Hadron Collider in 2012. No excess over the Standard Model
             expectation is found. The results are interpreted under the
             separate assumptions (i) that the top squark decays to a
             b-quark in addition to an on-shell chargino whose decay
             occurs via a real or virtual W boson, or (ii) that the top
             squark decays to a t-quark and the lightest neutralino. A
             top squark with a mass between 150 GeV and 445 GeV decaying
             to a b-quark and an on-shell chargino is excluded at 95%
             confidence level for a top squark mass equal to the chargino
             mass plus 10 GeV, in the case of a 1 GeV lightest
             neutralino. Top squarks with masses between 215 (90) GeV and
             530 (170) GeV decaying to an on-shell (off-shell) t-quark
             and a neutralino are excluded at 95% confidence level for a
             1 GeV neutralino. [Figure not available: see fulltext.] ©
             2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)124},
   Key = {fds310520}
}

@article{fds310521,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the low-mass Drell-Yan differential cross
             section at √s = 7 TeV using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)112},
   Abstract = {The differential cross section for the process Z/γ * →
             ℓℓ (ℓ = e, μ) as a function of dilepton invariant
             mass is measured in pp collisions at √s = 7 TeV at the LHC
             using the ATLAS detector. The measurement is performed in
             the e and μ channels for invariant masses between 26 GeV
             and 66 GeV using an integrated luminosity of 1.6 fb -1
             collected in 2011 and these measurements are combined. The
             analysis is extended to invariant masses as low as 12 GeV in
             the muon channel using 35 pb-1 of data collected in 2010.
             The cross sections are determined within fiducial acceptance
             regions and corrections to extrapolate the measurements to
             the full kinematic range are provided. Next-to-next-to-leading-
             order QCD predictions provide a significantly better
             description of the results than next-to-leading-order QCD
             calculations, unless the latter are matched to a parton
             shower calculation. [Figure not available: see fulltext.] ©
             2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)112},
   Key = {fds310521}
}

@article{fds310523,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
             C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for supersymmetry at √s= 8 TeV in final states with
             jets and two same-sign leptons or three leptons with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)035},
   Abstract = {A search for strongly produced supersymmetric particles is
             conducted using signatures involving multiple energetic jets
             and either two isolated leptons (e or μ) with the same
             electric charge, or at least three isolated leptons. The
             search also utilises jets originating from b-quarks, missing
             transverse momentum and other observables to extend its
             sensitivity. The analysis uses a data sample corresponding
             to a total integrated luminosity of 20.3 fb-1 of √s = 8
             TeV proton-proton collisions recorded with the ATLAS
             detector at the Large Hadron Collider in 2012. No deviation
             from the Standard Model expectation is observed. New or
             significantly improved exclusion limits are set on a wide
             variety of supersymmetric models in which the lightest
             squark can be of the first, second or third generations, and
             in which R-parity can be conserved or violated. [Figure not
             available: see fulltext.] © 2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)035},
   Key = {fds310523}
}

@article{fds310529,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
             G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
             M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
             OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
             T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
             M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella,
             G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
             N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
             AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
             Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
             V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
             RN},
   Title = {Muon reconstruction efficiency and momentum resolution of
             the ATLAS experiment in proton-proton collisions at
             [Formula: see text] TeV in 2010.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {9},
   Pages = {3034},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3034-9},
   Abstract = {This paper presents a study of the performance of the muon
             reconstruction in the analysis of proton-proton collisions
             at [Formula: see text] TeV at the LHC, recorded by the
             ATLAS detector in 2010. This performance is described in
             terms of reconstruction and isolation efficiencies and
             momentum resolutions for different classes of reconstructed
             muons. The results are obtained from an analysis of
             [Formula: see text] meson and [Formula: see text] boson
             decays to dimuons, reconstructed from a data sample
             corresponding to an integrated luminosity of 40 pb[Formula:
             see text]. The measured performance is compared to Monte
             Carlo predictions and deviations from the predicted
             performance are discussed.},
   Doi = {10.1140/epjc/s10052-014-3034-9},
   Key = {fds310529}
}

@article{fds310530,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
             D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
             GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
             T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
             J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
             S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
             R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
             Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
             L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
             A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {The differential production cross section of the [Formula:
             see text](1020) meson in [Formula: see text] = 7 TeV
             [Formula: see text] collisions measured with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {7},
   Pages = {2895},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2895-2},
   Abstract = {A measurement is presented of the [Formula: see text]
             production cross section at [Formula: see text] = 7 TeV
             using [Formula: see text] collision data corresponding to an
             integrated luminosity of 383 [Formula: see text], collected
             with the ATLAS experiment at the LHC. Selection of [Formula:
             see text](1020) mesons is based on the identification of
             charged kaons by their energy loss in the pixel detector.
             The differential cross section is measured as a function of
             the transverse momentum, [Formula: see text], and rapidity,
             [Formula: see text], of the [Formula: see text](1020) meson
             in the fiducial region 500 [Formula: see text] 1200 MeV,
             [Formula: see text] 0.8, kaon [Formula: see text] 230 MeV
             and kaon momentum [Formula: see text] 800 MeV. The
             integrated [Formula: see text]-meson production cross
             section in this fiducial range is measured to be [Formula:
             see text] = 570 [Formula: see text] 8 (stat) [Formula: see
             text] 66 (syst) [Formula: see text] 20 (lumi) [Formula: see
             text].},
   Doi = {10.1140/epjc/s10052-014-2895-2},
   Key = {fds310530}
}

@article{fds310531,
   Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
             SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
             A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
             M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
             N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji,
             W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and De Mendizabal,
             JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
             J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet,
             NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
             G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Renstrom, PABD and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
             LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill,
             R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland,
             W},
   Title = {Electron reconstruction and identification efficiency
             measurements with the ATLAS detector using the 2011 LHC
             proton-proton collision data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {7},
   Pages = {2941},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2941-0},
   Abstract = {Many of the interesting physics processes to be measured at
             the LHC have a signature involving one or more isolated
             electrons. The electron reconstruction and identification
             efficiencies of the ATLAS detector at the LHC have been
             evaluated using proton-proton collision data collected in
             2011 at [Formula: see text] TeV and corresponding to an
             integrated luminosity of 4.7 fb[Formula: see text].
             Tag-and-probe methods using events with leptonic decays of
             [Formula: see text] and [Formula: see text] bosons and
             [Formula: see text] mesons are employed to benchmark these
             performance parameters. The combination of all measurements
             results in identification efficiencies determined with an
             accuracy at the few per mil level for electron transverse
             energy greater than 30 GeV.},
   Doi = {10.1140/epjc/s10052-014-2941-0},
   Key = {fds310531}
}

@article{fds310532,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau,
             M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
             F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura,
             AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Light-quark and gluon jet discrimination in [Formula: see
             text] collisions at [Formula: see text] with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {8},
   Pages = {3023},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3023-z},
   Abstract = {A likelihood-based discriminant for the identification of
             quark- and gluon-initiated jets is built and validated using
             4.7 fb[Formula: see text] of proton-proton collision data
             at [Formula: see text] [Formula: see text] collected with
             the ATLAS detector at the LHC. Data samples with enriched
             quark or gluon content are used in the construction and
             validation of templates of jet properties that are the input
             to the likelihood-based discriminant. The discriminating
             power of the jet tagger is established in both data and
             Monte Carlo samples within a systematic uncertainty of
             [Formula: see text] 10-20 %. In data, light-quark jets can
             be tagged with an efficiency of [Formula: see text] while
             achieving a gluon-jet mis-tag rate of [Formula: see text] in
             a [Formula: see text] range between [Formula: see text] and
             [Formula: see text] for jets in the acceptance of the
             tracker. The rejection of gluon-jets found in the data is
             significantly below what is attainable using a Pythia 6
             Monte Carlo simulation, where gluon-jet mis-tag rates of
             10 % can be reached for a 50 % selection efficiency of
             light-quark jets using the same jet properties.},
   Doi = {10.1140/epjc/s10052-014-3023-z},
   Key = {fds310532}
}

@article{fds310533,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of distributions sensitive to the underlying
             event in inclusive Z-boson production in [Formula: see text]
             collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {12},
   Pages = {3195},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3195-6},
   Abstract = {A measurement of charged-particle distributions sensitive to
             the properties of the underlying event is presented for an
             inclusive sample of events containing a [Formula: see
             text]-boson, decaying to an electron or muon pair. The
             measurement is based on data collected using the ATLAS
             detector at the LHC in proton-proton collisions at a
             centre-of-mass energy of [Formula: see text] TeV with an
             integrated luminosity of [Formula: see text] fb[Formula:
             see text]. Distributions of the charged particle
             multiplicity and of the charged particle transverse momentum
             are measured in regions of azimuthal angle defined with
             respect to the [Formula: see text]-boson direction. The
             measured distributions are compared to similar distributions
             measured in jet events, and to the predictions of various
             Monte Carlo generators implementing different underlying
             event models.},
   Doi = {10.1140/epjc/s10052-014-3195-6},
   Key = {fds310533}
}

@article{fds310534,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Measurements of jet vetoes and azimuthal decorrelations in
             dijet events produced in [Formula: see text] collisions at
             [Formula: see text] using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {11},
   Pages = {3117},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3117-7},
   Abstract = {Additional jet activity in dijet events is measured using
             [Formula: see text] collisions at ATLAS at a centre-of-mass
             energy of [Formula: see text], for jets reconstructed using
             the [Formula: see text] algorithm with radius parameter
             [Formula: see text]. This is done using variables such as
             the fraction of dijet events without an additional jet in
             the rapidity interval bounded by the dijet subsystem and
             correlations between the azimuthal angles of the dijet s.
             They are presented, both with and without a veto on
             additional jet activity in the rapidity interval, as a
             function of the scalar average of the transverse momenta of
             the dijet s and of the rapidity interval size. The double
             differential dijet cross section is also measured as a
             function of the interval size and the azimuthal angle
             between the dijet s. These variables probe differences in
             the approach to resummation of large logarithms when
             performing QCD calculations. The data are compared to
             powheg, interfaced to the pythia 8 and herwig parton shower
             generators, as well as to hej with and without interfacing
             it to the ariadne parton shower generator. None of the
             theoretical predictions agree with the data across the full
             phase-space considered; however, powheg+pythia 8 and
             hej+ariadne are found to provide the best agreement with the
             data. These measurements use the full data sample collected
             with the ATLAS detector in [Formula: see text][Formula: see
             text] collisions at the LHC and correspond to integrated
             luminosities of [Formula: see text] and [Formula: see text]
             for data collected during 2010 and 2011,
             respectively.},
   Doi = {10.1140/epjc/s10052-014-3117-7},
   Key = {fds310534}
}

@article{fds310535,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, M and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Measurement of the muon reconstruction performance of the
             ATLAS detector using 2011 and 2012 LHC proton-proton
             collision data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {11},
   Pages = {3130},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3130-x},
   Abstract = {This paper presents the performance of the ATLAS muon
             reconstruction during the LHC run with [Formula: see text]
             collisions at [Formula: see text]-8 TeV in 2011-2012,
             focusing mainly on data collected in 2012. Measurements of
             the reconstruction efficiency and of the momentum scale and
             resolution, based on large reference samples of [Formula:
             see text], [Formula: see text] and [Formula: see text]
             decays, are presented and compared to Monte Carlo
             simulations. Corrections to the simulation, to be used in
             physics analysis, are provided. Over most of the covered
             phase space (muon [Formula: see text] and [Formula: see
             text] GeV) the efficiency is above [Formula: see text] and
             is measured with per-mille precision. The momentum
             resolution ranges from [Formula: see text] at central
             rapidity and for transverse momentum [Formula: see
             text] GeV, to [Formula: see text] at large rapidity and
             [Formula: see text] GeV. The momentum scale is known with
             an uncertainty of [Formula: see text] to [Formula: see text]
             depending on rapidity. A method for the recovery of final
             state radiation from the muons is also presented.},
   Doi = {10.1140/epjc/s10052-014-3130-x},
   Key = {fds310535}
}

@article{fds310536,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {A measurement of the ratio of the production cross sections
             for [Formula: see text] and [Formula: see text] bosons in
             association with jets with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {12},
   Pages = {3168},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3168-9},
   Abstract = {The ratio of the production cross sections for [Formula: see
             text] and [Formula: see text] bosons in association with
             jets has been measured in proton-proton collisions at
             [Formula: see text] with the ATLAS experiment at the Large
             Hadron Collider. The measurement is based on the entire 2011
             dataset, corresponding to an integrated luminosity of
             [Formula: see text]. Inclusive and differential
             cross-section ratios for massive vector bosons decaying to
             electrons and muons are measured in association with jets
             with transverse momentum [Formula: see text] and jet
             rapidity [Formula: see text]. The measurements are compared
             to next-to-leading-order perturbative QCD calculations and
             to predictions from different Monte Carlo generators
             implementing leading-order matrix elements supplemented by
             parton showers.},
   Doi = {10.1140/epjc/s10052-014-3168-9},
   Key = {fds310536}
}

@article{fds310537,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for contact interactions and large extra dimensions
             in the dilepton channel using proton-proton collisions at
             [Formula: see text] 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {12},
   Pages = {3134},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3134-6},
   Abstract = {A search is conducted for non-resonant new phenomena in
             dielectron and dimuon final states, originating from either
             contact interactions or large extra spatial dimensions. The
             LHC 2012 proton-proton collision dataset recorded by the
             ATLAS detector is used, corresponding to 20 fb[Formula: see
             text] at [Formula: see text] = 8 TeV. The dilepton
             invariant mass spectrum is a discriminating variable in both
             searches, with the contact interaction search additionally
             utilizing the dilepton forward-backward asymmetry. No
             significant deviations from the Standard Model expectation
             are observed. Lower limits are set on the [Formula: see
             text] contact interaction scale [Formula: see text] between
             15.4 TeV and 26.3 TeV, at the 95 % credibility level. For
             large extra spatial dimensions, lower limits are set on the
             string scale [Formula: see text] between 3.2 TeV to
             5.0 TeV.},
   Doi = {10.1140/epjc/s10052-014-3134-6},
   Key = {fds310537}
}

@article{fds310538,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Measurement of the [Formula: see text] production
             cross-section using [Formula: see text] events with
             [Formula: see text]-tagged jets in [Formula: see text]
             collisions at [Formula: see text] and 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {10},
   Pages = {3109},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3109-7},
   Abstract = {The inclusive top quark pair ([Formula: see text])
             production cross-section [Formula: see text] has been
             measured in proton-proton collisions at [Formula: see text]
             and [Formula: see text] with the ATLAS experiment at the
             LHC, using [Formula: see text] events with an
             opposite-charge [Formula: see text] pair in the final state.
             The measurement was performed with the 2011 7 TeV dataset
             corresponding to an integrated luminosity of 4.6 [Formula:
             see text] and the 2012 8 TeV dataset of 20.3 [Formula: see
             text]. The numbers of events with exactly one and exactly
             two [Formula: see text]-tagged jets were counted and used to
             simultaneously determine [Formula: see text] and the
             efficiency to reconstruct and [Formula: see text]-tag a jet
             from a top quark decay, thereby minimising the associated
             systematic uncertainties. The cross-section was measured to
             be: [Formula: see text]where the four uncertainties arise
             from data statistics, experimental and theoretical
             systematic effects, knowledge of the integrated luminosity
             and of the LHC beam energy. The results are consistent with
             recent theoretical QCD calculations at next-to-next-to-leading
             order. Fiducial measurements corresponding to the
             experimental acceptance of the leptons are also reported,
             together with the ratio of cross-sections measured at the
             two centre-of-mass energies. The inclusive cross-section
             results were used to determine the top quark pole mass via
             the dependence of the theoretically predicted cross-section
             on [Formula: see text] giving a result of [Formula: see
             text][Formula: see text] GeV. By looking for an excess of
             [Formula: see text] production with respect to the QCD
             prediction, the results were also used to place limits on
             the pair-production of supersymmetric top squarks [Formula:
             see text] with masses close to the top quark mass, decaying
             via [Formula: see text] to predominantly right-handed top
             quarks and a light neutralino [Formula: see text], the
             lightest supersymmetric particle. Top squarks with masses
             between the top quark mass and 177 GeV are excluded at the
             95 % confidence level.},
   Doi = {10.1140/epjc/s10052-014-3109-7},
   Key = {fds310538}
}

@article{fds310539,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
             Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurement of the centrality and pseudorapidity dependence
             of the integrated elliptic flow in lead-lead collisions at
             [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {8},
   Pages = {2982},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2982-4},
   Abstract = {The integrated elliptic flow of charged particles produced
             in Pb+Pb collisions at [Formula: see text] TeV has been
             measured with the ATLAS detector using data collected at the
             Large Hadron Collider. The anisotropy parameter, [Formula:
             see text], was measured in the pseudorapidity range
             [Formula: see text] with the event-plane method. In order to
             include tracks with very low transverse momentum [Formula:
             see text], thus reducing the uncertainty in [Formula: see
             text] integrated over [Formula: see text], a [Formula: see
             text] data sample recorded without a magnetic field in the
             tracking detectors is used. The centrality dependence of the
             integrated [Formula: see text] is compared to other
             measurements obtained with higher [Formula: see text]
             thresholds. The integrated elliptic flow is weakly
             decreasing with [Formula: see text]. The integrated
             [Formula: see text] transformed to the rest frame of one of
             the colliding nuclei is compared to the lower-energy RHIC
             data.},
   Doi = {10.1140/epjc/s10052-014-2982-4},
   Key = {fds310539}
}

@article{fds310540,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
             Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Guimarães da Costa and JB and Bartoldus, R and Barton,
             AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
             CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
             J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
             R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart,
             D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens,
             JC},
   Title = {Search for direct top squark pair production in events with
             a [Formula: see text] boson, [Formula: see text]-jets and
             missing transverse momentum in [Formula: see text] TeV
             [Formula: see text] collisions with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {74},
   Number = {6},
   Pages = {2883},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2883-6},
   Abstract = {A search is presented for direct top squark pair production
             using events with at least two leptons including a
             same-flavour opposite-sign pair with invariant mass
             consistent with the [Formula: see text] boson mass, jets
             tagged as originating from [Formula: see text]-quarks and
             missing transverse momentum. The analysis is performed with
             proton-proton collision data at [Formula: see text]
             collected with the ATLAS detector at the LHC in 2012
             corresponding to an integrated luminosity of
             20.3 fb[Formula: see text]. No excess beyond the Standard
             Model expectation is observed. Interpretations of the
             results are provided in models based on the direct pair
             production of the heavier top squark state ([Formula: see
             text]) followed by the decay to the lighter top squark state
             ([Formula: see text]) via [Formula: see text], and for
             [Formula: see text] pair production in natural
             gauge-mediated supersymmetry breaking scenarios where the
             neutralino ([Formula: see text]) is the next-to-lightest
             supersymmetric particle and decays producing a [Formula: see
             text] boson and a gravitino ([Formula: see text]) via the
             [Formula: see text] process.},
   Doi = {10.1140/epjc/s10052-014-2883-6},
   Key = {fds310540}
}

@article{fds313370,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for top quark decays t → qH with H → γγ using
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {6},
   Year = {2014},
   Month = {January},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP06(2014)008},
   Abstract = {A search is performed for flavour-changing neutral currents
             in the decay of a top quark to an up-type (c, u) quark and a
             Higgs boson, where the Higgs boson decays to two photons.
             The proton-proton collision data set used corresponds to 4.7
             fb-1 at √ = 7TeV and 20.3fb-1 at √ = 8TeV collected by
             the ATLAS experiment at the LHC. Top quark pair events are
             searched for in which one top quark decays to qH and the
             other decays to bW. Both the hadronic and the leptonic decay
             modes of the W boson are used. No significant signal is
             observed and an upper limit is set on the t → qH branching
             ratio of 0.79 at the 95% confidence level. The corresponding
             limit on the tqH coupling combination λtcH2 + λtuH2 is
             0.17. © 2014 The Author(s).},
   Doi = {10.1007/JHEP06(2014)008},
   Key = {fds313370}
}

@article{fds308946,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
             JF},
   Title = {Measurement of the mass difference between top and anti-top
             quarks in pp collisions at √s=7 TeV using the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {728},
   Pages = {363-379},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2013.12.010},
   Abstract = {A measurement of the mass difference between top and
             anti-top quarks is presented. In a 4.7 fb−1 data sample of
             proton–proton collisions at s=7 TeV recorded with the
             ATLAS detector at the LHC, events consistent with tt¯
             production and decay into a single charged lepton final
             state are reconstructed. For each event, the mass difference
             between the top and anti-top quark candidate is calculated.
             A two b-tag requirement is used in order to reduce the
             background contribution. A maximum likelihood fit to these
             per-event mass differences yields Δm≡mt−mt¯=0.67±0.61(stat)±0.41(syst)
             GeV, consistent with CPT invariance.},
   Doi = {10.1016/j.physletb.2013.12.010},
   Key = {fds308946}
}

@article{fds308942,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
             JF},
   Title = {Search for a multi-Higgs-boson cascade in W+W
             -bb̄ events with the ATLAS detector in pp
             collisions at √s = 8 TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.032002},
   Abstract = {A search is presented for new particles in an extension to
             the Standard Model that includes a heavy Higgs boson (H0),
             an intermediate charged Higgs-boson pair (H-), and a light
             Higgs boson (h0). The analysis searches for events involving
             the production of a single heavy neutral Higgs boson which
             decays to the charged Higgs boson and a W boson, where the
             charged Higgs boson subsequently decays into a W boson and
             the lightest neutral Higgs boson decaying to a
             bottom-antibottom-quark pair. Such a cascade results in a
             W-boson pair and a bottom-antibottom-quark pair in the final
             state. Events with exactly one lepton, missing transverse
             momentum, and at least four jets are selected from a data
             sample corresponding to an integrated luminosity of 20.3
             fb-1, collected by the ATLAS detector in proton-proton
             collisions at √s = 8 TeV at the LHC. The data are found to
             be consistent with Standard Model predictions, and 95%
             confidence-level upper limits are set on the product of
             cross section and branching ratio. These limits range from
             0.065 to 43 pb as a function of H0 and H- masses, with mh0
             fixed at 125 GeV. © 2014 CERN, for the ATLAS
             Collaboration.},
   Doi = {10.1103/PhysRevD.89.032002},
   Key = {fds308942}
}

@article{fds308939,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
             P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canelli, F and Canepa,
             A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
             V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
             J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
   Title = {Search for quantum black hole production in
             high-invariant-mass lepton+jet final states using pp
             collisions at √s=8  TeV and the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {9},
   Pages = {091804},
   Year = {2014},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.112.091804},
   Abstract = {This Letter presents a search for quantum black-hole
             production using 20.3 fb-1 of data collected with the ATLAS
             detector in pp collisions at the LHC at √s = 8 TeV. The
             quantum black holes are assumed to decay into a final state
             characterized by a lepton (electron or muon) and a jet. In
             either channel, no event with a lepton-jet invariant mass of
             3.5 TeV or more is observed, consistent with the expected
             background. Limits are set on the product of cross sections
             and branching fractions for the lepton+jet final states of
             quantum black holes produced in a search region for
             invariant masses above 1 TeV. The combined 95% confidence
             level upper limit on this product for quantum black holes
             with threshold mass above 3.5 TeV is 0.18 fb. This limit
             constrains the threshold quantum black-hole mass to be above
             5.3 TeV in the model considered.},
   Doi = {10.1103/physrevlett.112.091804},
   Key = {fds308939}
}

@article{fds308941,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester Iii and WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {First search for exotic Z Boson decays into photons and
             neutral pions in hadron collisions.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {11},
   Pages = {111803},
   Year = {2014},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.112.111803},
   Abstract = {A search for forbidden and exotic Z boson decays in the
             diphoton mass spectrum is presented for the first time in
             hadron collisions, based on data corresponding to 10.0
             fb(-1) of integrated luminosity from proton-antiproton
             collisions at √s = 1.96 TeV collected by the CDF
             experiment. No evidence of signal is observed, and 95%
             credibility level Bayesian upper limits are set on the
             branching ratios of decays of the Z boson to a photon and
             neutral pion (which is detected as a photon), a pair of
             photons, and a pair of neutral pions. The observed branching
             ratio limits are 2.01 × 10(-5) for Z → π(0)γ, 1.46 ×
             10(-5) for Z → γγ, and 1.52 × 10(-5) for Z →
             π(0)π(0). The Z → π(0)γ and Z → γγ limits improve
             the most stringent results from other experiments by factors
             of 2.6 and 3.6, respectively. The Z → π(0)π(0) branching
             ratio limit is the first experimental result on this
             decay.},
   Doi = {10.1103/physrevlett.112.111803},
   Key = {fds308941}
}

@article{fds308940,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
   Title = {Measurement of the inclusive isolated prompt photons cross
             section in pp collisions at √s =7 TeV with the ATLAS
             detector using 4.6 fb-1},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.052004},
   Abstract = {A measurement of the cross section for the production of
             isolated prompt photons in pp collisions at a center-of-mass
             energy √s=7 TeV is presented. The results are based on an
             integrated luminosity of 4.6 fb-1 collected with the ATLAS
             detector at the LHC. The cross section is measured as a
             function of photon pseudorapidity ηγ and transverse energy
             ETγ in the kinematic range 100≤ETγ<1000 GeV and in the
             regions |ηγ|<1.37 and 1.52≤|ηγ|<2.37. The results are
             compared to leading-order parton-shower Monte Carlo models
             and next-to-leading-order perturbative QCD calculations.
             Next-to-leading-order perturbative QCD calculations agree
             well with the measured cross sections as a function of ETγ
             and ηγ.},
   Doi = {10.1103/PhysRevD.89.052004},
   Key = {fds308940}
}

@article{fds225671,
   Author = {Atlas Collaboration},
   Title = {Search for Invisible Decays of a Higgs Boson Produced in
             Association with a Z Boson in ATLAS},
   Journal = {Phys. Lett. B 732C (2014)},
   Year = {2014},
   Month = {March},
   Key = {fds225671}
}

@article{fds308934,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
             A},
   Title = {Combination of measurements of the top-quark pair production
             cross section from the Tevatron Collider},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072001},
   Abstract = {We combine six measurements of the inclusive top-quark pair
             (tt̄) production cross section (σtt̄) from data collected
             with the CDF and D0 detectors at the Fermilab Tevatron with
             proton-antiproton collisions at s=1.96TeV. The data
             correspond to integrated luminosities of up to 8.8fb-1. We
             obtain a value of σtt̄=7.60±0.41pb for a top-quark mass
             of mt=172.5GeV. The contributions to the uncertainty are
             0.20 pb from statistical sources, 0.29 pb from systematic
             sources, and 0.21 pb from the uncertainty on the integrated
             luminosity. The result is in good agreement with the
             standard model expectation of 7.35-0.33+0.28pb at
             next-to-next-to-leading order and next-to-next-to leading
             logarithms in perturbative QCD. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.89.072001},
   Key = {fds308934}
}

@article{fds308936,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
             M},
   Title = {Measurement of the production cross section of prompt J/ψ
             mesons in association with a W± boson in pp collisions at
             √s = 7 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2014)172},
   Abstract = {The process pp → W±J/ψ provides a powerful probe of the
             production mechanism of charmonium in hadronic collisions,
             and is also sensitive to multiple parton interactions in the
             colliding protons. Using the 2011 ATLAS dataset of 4.5 fb-1
             of p s = 7TeV pp collisions at the LHC, the first
             observation is made of the production of W± + prompt J/
             events in hadronic collisions, using W± → μ and J/ψ →
             μ+μ-. A yield of 27.4±7.5 -6.5 W± + prompt J/ψ events
             is observed, with a statistical significance of 5.1. The
             production rate as a ratio to the inclusive W± boson
             production rate is measured, and the double parton
             scattering contribution to the cross section is estimated.
             Copyright CERN, for the benefit of the ATLAS
             Collaboration.},
   Doi = {10.1007/JHEP04(2014)172},
   Key = {fds308936}
}

@article{fds308933,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
             M and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith,
             D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A},
   Title = {Precise measurement of the W -boson mass with the Collider
             Detector at Fermilab},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Pages = {072003},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072003},
   Abstract = {We present a measurement of the W-boson mass, MW, using data
             corresponding to 2.2fb-1 of integrated luminosity collected
             in pp̄ collisions at s=1.96TeV with the CDF II detector at
             the Fermilab Tevatron. The selected sample of 470126 W→eν
             candidates and 624708 W→μν candidates yields the
             measurement MW=80387±12(stat)±15(syst)=80387±19MeV/c2.
             This is the most precise single measurement of the W-boson
             mass to date. © 2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.89.072003},
   Key = {fds308933}
}

@article{fds308932,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Indirect measurement of sin2θW (or MW) using μ+μ- pairs
             from γ* /Z bosons produced in p p ̄ collisions at a
             center-of-momentum energy of 1.96 TeV INDIRECT MEASUREMENT
             of sin2θW (OR ... T. AALTONEN et al.},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072005},
   Abstract = {Drell-Yan lepton pairs are produced in the process
             pp̄→μ+μ- +X through an intermediate γ*/Zboson. The
             forward-backward asymmetry in the polar-angle distribution
             of the μ- as a function of the invariant mass of the μ+μ-
             pair is used to obtain the effective leptonic determination
             sin2θefflept of the electroweak-mixing parameter sin2θW,
             from which the value of sin2θW is derived assuming the
             standard model. The measurement sample, recorded by the
             Collider Detector at Fermilab (CDF), corresponds to 9.2fb-1
             of integrated luminosity from pp̄ collisions at a
             center-of-momentum energy of 1.96 TeV, and is the full CDF
             Run II data set. The value of sin2θefflept is found to be
             0.2315±0. 0010, where statistical and systematic
             uncertainties are combined in quadrature. When interpreted
             within the context of the standard model using the on-shell
             renormalization scheme, where sin2θW=1-MW2/MZ2, the
             measurement yields sin2θW=0.2233±0.0009, or equivalently a
             W-boson mass of 80.365±0.047GeV/c2. The value of the
             W-boson mass is in agreement with previous determinations in
             electron-positron collisions and at the Tevatron collider.
             © 2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.89.072005},
   Key = {fds308932}
}

@article{fds308935,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
             BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
             S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
             BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
             J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
             V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
             E and Arik, M and Armbruster, AJ},
   Title = {Study of heavy-flavor quarks produced in association with
             top-quark pairs at s =7TeV using the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072012},
   Abstract = {Using a sample of dilepton top-quark pair (tt̄) candidate
             events, a study is performed of the production of top-quark
             pairs together with heavy-flavor (HF) quarks, the sum of
             tt̄+b+X and tt̄+c+X, collectively referred to as tt̄+HF.
             The data set used corresponds to an integrated luminosity of
             4.7fb-1 of proton-proton collisions at a center-of-mass
             energy of 7 TeV recorded by the ATLAS detector at the CERN
             Large Hadron Collider. The presence of additional HF (b or
             c) quarks in the tt̄ sample is inferred by looking for
             events with at least three b-tagged jets, where two are
             attributed to the b quarks from the tt̄ decays and the
             third to additional HF production. The dominant background
             to tt̄+HF in this sample is tt̄+jet events in which a
             light-flavor jet is misidentified as a heavy-flavor jet. To
             determine the heavy- and light-flavor content of the
             additional b-tagged jets, a fit to the vertex mass
             distribution of b-tagged jets in the sample is performed.
             The result of the fit shows that 79±14(stat)±22(syst) of
             the 105 selected extra b-tagged jets originate from HF
             quarks, 3 standard deviations away from the hypothesis of
             zero tt̄+HF production. The result for extra HF production
             is quoted as a ratio (RHF) of the cross section for tt̄+HF
             production to the cross section for tt̄ production with at
             least one additional jet. Both cross sections are measured
             in a fiducial kinematic region within the ATLAS acceptance.
             RHF is measured to be [6.2±1.1(stat)±1.8(syst)]% for jets
             with pT>25GeV and |η|<2.5, in agreement with the
             expectations from Monte Carlo generators. © 2014 CERN, for
             the ATLAS Collaboration.},
   Doi = {10.1103/PhysRevD.89.072012},
   Key = {fds308935}
}

@article{fds308931,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Mass and lifetime measurements of bottom and charm baryons
             in p p ̄ collisions at s =1.96TeV MASS and LIFETIME
             MEASUREMENTS of BOTTOM and ⋯ T. AALTONEN},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {April},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.072014},
   Abstract = {We report on mass and lifetime measurements of several
             ground state charmed and bottom baryons, using a data sample
             corresponding to 9.6fb-1 from pp̄ collisions at s=1.96TeV
             and recorded with the Collider Detector at Fermilab. Baryon
             candidates are reconstructed from data collected with an
             online event selection designed for the collection of
             long-lifetime heavy-flavor decay products and a second event
             selection designed to collect J/ ψ→μ+μ- candidates.
             First evidence for the process Ωb-→Ωc0π- is presented
             with a significance of 3.3σ. We measure the following
             baryon masses: M(Ξc0)=2470.85±0.24(stat)
             ±0.55(syst)MeV/c2,M(Ξc+)=2468.00±0.18(stat)±0.51(syst)
             MeV/c2,M(Λb)=5620.15±0.31(stat)±0.47(syst)MeV/c2,M(Ξb-)=
             5793.4±1.8(stat)±0.7(syst)MeV/c2,M(Ξb0)=5788.7±4.3(stat)
             ±1.4(syst)MeV/c2,andM(Ωb-)=6047.5±3.8(stat)±0.6(syst)
             MeV/c2.The isospin splitting of the Ξb-,0 states is found
             to be M(Ξb-)-M(Ξb0)=4.7±4.7(stat)±0.7(syst)MeV/c2. The
             isospin splitting of the Ξc0,+ states is found to be
             M(Ξc0)-M(Ξc+)=2. 85±0.30(stat)±0.04(syst)MeV/c2. The
             following lifetime measurements are made:
             τ(Λb)=1.565±0.035(stat)±0. 020(syst)ps,τ(Ξb-)=1.32±0.14(stat)±0.02(syst)ps,
             τ(Ωb-)=1.66-0.40+0.53(stat)±0.02(syst)ps. © 2014
             American Physical Society.},
   Doi = {10.1103/PhysRevD.89.072014},
   Key = {fds308931}
}

@article{fds308929,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and A°kesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ},
   Title = {Search for Higgs boson decays to a photon and a Z boson in
             pp collisions at s=7 and 8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {732},
   Pages = {8-27},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.03.015},
   Abstract = {A search is reported for a neutral Higgs boson in the decay
             channel H→Zγ, Z→ℓ +ℓ -(ℓ = e, μ), using 4.5
             fb-1of pp collisions at s=7 TeV and 20.3 fb-1of pp
             collisions at s=8 TeV, recorded by the ATLAS detector at the
             CERN Large Hadron Collider. The observed distribution of the
             invariant mass of the three final-state particles,mℓℓγ,
             is consistent with the Standard Model hypothesis in the
             investigated mass range of 120-150 GeV. For a Higgs boson
             with a mass of 125.5 GeV, the observed upper limit at the
             95% confidence level is 11 times the Standard Model
             expectation. Upper limits are set on the cross section times
             branching ratio of a neutral Higgs boson with mass in the
             range 120-150 GeV between 0.13 and 0.5 pb for s=8 TeV at 95%
             confidence level. © 2014.},
   Doi = {10.1016/j.physletb.2014.03.015},
   Key = {fds308929}
}

@article{fds310526,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
             M},
   Title = {Measurement of the production of a W boson in association
             with a charm quark in pp collisions at √s = 7TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {5},
   Pages = {1-67},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2014)068},
   Abstract = {The production of a W boson in association with a single
             charm quark is studied using 4.6 fb-1 of pp collision data
             at √s = 7TeV collected with the ATLAS detector at the
             Large Hadron Collider. In events in which a W boson decays
             to an electron or muon, the charm quark is tagged either by
             its semileptonic decay to a muon or by the presence of a
             charmed meson. The integrated and differential cross
             sections as a function of the pseudorapidity of the lepton
             from the W-boson decay are measured. Results are compared to
             the predictions of next-to-leading-order QCD calculations
             obtained from various parton distribution function
             parameterisations. The ratio of the strange-to-down
             sea-quark distributions is determined to be 0.96+-00.30 at
             Q2 = 1.9 GeV, which supports the hypothesis of an
             SU(3)-symmetric composition of the light-quark sea.
             Additionally the cross-section ratio σ(W+ + c)/σ(W- +c) is
             compared to the predictions obtained using parton
             distribution function parameterisations with different
             assumptions about the s–s quark asymmetry.},
   Doi = {10.1007/JHEP05(2014)068},
   Key = {fds310526}
}

@article{fds308928,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Invariant-mass distribution of jet pairs produced in
             association with a W boson in p p ̄ collisions at s
             =1.96TeV using the full CDF Run II data set invariant-mass
             distribution of ⋯ T. Aaltonen et al.},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {9},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.092001},
   Abstract = {We report on a study of the dijet invariant-mass
             distribution in events with one identified lepton, a
             significant imbalance in the total event transverse
             momentum, and two jets. This distribution is sensitive to
             the possible production of a new particle in association
             with a W boson, where the boson decays leptonically. We use
             the full data set of proton-antiproton collisions at 1.96
             TeV center-of-mass energy collected by the Collider Detector
             at the Fermilab Tevatron, corresponding to an integrated
             luminosity of 8.9fb-1. The data are found to be consistent
             with standard model expectations, and a 95% confidence level
             upper limit is set on the production cross section of a W
             boson in association with a new particle decaying into two
             jets. © 2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.89.092001},
   Key = {fds308928}
}

@article{fds308927,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Study of top quark production and decays involving a tau
             lepton at CDF and limits on a charged Higgs boson
             contribution},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.091101},
   Abstract = {We present an analysis of top-antitop quark production and
             decay into a tau lepton, tau neutrino, and bottom quark
             using data from 9fb-1 of integrated luminosity at the
             Collider Detector at Fermilab. Dilepton events, where one
             lepton is an energetic electron or muon and the other a
             hadronically decaying tau lepton, originating from
             proton-antiproton collisions at s=1.96TeV, are used. A
             top-antitop quark production cross section of 8.1±2.1pb is
             measured, assuming standard-model top quark decays. By
             separately identifying for the first time the single-tau and
             the ditau components, we measure the branching fraction of
             the top quark into the tau lepton, tau neutrino, and bottom
             quark to be (9.6±2.8)%. The branching fraction of top quark
             decays into a charged Higgs boson and a bottom quark, which
             would imply violation of lepton universality, is limited to
             be less than 5.9% at a 95% confidence level [for
             B(H-→τν̄)=1]. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.89.091101},
   Key = {fds308927}
}

@article{fds336990,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for direct production of charginos, neutralinos and
             sleptons in final states with two leptons and missing
             transverse momentum in pp collisions at √s = 8TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {5},
   Pages = {1-51},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2014)071},
   Abstract = {Searches for the electroweak production of charginos,
             neutralinos and sleptons in final states characterized by
             the presence of two leptons (electrons and muons) and
             missing transverse momentum are performed using 20.3 fb-1of
             proton-proton collision data at √s = 8TeV recorded with
             the ATLAS experiment at the Large Hadron Collider. No
             significant excess beyond Standard Model expectations is
             observed. Limits are set on the masses of the lightest
             chargino, next-to-lightest neutralino and sleptons for
             different lightest-neutralino mass hypotheses in simplified
             models. Results are also interpreted in various scenarios of
             the phenomenological Minimal Supersymmetric Standard
             Model.},
   Doi = {10.1007/JHEP05(2014)071},
   Key = {fds336990}
}

@article{fds308930,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Measurement of the parity-violating asymmetry parameter αb
             and the helicity amplitudes for the decay Λb0 →j /ψ Λ0
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.092009},
   Abstract = {A measurement of the parity-violating decay asymmetry
             parameter, αb, and the helicity amplitudes for the decay
             Λb0→J/ψ(μ+μ-)Λ0(pπ-) is reported. The analysis is
             based on 1400 Λb0 and Λ¯b0 baryons selected in 4.6 fb-1
             of proton-proton collision data with a center-of-mass energy
             of 7 TeV recorded by the ATLAS experiment at the LHC. By
             combining the Λb0 and Λ¯b0 samples under the assumption
             of CP conservation, the value of αb is measured to be
             0.30±0.16(stat)±0.06(syst). This measurement provides a
             test of theoretical models based on perturbative QCD or
             heavy-quark effective theory.},
   Doi = {10.1103/PhysRevD.89.092009},
   Key = {fds308930}
}

@article{fds308922,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
             Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JC and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC},
   Title = {Measurements of four-lepton production at the Z resonance in
             pp collisions at sqrt[s] = 7 and 8 TeV with
             ATLAS.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231806},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231806},
   Abstract = {Measurements of four-lepton (4ℓ, ℓ=e,μ) production
             cross sections at the Z resonance in pp collisions at the
             LHC with the ATLAS detector are presented. For dilepton and
             four-lepton invariant mass regions m(ℓ+ℓ(-)) > 5 GeV and
             80<m(4ℓ) < 100 GeV, the measured cross sections are 76 ±
             18(stat) ± 4(syst) ± 1.4(lumi) fb and 107 ± 9(stat) ±
             4(syst) ± 3.0(lumi) fb at sqrt[s] = 7 and 8 TeV,
             respectively. By subtracting the nonresonant 4ℓ production
             contributions and normalizing with Z → μ(+)μ(-) events,
             the branching fraction for the Z boson decay to 4ℓ is
             determined to be (3.20 ± 0.25(stat) ± 0.13(syst)) ×
             10(-6), consistent with the standard model
             prediction.},
   Doi = {10.1103/physrevlett.112.231806},
   Key = {fds308922}
}

@article{fds308924,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
             O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
             D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de Barbaro, P and de Jong, SJ and De La
             Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov, SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto, F and Di Canto and A and Di Ruzza,
             B and Diehl, HT and Diesburg, M and Ding, PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti,
             A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov,
             V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu,
             G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
             La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
             A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
             AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim,
             YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich, I and Knoepfel,
             K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr,
             T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon,
             K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
             H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour,
             J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega,
             J and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta,
             A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed,
             S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett,
             J and Neu, C and Neustroev, P},
   Title = {Observation of s-channel production of single top quarks at
             the Tevatron.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231803},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231803},
   Abstract = {We report the first observation of single-top-quark
             production in the s channel through the combination of the
             CDF and D0 measurements of the cross section in
             proton-antiproton collisions at a center-of-mass energy of
             1.96 TeV. The data correspond to total integrated
             luminosities of up to 9.7 fb(-1) per experiment. The
             measured cross section is σ(s) = 1.29(-0.24)(+0.26) pb. The
             probability of observing a statistical fluctuation of the
             background to a cross section of the observed size or larger
             is 1.8 × 10(-10), corresponding to a significance of 6.3
             standard deviations for the presence of an s-channel
             contribution to the production of single-top
             quarks.},
   Doi = {10.1103/physrevlett.112.231803},
   Key = {fds308924}
}

@article{fds308925,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Evidence for s-channel single-top-quark production in events
             with one charged lepton and two jets at CDF.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231804},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231804},
   Abstract = {We report evidence for s-channel single-top-quark production
             in proton-antiproton collisions at center-of-mass energy
             sqrt[s] = 1.96 TeV using a data set that corresponds to an
             integrated luminosity of 9.4 fb(-1) collected by the
             Collider Detector at Fermilab. We select events consistent
             with the s-channel process including two jets and one
             leptonically decaying W boson. The observed significance is
             3.8 standard deviations with respect to the background-only
             prediction. Assuming a top-quark mass of 172.5 GeV/c(2), we
             measure the s-channel cross section to be 1.41(-0.42)(+0.44)
             pb.},
   Doi = {10.1103/physrevlett.112.231804},
   Key = {fds308925}
}

@article{fds308926,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Search for s-channel single-top-quark production in events
             with missing energy plus jets in pp collisions at sqrt[s] =
             1.96 TeV.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {23},
   Pages = {231805},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.112.231805},
   Abstract = {The first search for single-top-quark production from the
             exchange of an s-channel virtual W boson using events with
             an imbalance in the total transverse energy, b-tagged jets,
             and no identified leptons is presented. Assuming the
             electroweak production of top quarks of mass 172.5 GeV/c(2)
             in the s channel, a cross section of 1.12(-0.57)(+0.61)
             (stat+syst) pb with a significance of 1.9 standard
             deviations is measured. This measurement is combined with
             the result obtained from events with an imbalance in total
             transverse momentum, b-tagged jets, and exactly one
             identified lepton, yielding a cross section of
             1.36(-0.32)(+0.37) (stat+syst) pb, with a significance of
             4.2 standard deviations.},
   Doi = {10.1103/physrevlett.112.231805},
   Key = {fds308926}
}

@article{fds310541,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
             A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
             JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
             G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
             G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
             A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
             C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
             L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
             Collaboration)},
   Title = {Measurement of B(t→Wb)/B(t→Wq) in top-quark-pair decays
             using dilepton events and the full CDF Run II data
             set.},
   Journal = {Physical review letters},
   Volume = {112},
   Number = {22},
   Pages = {221801},
   Year = {2014},
   Month = {June},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.112.221801},
   Abstract = {We present a measurement of the ratio of the top-quark
             branching fractions R=B(t→Wb)/B(t→Wq), where q
             represents any quark flavor, in events with two charged
             leptons, imbalance in total transverse energy, and at least
             two jets. The measurement uses proton-antiproton collision
             data at center-of-mass energy 1.96 TeV, corresponding to an
             integrated luminosity of 8.7  fb^{-1} collected with the
             Collider Detector at Fermilab during Run II of the Tevatron.
             We measure R to be 0.87±0.07, and extract the magnitude of
             the top-bottom quark coupling to be |V_{tb}|=0.93±0.04,
             assuming three generations of quarks. Under these
             assumptions, a lower limit of |V_{tb}|>0.85(0.87) at 95%
             (90%) credibility level is set.},
   Doi = {10.1103/physrevlett.112.221801},
   Key = {fds310541}
}

@article{fds310524,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Measurement of the ZZ production cross section using the
             full CDF II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {89},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.89.112001},
   Abstract = {We present a measurement of the ZZ-boson pair-production
             cross section in 1.96 TeV center-of-mass energy pp̄
             collisions. We reconstruct final states incorporating four
             charged leptons or two charged leptons and two neutrinos
             from the full data set collected by the Collider Detector
             experiment at the Fermilab Tevatron, corresponding to
             9.7fb-1 of integrated luminosity. Combining the results
             obtained from each final state, we measure a cross section
             of 1.04-0.25+0.32pb, in good agreement with the standard
             model prediction at next-to-leading order in the
             strong-interaction coupling. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.89.112001},
   Key = {fds310524}
}

@article{fds310514,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
             M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
             C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
             T and Hatakeyama, K and Hays, C and Heinrich, J and Henry, S and Herndon,
             M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
             L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
             A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
             A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
             E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
             E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
             Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Measurement of the inclusive leptonic asymmetry in top-quark
             pairs that decay to two charged leptons at
             CDF.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {4},
   Pages = {042001},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.113.042001},
   Abstract = {We measure the inclusive forward-backward asymmetry of the
             charged-lepton pseudorapidities from top-quark pairs
             produced in proton-antiproton collisions and decaying to
             final states that contain two charged leptons (electrons or
             muons). The data are collected with the Collider Detector at
             Fermilab and correspond to an integrated luminosity of 9.1
             fb(-1). We measure the leptonic forward-backward asymmetry,
             A(FB)(ℓ), to be 0.072 ± 0.060 and the leptonic pair
             forward-backward asymmetry, A(FB)(ℓℓ), to be 0.076 ±
             0.082. The measured values can be compared with the standard
             model predictions of A(FB)(ℓ) = 0.038 ± 0.003 and
             A(FB)(ℓℓ) = 0.048 ± 0.004, respectively. Additionally,
             we combine the A(FB)(ℓ) result with a previous
             determination from a final state with a single lepton and
             hadronic jets and obtain A(FB)(ℓ) = 0.090(-0.026)(+0.028).},
   Doi = {10.1103/physrevlett.113.042001},
   Key = {fds310514}
}

@article{fds310515,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Monitoring and data quality assessment of the ATLAS liquid
             argon calorimeter},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {7},
   Pages = {P07024-P07024},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1088/1748-0221/9/07/P07024},
   Abstract = {The liquid argon calorimeter is a key component of the ATLAS
             detector installed at the CERN Large Hadron Collider. The
             primary purpose of this calorimeter is the measurement of
             electron and photon kinematic properties. It also provides a
             crucial input for measuring jets and missing transverse
             momentum. An advanced data monitoring procedure was designed
             to quickly identify issues that would affect detector
             performance and ensure that only the best quality data are
             used for physics analysis. This article presents the
             validation procedure developed during the 2011 and 2012 LHC
             data-taking periods, in which more than 98% of the
             proton-proton luminosity recorded by ATLAS at a
             centre-of-mass energy of 7-8 TeV had calorimeter data
             quality suitable for physics analysis. © CERN 2014 for the
             benefit of the ATLAS collaboration.},
   Doi = {10.1088/1748-0221/9/07/P07024},
   Key = {fds310515}
}

@article{fds310516,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for dark matter in events with a Z boson and missing
             transverse momentum in pp collisions at s =8TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.012004},
   Abstract = {A search is presented for production of dark-matter
             particles recoiling against a leptonically decaying Z boson
             in 20.3fb-1 of pp collisions at s=8TeV with the ATLAS
             detector at the Large Hadron Collider. Events with large
             missing transverse momentum and two oppositely charged
             electrons or muons consistent with the decay of a Z boson
             are analyzed. No excess above the Standard Model prediction
             is observed. Limits are set on the mass scale of the contact
             interaction as a function of the dark-matter particle mass
             using an effective field theory description of the
             interaction of dark matter with quarks or with Z bosons.
             Limits are also set on the coupling and mediator mass of a
             model in which the interaction is mediated by a scalar
             particle. © 2014 CERN, for the ATLAS Collaboration.},
   Doi = {10.1103/PhysRevD.90.012004},
   Key = {fds310516}
}

@article{fds310519,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Search for new physics in trilepton events and limits on the
             associated chargino-neutralino production at
             CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {1},
   Pages = {012011},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.012011},
   Abstract = {We perform a search for new physics using final states
             consisting of three leptons and a large imbalance in
             transverse momentum resulting from proton-antiproton
             collisions at 1.96 TeV center-of-mass energy. We use data
             corresponding to 5.8fb-1 of integrated luminosity recorded
             by the CDF II detector at the Tevatron collider. Our main
             objective is to investigate possible new low-momentum (down
             to 5GeV/c) multileptonic final states not investigated by
             LHC experiments. Relative to previous CDF analyses, we
             expand the geometric and kinematic coverage of electrons and
             muons and utilize tau leptons that decay hadronically.
             Inclusion of tau leptons is particularly important for
             supersymmetry (SUSY) searches. The results are consistent
             with standard-model predictions within 1.85σ. By optimizing
             our event selection to increase sensitivity to the minimal
             supergravity (mSUGRA) SUSY model, we set limits on the
             associated production of chargino and next-to-lightest
             neutralino, the SUSY partners of the electroweak gauge
             bosons. We exclude cross sections up to 0.1 pb and chargino
             masses up to 168GeV/c2 at 95% C.L., for a suitable set of
             mSUGRA parameters. We also exclude a region of the
             two-dimensional space of the masses of the neutralino and
             the supersymmetric partner of the tau lepton, not previously
             excluded at the Tevatron. © 2014 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.90.012011},
   Key = {fds310519}
}

@article{fds310518,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Study of orbitally excited B mesons and evidence for a new
             Bπ resonance},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {1},
   Pages = {012013},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.012013},
   Abstract = {Using the full CDF Run II data sample, we report evidence
             for a new resonance, which we refer to as B(5970), found
             simultaneously in the B0π+ and B+π- mass distributions
             with a significance of 4.4 standard deviations. We further
             report the first study of resonances consistent with
             orbitally excited B+ mesons and an updated measurement of
             the properties of orbitally excited B0 and Bs0 mesons. We
             measure the masses and widths of all states, as well as the
             relative production rates of the B1, B2*, and B(5970) states
             and the branching fraction of the Bs2*0 state to either
             B*+K- and B+K-. Furthermore, we measure the production rates
             of the orbitally excited B0,+ states relative to the B0,+
             ground state. The masses of the new B(5970) resonances are
             5978±5(stat)±12(syst)MeV/c2 for the neutral state and
             5961±5(stat)±12(syst)MeV/c2 for the charged state,
             assuming that the resonance decays into Bπ final states.
             The properties of the orbitally excited and the new
             B(5970)0,+ states are compatible with isospin symmetry. ©
             2014 American Physical Society.},
   Doi = {10.1103/PhysRevD.90.012013},
   Key = {fds310518}
}

@article{fds325315,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Da Barreiro Guimarães Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
             GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
             K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and De Bruckman Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
             B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
             P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
             CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Cherkaoui Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Measurement of χc1 and ψχc2 production with √s = 7 TeV
             pp collisions at ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {7},
   Pages = {1-51},
   Publisher = {Springer Verlag},
   Year = {2014},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2014)154},
   Abstract = {The prompt and non-prompt production cross-sections for the
             χc1 and χc2 charmonium states are measured in pp
             collisions at √s = 7TeV with the ATLAS detector at the LHC
             using 4.5 fb−1 of integrated luminosity. The χc states
             are reconstructed through the radiative decay χc → J/ψγ
             (with J/ψ → μ+μ−) where photons are reconstructed
             from γ → e+e− conversions. The production rate of the
             χc2 state relative to the χc1 state is measured for prompt
             and non-prompt χc as a function of J/ψ transverse
             momentum. The prompt χc cross-sections are combined with
             existing measurements of prompt J/ψ production to derive
             the fraction of prompt J/ψ produced in feed-down from χc
             decays. The fractions of χc1 and χc2 produced in b-hadron
             decays are also measured.},
   Doi = {10.1007/JHEP07(2014)154},
   Key = {fds325315}
}

@article{fds310511,
   Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
             C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
             C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso,
             S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
   Title = {Measurement of the underlying event in jet events from
             7 TeV proton–proton collisions with the ATLAS
             detector},
   Journal = {European Physical Journal C},
   Volume = {74},
   Number = {8},
   Pages = {1-29},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {August},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-2965-5},
   Abstract = {Distributions sensitive to the underlying event in QCD jet
             events have been measured with the ATLAS detector at the
             LHC, based on (Formula presented.) of proton–proton
             collision data collected at a centre-of-mass energy of
             7 (Formula presented.). Charged-particle mean (Formula
             presented.) and densities of all-particle (Formula
             presented.) and charged-particle multiplicity and (Formula
             presented.) have been measured in regions azimuthally
             transverse to the hardest jet in each event. These are
             presented both as one-dimensional distributions and with
             their mean values as functions of the leading-jet transverse
             momentum from 20 to 800 (Formula presented.). The
             correlation of charged-particle mean (Formula presented.)
             with charged-particle multiplicity is also studied, and the
             (Formula presented.) densities include the forward rapidity
             region; these features provide extra data constraints for
             Monte Carlo modelling of colour reconnection and
             beam-remnant effects respectively. For the first time,
             underlying event observables have been computed separately
             for inclusive jet and exclusive dijet event selections,
             allowing more detailed study of the interplay of multiple
             partonic scattering and QCD radiation contributions to the
             underlying event. Comparisons to the predictions of
             different Monte Carlo models show a need for further model
             tuning, but the standard approach is found to generally
             reproduce the features of the underlying event in both types
             of event selection.},
   Doi = {10.1140/epjc/s10052-014-2965-5},
   Key = {fds310511}
}

@article{fds310512,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O and Arnal, V},
   Title = {Measurement of event-plane correlations in √sNN
             = 2.76 TeV lead-lead collisions with the ATLAS
             detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {90},
   Number = {2},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevC.90.024905},
   Abstract = {A measurement of event-plane correlations involving two or
             three event planes of different order is presented as a
             function of centrality for 7 μb-1 Pb+Pb collision data at
             sNN=2.76 TeV, recorded by the ATLAS experiment at the Large
             Hadron Collider. Fourteen correlators are measured using a
             standard event-plane method and a scalar-product method, and
             the latter method is found to give a systematically larger
             correlation signal. Several different trends in the
             centrality dependence of these correlators are observed.
             These trends are not reproduced by predictions based on the
             Glauber model, which includes only the correlations from the
             collision geometry in the initial state. Calculations that
             include the final-state collective dynamics are able to
             describe qualitatively, and in some cases also
             quantitatively, the centrality dependence of the measured
             correlators. These observations suggest that both the
             fluctuations in the initial geometry and the nonlinear
             mixing between different harmonics in the final state are
             important for creating these correlations in momentum
             space.},
   Doi = {10.1103/PhysRevC.90.024905},
   Key = {fds310512}
}

@article{fds225676,
   Author = {CDF collaboration},
   Title = {Measurement of B Baryon Properties},
   Journal = {Phys Rev D.89 072014},
   Year = {2014},
   Month = {August},
   Key = {fds225676}
}

@article{fds321458,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for new particles in events with one lepton and
             missing transverse momentum in pp collisions at √s = 8 TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Pages = {1-42},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)037},
   Abstract = {This paper presents a search for new particles in events
             with one lepton (electron or muon) and missing transverse
             momentum using 20.3 fb−1 of proton-proton collision data
             at √s = 8 TeV recorded by the ATLAS experiment at the
             Large Hadron Collider. No significant excess beyond Standard
             Model expectations is observed. A W ′ with Sequential
             Standard Model couplings is excluded at the 95% confidence
             level for masses up to 3.24 TeV. Excited chiral bosons (W*)
             with equivalent coupling strengths are excluded for masses
             up to 3.21 TeV. In the framework of an effective field
             theory limits are also set on the dark matter-nucleon
             scattering cross-section as well as the mass scale M* of the
             unknown mediating interaction for dark matter pair
             production in association with a leptonically decaying
             W.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP09(2014)037},
   Key = {fds321458}
}

@article{fds321459,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the Z/γ* boson transverse
             momentum distribution in pp collisions at √s = 7 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)145},
   Abstract = {This paper describes a measurement of the Z/γ* boson
             transverse momentum spectrum using ATLAS proton-proton
             collision data at a centre-of-mass energy of (Formula
             presented) TeV at the LHC. The measurement is performed in
             the Z/γ* → e+e− and Z/γ* → μ+μ− channels, using
             data corresponding to an integrated luminosity of 4.7
             fb−1. Normalized differential cross sections as a function
             of the Z/γ* boson transverse momentum are measured for
             transverse momenta up to 800 GeV. The measurement is
             performed inclusively for Z/γ* rapidities up to 2.4, as
             well as in three rapidity bins. The channel results are
             combined, compared to perturbative and resummed QCD
             calculations and used to constrain the parton shower
             parameters of Monte Carlo generators.},
   Doi = {10.1007/JHEP09(2014)145},
   Key = {fds321459}
}

@article{fds310501,
   Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyka, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
             C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Amor Dos
             Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
             XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araquea, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
             M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {A neural network clustering algorithm for the ATLAS silicon
             pixel detector},
   Journal = {Journal of Instrumentation},
   Volume = {9},
   Number = {9},
   Pages = {P09009-P09009},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1088/1748-0221/9/09/P09009},
   Abstract = {A novel technique to identify and split clusters created by
             multiple charged particles in the ATLAS pixel detector using
             a set of artificial neural networks is presented. Such
             merged clusters are a common feature of tracks originating
             from highly energetic objects, such as jets. Neural networks
             are trained using Monte Carlo samples produced with a
             detailed detector simulation. This technique replaces the
             former clustering approach based on a connected component
             analysis and charge interpolation. The performance of the
             neural network splitting technique is quantified using data
             from proton-proton collisions at the LHC collected by the
             ATLAS detector in 2011 and from Monte Carlo simulations.
             This technique reduces the number of clusters shared between
             tracks in highly energetic jets by up to a factor of three.
             It also provides more precise position and error estimates
             of the clusters in both the transverse and longitudinal
             impact parameter resolution.},
   Doi = {10.1088/1748-0221/9/09/P09009},
   Key = {fds310501}
}

@article{fds310505,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for direct pair production of the top squark in
             all-hadronic final states in proton-proton collisions at
             √s = 8TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Pages = {1-51},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)015},
   Abstract = {The results of a search for direct pair production of the
             scalar partner to the top quark using an integrated
             luminosity of 20.1 fb-1 of proton-proton collision data at
             yfs = 8 TeV recorded with the ATLAS detector at the LHC are
             reported. The top squark is assumed to decay via t → t
             χ¯01 or t → b χ1 → bW(*)χ-01, where χ-01 (x1)
             denotes the lightest neutralino (chargino) in supersymmetric
             models. The search targets a fully-hadronic final state in
             events with four or more jets and large missing transverse
             momentum. No significant excess over the Standard Model
             background prediction is observed, and exclusion limits are
             reported in terms of the top squark and neutralino masses
             and as a function of the branching fraction of t → t
             χ-01. For a branching fraction of 100%, top squark masses
             in the range 270-645 GeV are excluded for χ-01 masses below
             30GeV. For a branching fraction of 50% to either t → t
             χ-01 or t → b χ-01, and assuming the χ¯1 mass to be
             twice the χ-01 mass, top squark masses in the range 250-550
             GeV are excluded for χ-01 masses below 60
             GeV.},
   Doi = {10.1007/JHEP09(2014)015},
   Key = {fds310505}
}

@article{fds310504,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for supersymmetry in events with four or more leptons
             in √s =8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052001},
   Abstract = {Results from a search for supersymmetry in events with four
             or more leptons including electrons, muons and taus are
             presented. The analysis uses a data sample corresponding to
             20.3 fb-1 of proton-proton collisions delivered by the Large
             Hadron Collider at s=8 TeV and recorded by the ATLAS
             detector. Signal regions are designed to target
             supersymmetric scenarios that can be either enriched in or
             depleted of events involving the production of a Z boson. No
             significant deviations are observed in data from standard
             model predictions and results are used to set upper limits
             on the event yields from processes beyond the standard
             model. Exclusion limits at the 95% confidence level on the
             masses of relevant supersymmetric particles are obtained. In
             R-parity-violating simplified models with decays of the
             lightest supersymmetric particle to electrons and muons,
             limits of 1350 and 750 GeV are placed on gluino and chargino
             masses, respectively. In R-parity-conserving simplified
             models with heavy neutralinos decaying to a massless
             lightest supersymmetric particle, heavy neutralino masses up
             to 620 GeV are excluded. Limits are also placed on other
             supersymmetric scenarios.},
   Doi = {10.1103/PhysRevD.90.052001},
   Key = {fds310504}
}

@article{fds310503,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abidi, SH and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the Higgs boson mass from the H → γγ and
             H → ZZ- 4ℓ channels inpp collisions at
             center-of-mass energies of 7 and 8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052004},
   Abstract = {An improved measurement of the mass of the Higgs boson is
             derived from a combined fit to the reconstructed invariant
             mass spectra of the decay channels H → γγ and H →
             ZZ∗→ 4ℓ. The analysis uses the pp collision data
             sample recorded by the ATLAS experiment at the CERN Large
             Hadron Collider at center-of-mass energies of 7 TeV and 8
             TeV, corresponding to an integrated luminosity of 25 fb-1.
             The measured value of the Higgs boson mass is mH= 125.36 ±
             0.37(stat) ± 0.18(syst) GeV. This result is based on
             improved energy-scale calibrations for photons, electrons,
             and muons as well as other analysis improvements, and
             supersedes the previous result from ATLAS. Upper limits on
             the total width of the Higgs boson are derived from fits to
             the invariant mass spectra of the H → γγ and H →
             ZZ∗→ 4ℓ decay channels.},
   Doi = {10.1103/PhysRevD.90.052004},
   Key = {fds310503}
}

@article{fds313375,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurements of fiducial and differential cross sections for
             Higgs boson production in the diphoton decay channel at √s
             = 8 TeV with ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Pages = {1-60},
   Year = {2014},
   Month = {September},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)112},
   Abstract = {Measurements of fiducial and differential cross sections are
             presented for Higgs boson production in proton-proton
             collisions at a centre-of-mass energy of √s = 8TeV. The
             analysis is performed in the H → γγ decay channel using
             20.3 fb−1 of data recorded by the ATLAS experiment at the
             CERN Large Hadron Collider. The signal is extracted using a
             fit to the diphoton invariant mass spectrum assuming that
             the width of the resonance is much smaller than the
             experimental resolution. The signal yields are corrected for
             the effects of detector inefficiency and resolution. The pp
             → H → γγ fiducial cross section is measured to be 43.2
             ±9.4 (stat.) +3.2−2.9 (syst.) ±1.2 (lumi) fb for a Higgs
             boson of mass 125.4 GeV decaying to two isolated photons
             that have transverse momentum greater than 35% and 25% of
             the diphoton invariant mass and each with absolute
             pseudorapidity less than 2.37. Four additional fiducial
             cross sections and two cross-section limits are presented in
             phase space regions that test the theoretical modelling of
             different Higgs boson production mechanisms, or are
             sensitive to physics beyond the Standard Model. Differential
             cross sections are also presented, as a function of
             variables related to the diphoton kinematics and the jet
             activity produced in the Higgs boson events. The observed
             spectra are statistically limited but broadly in line with
             the theoretical expectations.},
   Doi = {10.1007/JHEP09(2014)112},
   Key = {fds313375}
}

@article{fds310506,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allen, K and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
             Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ and Arnaez, O},
   Title = {Search for high-mass dilepton resonances in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052005},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for high-mass resonances decaying to dielectron or
             dimuon final states. Results are presented from an analysis
             of proton-proton (pp) collisions at a center-of-mass energy
             of 8 TeV corresponding to an integrated luminosity of 20.3
             fb-1 in the dimuon channel. A narrow resonance with Standard
             Model Z couplings to fermions is excluded at 95% confidence
             level for masses less than 2.79 TeV in the dielectron
             channel, 2.53 TeV in the dimuon channel, and 2.90 TeV in the
             two channels combined. Limits on other model interpretations
             are also presented, including a grand-unification model
             based on the E6 gauge group, Z∗ bosons, minimal Z′
             models, a spin-2 graviton excitation from Randall-Sundrum
             models, quantum black holes, and a minimal walking
             technicolor model with a composite Higgs
             boson.},
   Doi = {10.1103/PhysRevD.90.052005},
   Key = {fds310506}
}

@article{fds310502,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
             M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
             L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
             AJ},
   Title = {Flavor tagged time-dependent angular analysis of the Bs0
             →J/ψφ decay and extraction of ΔΓs and the weak phase
             φs in ATLAS},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052007},
   Abstract = {A measurement of the Bs0→J/ψφ decay parameters, updated
             to include flavor tagging is reported using 4.9fb-1 of
             integrated luminosity collected by the ATLAS detector from
             s=7TeV pp collisions recorded in 2011 at the LHC. The values
             measured for the physical parameters are
             φs=0.12±0.25(stat)±0.05(syst)radΔΓs=0.053±0.021(stat)±0.010(syst)ps-1Γs=0.677±0.007(stat)±0.004(syst)ps-1|A
             (0)|2=0.220±0.008(stat)±0.009(syst)|A0(0)|2=0.529±0.006(stat)±0.012(syst)δ=3.89±0.47(stat)±0.11(syst)radwhere
             the parameter ΔΓs is constrained to be positive. The
             S-wave contribution was measured and found to be compatible
             with zero. Results for φs and ΔΓs are also presented as
             68% and 95% likelihood contours, which show agreement with
             the Standard Model expectations.},
   Doi = {10.1103/PhysRevD.90.052007},
   Key = {fds310502}
}

@article{fds310507,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for pair-produced third-generation squarks decaying
             via charm quarks or in compressed supersymmetric scenarios
             in pp collisions at √s =8TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.052008},
   Abstract = {Results of a search for supersymmetry via direct production
             of third-generation squarks are reported, using 20.3fb-1 of
             proton-proton collision data at s=8TeV recorded by the ATLAS
             experiment at the LHC in 2012. Two different analysis
             strategies based on monojetlike and c-tagged event
             selections are carried out to optimize the sensitivity for
             direct top squark-pair production in the decay channel to a
             charm quark and the lightest neutralino (t∼1→c+χ∼10)
             across the top squark-neutralino mass parameter space. No
             excess above the Standard Model background expectation is
             observed. The results are interpreted in the context of
             direct pair production of top squarks and presented in terms
             of exclusion limits in the (mt∼1, mχ∼10) parameter
             space. A top squark of mass up to about 240 GeV is excluded
             at 95% confidence level for arbitrary neutralino masses,
             within the kinematic boundaries. Top squark masses up to 270
             GeV are excluded for a neutralino mass of 200 GeV. In a
             scenario where the top squark and the lightest neutralino
             are nearly degenerate in mass, top squark masses up to 260
             GeV are excluded. The results from the monojetlike analysis
             are also interpreted in terms of compressed scenarios for
             top squark-pair production in the decay channel
             t∼1→b+ff′+χ∼10 and sbottom pair production with
             b∼1→b+χ∼10, leading to a similar exclusion for nearly
             mass-degenerate third-generation squarks and the lightest
             neutralino. The results in this paper significantly extend
             previous results at colliders.},
   Doi = {10.1103/PhysRevD.90.052008},
   Key = {fds310507}
}

@article{fds225672,
   Author = {ATLAS collaboration},
   Title = {Measurement of the Higgs boson mass from the $H → γ γ$
             and $H → ZZ^{*} → 4 \ell$ channels with the ATLAS
             detector at the LHC},
   Journal = {Phys Rev D.90 052004},
   Year = {2014},
   Month = {September},
   Key = {fds225672}
}

@article{fds225673,
   Author = {ATLAS collaboration},
   Title = {Search for the Standard Model Higgs boson decay to mu+mu-
             with the ATLAS detector},
   Journal = {Physics Letters B 738, 68-86},
   Year = {2014},
   Month = {September},
   Key = {fds225673}
}

@article{fds310510,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for squarks and gluinos with the ATLAS detector in
             final states with jets and missing transverse momentum using
             √s = 8 TeV proton-proton collision data},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2014)176},
   Abstract = {A search for squarks and gluinos in final states containing
             high-pTjets, missing transverse momentum and no electrons or
             muons is presented. The data were recorded in 2012 by the
             ATLAS experiment in √s = 8TeV proton-proton collisions at
             the Large Hadron Collider, with a total integrated
             luminosity of 20.3 fb−1. Results are interpreted in a
             variety of simplified and specific supersymmetry-breaking
             models assuming that R-parity is conserved and that the
             lightest neutralino is the lightest supersymmetric particle.
             An exclusion limit at the 95% confidence level on the mass
             of the gluino is set at 1330GeV for a simplified model
             incorporating only a gluino and the lightest neutralino. For
             a simplified model involving the strong production of first-
             and second-generation squarks, squark masses below 850GeV
             (440GeV) are excluded for a massless lightest neutralino,
             assuming mass degenerate (single light-flavour) squarks. In
             mSUGRA/CMSSM models with tan β = 30, A0= −2m0and μ > 0,
             squarks and gluinos of equal mass are excluded for masses
             below 1700GeV. Additional limits are set for non-universal
             Higgs mass models with gaugino mediation and for simplified
             models involving the pair production of gluinos, each
             decaying to a top squark and a top quark, with the top
             squark decaying to a charm quark and a neutralino. These
             limits extend the region of supersymmetric parameter space
             excluded by previous searches with the ATLAS
             detector.},
   Doi = {10.1007/JHEP09(2014)176},
   Key = {fds310510}
}

@article{fds310494,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Search for scalar diphoton resonances in the mass range
             65-600 GeV with the ATLAS detector in pp collision data at
             √s=8 TeV.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {17},
   Pages = {171801},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.113.171801},
   Abstract = {A search for scalar particles decaying via narrow resonances
             into two photons in the mass range 65-600 GeV is performed
             using 20.3  fb(-1) of √s 8 TeV pp collision data
             collected with the ATLAS detector at the Large Hadron
             Collider. The recently discovered Higgs boson is treated as
             a background. No significant evidence for an additional
             signal is observed. The results are presented as limits at
             the 95% confidence level on the production cross section of
             a scalar boson times branching ratio into two photons, in a
             fiducial volume where the reconstruction efficiency is
             approximately independent of the event topology. The upper
             limits set extend over a considerably wider mass range than
             previous searches.},
   Doi = {10.1103/physrevlett.113.171801},
   Key = {fds310494}
}

@article{fds310496,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker,
             S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
             E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch,
             A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y},
   Title = {Evidence for electroweak production of W±W±jj in pp
             collisions at sqrt[s] = 8 TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {14},
   Pages = {141803},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/physrevlett.113.141803},
   Abstract = {This Letter presents the first study of W(±)W(±)jj,
             same-electric-charge diboson production in association with
             two jets, using 20.3 fb(-1) of proton-proton collision data
             at sqrt[s] = 8  TeV recorded by the ATLAS detector at
             the Large Hadron Collider. Events with two reconstructed
             same-charge leptons (e(±)e(±), e(±)μ(±), and
             μ(±)μ(±)) and two or more jets are analyzed. Production
             cross sections are measured in two fiducial regions, with
             different sensitivities to the electroweak and strong
             production mechanisms. First evidence for W(±)W(±)jj
             production and electroweak-only W(±)W(±)jj production is
             observed with a significance of 4.5 and 3.6 standard
             deviations, respectively. The measured production cross
             sections are in agreement with standard model predictions.
             Limits at 95% confidence level are set on anomalous quartic
             gauge couplings.},
   Doi = {10.1103/physrevlett.113.141803},
   Key = {fds310496}
}

@article{fds310495,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for WZ resonances in the fully leptonic channel using
             pp collisions at s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {737},
   Pages = {223-243},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.08.039},
   Abstract = {A search for resonant WZ production in the ℓνℓ'ℓ'
             (ℓ,ℓ'=e,μ) decay channel using 20.3 fb-1 of s=8TeV pp
             collision data collected by the ATLAS experiment at LHC is
             presented. No significant deviation from the Standard Model
             prediction is observed and upper limits on the production
             cross sections of WZ resonances from an extended gauge model
             W' and from a simplified model of heavy vector triplets are
             derived. A corresponding observed (expected) lower mass
             limit of 1.52 (1.49) TeV is derived for the W' at the 95%
             confidence level. © 2014 Elsevier B.V.},
   Doi = {10.1016/j.physletb.2014.08.039},
   Key = {fds310495}
}

@article{fds310497,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of long-range pseudorapidity correlations and
             azimuthal harmonics in √sNN =5.02 TeV
             proton-lead collisions with the ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {90},
   Number = {4},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevC.90.044906},
   Abstract = {Measurements of two-particle correlation functions and the
             first five azimuthal harmonics, v1 to v5, are presented,
             using 28 nb-1 of p+Pb collisions at a nucleon-nucleon
             center-of-mass energy of √sNN=5.02 TeV measured with the
             ATLAS detector at the LHC. Significant long-range
             "ridgelike" correlations are observed for pairs with small
             (|Δϕ|<π/3) and back-to-back pairs (|Δφ|>2π/3) over the
             transverse momentum range 0.4<pT<12 GeV and in different
             intervals of event activity. The event activity is defined
             by either the number of reconstructed tracks or the total
             transverse energy on the Pb-fragmentation side. The
             azimuthal structure of such long-range correlations is
             Fourier decomposed to obtain the harmonics νn as a function
             of pT and event activity. The extracted νn values for n=2
             to 5 decrease with n. The ν2 and ν3 values are found to be
             positive in the measured pT range. The ν1 is also measured
             as a function of pT and is observed to change sign around
             pT≈1.5-2.0 GeV and then increase to about 0.1 for pT>4
             GeV. The ν2 (pT), ν3 (pT), and ν4 (pT) are compared to
             the νn coefficients in Pb+Pb collisions at √sNN=2.76 TeV
             with similar event multiplicities. Reasonable agreement is
             observed after accounting for the difference in the average
             pT of particles produced in the two collision
             systems.},
   Doi = {10.1103/PhysRevC.90.044906},
   Key = {fds310497}
}

@article{fds310500,
   Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Electron and photon energy calibration with the ATLAS
             detector using LHC Run 1 data},
   Journal = {European Physical Journal C},
   Volume = {74},
   Number = {10},
   Pages = {1-48},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3071-4},
   Abstract = {This paper presents the electron and photon energy
             calibration achieved with the ATLAS detector using about
             25 fb-1 of LHC proton–proton collision data taken at
             centre-of-mass energies of (Equation Present) and 8 TeV.
             The reconstruction of electron and photon energies is
             optimised using multivariate algorithms. The response of the
             calorimeter layers is equalised in data and simulation, and
             the longitudinal profile of the electromagnetic showers is
             exploited to estimate the passive material in front of the
             calorimeter and reoptimise the detector simulation. After
             all corrections, the Z resonance is used to set the absolute
             energy scale. For electrons from Z decays, the achieved
             calibration is typically accurate to 0.05 % in most of the
             detector acceptance, rising to 0.2 % in regions with large
             amounts of passive material. The remaining inaccuracy is
             less than 0.2–1 % for electrons with a transverse energy
             of 10 GeV, and is on average 0.3 % for photons. The
             detector resolution is determined with a relative inaccuracy
             of less than 10 % for electrons and photons up to 60 GeV
             transverse energy, rising to 40 % for transverse energies
             above 500 GeV.},
   Doi = {10.1140/epjc/s10052-014-3071-4},
   Key = {fds310500}
}

@article{fds310498,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Djuvsland, JI and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Kucuk, H and Anisenkov,
             AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for the lepton flavor violating decay Z → eμ in pp
             collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.072010},
   Abstract = {The ATLAS detector at the Large Hadron Collider is used to
             search for the lepton flavor violating process Z → eμ in
             pp collisions using 20.3 fb-1 of data collected at √s = 8
             TeV. An enhancement in the eμ invariant mass spectrum is
             searched for at the Z-boson mass. The number of Z bosons
             produced in the data sample is estimated using events of
             similar topology, Z → ee and μμ, significantly reducing
             the systematic uncertainty in the measurement. There is no
             evidence of an enhancement at the Z-boson mass, resulting in
             an upper limit on the branching fraction, B(Z → 7.5 ×
             10.7 at the 95% confidence level.},
   Doi = {10.1103/PhysRevD.90.072010},
   Key = {fds310498}
}

@article{fds310486,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
             M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
             V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
             A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
   Title = {Observation of an excited Bc(±) meson state with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {21},
   Pages = {212004},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1103/physrevlett.113.212004},
   Abstract = {A search for excited states of the Bc(±) meson is performed
             using 4.9  fb(-1) of 7 TeV and 19.2  fb(-1) of 8 TeV
             pp collision data collected by the ATLAS experiment at the
             LHC. A new state is observed through its hadronic transition
             to the ground state, with the latter detected in the decay
             Bc(±)→J/ψπ(±). The state appears in the
             m(Bc(±)π(+)π(-))-m(Bc(±))-2m(π(±)) mass difference
             distribution with a significance of 5.2 standard deviations.
             The mass of the observed state is 6842±4±5  MeV, where
             the first error is statistical and the second is systematic.
             The mass and decay of this state are consistent with
             expectations for the second S-wave state of the Bc(±)
             meson, Bc(±)(2S).},
   Doi = {10.1103/physrevlett.113.212004},
   Key = {fds310486}
}

@article{fds310492,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for top squark pair production in final states with
             one isolated lepton, jets, and missing transverse momentum
             in √ s = 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)118},
   Abstract = {The results of a search for top squark (stop) pair
             production in final states with one isolated lepton, jets,
             and missing transverse momentum are reported. The analysis
             is performed with proton-proton collision data at (Formula
             presented.) = 8 TeV collected with the ATLAS detector at the
             LHC in 2012 corresponding to an integrated luminosity of 20
             fb−1. The lightest supersymmetric particle (LSP) is taken
             to be the lightest neutralino which only interacts weakly
             and is assumed to be stable. The stop decay modes considered
             are those to a top quark and the LSP as well as to a bottom
             quark and the lightest chargino, where the chargino decays
             to the LSP by emitting a W boson. A wide range of scenarios
             with different mass splittings between the stop, the
             lightest neutralino and the lightest chargino are
             considered, including cases where the W bosons or the top
             quarks are off-shell. Decay modes involving the heavier
             charginos and neutralinos are addressed using a set of
             phenomenological models of supersymmetry. No significant
             excess over the Standard Model prediction is observed. A
             stop with a mass between 210 and 640 GeV decaying directly
             to a top quark and a massless LSP is excluded at 95%
             confidence level, and in models where the mass of the
             lightest chargino is twice that of the LSP, stops are
             excluded at 95% confidence level up to a mass of 500 GeV for
             an LSP mass in the range of 100 to 150 GeV. Stringent
             exclusion limits are also derived for all other stop decay
             modes considered, and model-independent upper limits are set
             on the visible cross-section for processes beyond the
             Standard Model.},
   Doi = {10.1007/JHEP11(2014)118},
   Key = {fds310492}
}

@article{fds310487,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
             VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of the cross-section of high transverse momentum
             vector bosons reconstructed as single jets and studies of
             jet substructure in pp collisions at √s = 7 TeV with the
             ATLAS detector},
   Journal = {New Journal of Physics},
   Volume = {16},
   Number = {11},
   Pages = {113013-113013},
   Publisher = {IOP Publishing},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1367-2630/16/11/113013},
   Abstract = {This paper presents a measurement of the cross-section for
             high transverse momentum W and Z bosons produced in pp
             collisions and decaying to all-hadronic final states. The
             data used in the analysis were recorded by the ATLAS
             detector at the CERN Large Hadron Collider at a
             centre-of-mass energy of and correspond to an integrated
             luminosity of . The measurement is performed by
             reconstructing the boosted W or Z bosons in single jets. The
             reconstructed jet mass is used to identify the W and Z
             bosons, and a jet substructure method based on energy
             cluster information in the jet centre-of-mass frame is used
             to suppress the large multi-jet background. The
             cross-section for events with a hadronically decaying W or Z
             boson, with transverse momentum and pseudorapidity , is
             measured to be pb and is compared to next-to-leading-order
             calculations. The selected events are further used to study
             jet grooming techniques.},
   Doi = {10.1088/1367-2630/16/11/113013},
   Key = {fds310487}
}

@article{fds321460,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of the cross section of high transverse momentum
             Z→bb¯ production in proton–proton collisions at √s=8
             TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Pages = {25-43},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.09.020},
   Abstract = {This Letter reports the observation of a high transverse
             momentum Z→bb¯ signal in proton–proton collisions at
             s=8 TeV and the measurement of its production cross section.
             The data analysed were collected in 2012 with the ATLAS
             detector at the LHC and correspond to an integrated
             luminosity of 19.5 fb−1. The Z→bb¯ decay is
             reconstructed from a pair of b-tagged jets, clustered with
             the anti-kt jet algorithm with R=0.4, that have low angular
             separation and form a dijet with pT>200 GeV. The signal
             yield is extracted from a fit to the dijet invariant mass
             distribution, with the dominant, multi-jet background mass
             shape estimated by employing a fully data-driven technique
             that reduces the dependence of the analysis on simulation.
             The fiducial cross section is determined to be
             σZ→bb¯fid=2.02±0.20 (stat.) ±0.25 (syst.)±0.06
             (lumi.) pb=2.02 ±0.33 pb, in good agreement with
             next-to-leading-order theoretical predictions.},
   Doi = {10.1016/j.physletb.2014.09.020},
   Key = {fds321460}
}

@article{fds310527,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for the Standard Model Higgs boson decay to
             μ+μ with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Number = {1},
   Pages = {68-86},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.09.008},
   Abstract = {A search is reported for Higgs boson decay to μ+μ− using
             data with an integrated luminosity of 24.8 fb−1collected
             with the ATLAS detector in pp collisions at s=7and8 TeV at
             the CERN Large Hadron Collider. The observed dimuon
             invariant mass distribution is consistent with the Standard
             Model background-only hypothesis in the 120–150 GeV search
             range. For a Higgs boson with a mass of 125.5 GeV, the
             observed (expected) upper limit at the 95% confidence level
             is 7.0 (7.2) times the Standard Model expectation. This
             corresponds to an upper limit on the branching ratio
             BR(H→μ+μ−) of 1.5×10−3.},
   Doi = {10.1016/j.physletb.2014.09.008},
   Key = {fds310527}
}

@article{fds310488,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for new resonances in Wγ and Zγ final states in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {738},
   Pages = {428-447},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.10.002},
   Abstract = {This letter presents a search for new resonances decaying to
             final states with a vector boson produced in association
             with a high transverse momentum photon, Vγ with
             V=W(→ℓν) or Z(→ℓ+ℓ−), where ℓ=e or μ. The
             measurements use 20.3 fb−1 of proton–proton collision
             data at a center–of–mass energy of s=8 TeV recorded with
             the ATLAS detector. No deviations from the Standard Model
             expectations are found, and production cross section limits
             are set at 95% confidence level. Masses of the hypothetical
             aT and ωT states of a benchmark Low Scale Technicolor model
             are excluded in the ranges [275,960] GeV and
             [200,700]∪[750,890] GeV, respectively. Limits at 95%
             confidence level on the production cross section of a
             singlet scalar resonance decaying to Zγ final states have
             also been obtained for masses below 1180
             GeV.},
   Doi = {10.1016/j.physletb.2014.10.002},
   Key = {fds310488}
}

@article{fds310490,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for neutral Higgs bosons of the minimal
             supersymmetric standard model in pp collisions at vs= 8TeV
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Pages = {1-47},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)056},
   Abstract = {Abstract: A search for the neutral Higgs bosons predicted by
             the Minimal Supersymmetric Standard Model (MSSM) is
             reported. The analysis is performed on data from
             proton-proton collisions at a centre-of-mass energy of 8 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider. The samples used for this search were collected in
             2012 and correspond to integrated luminosities in the range
             19.5-20.3 fb−1. The MSSM Higgs bosons are searched for in
             the τ τ final state. No significant excess over the
             expected background is observed, and exclusion limits are
             derived for the production cross section times branching
             fraction of a scalar particle as a function of its mass. The
             results are also interpreted in the MSSM parameter space for
             various benchmark scenarios.},
   Doi = {10.1007/JHEP11(2014)056},
   Key = {fds310490}
}

@article{fds310493,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the top-quark mass in the all-hadronic
             channel using the full CDF data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.091101},
   Abstract = {The top-quark mass Mtop is measured using top
             quark-antiquark pairs produced in proton-antiproton
             collisions at a center-of-mass energy of 1.96 TeV and that
             decay into a fully hadronic final state. The full data set
             collected with the CDF II detector at the Fermilab Tevatron
             Collider, corresponding to an integrated luminosity of
             9.3fb-1, is used. Events are selected that have six to eight
             jets, at least one of which is identified as having
             originated from a b quark. In addition, a multivariate
             algorithm, containing multiple kinematic variables as
             inputs, is used to discriminate signal events from
             background events due to QCD multijet production. Templates
             for the reconstructed top-quark mass are combined in a
             likelihood fit to measure Mtop with a simultaneous
             calibration of the jet energy scale. A value of
             Mtop=175.07±1.19(stat)-1.58+1.55(syst)GeV/c2 is obtained
             for the top-quark mass.},
   Doi = {10.1103/PhysRevD.90.091101},
   Key = {fds310493}
}

@article{fds310489,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for pair and single production of new heavy quarks
             that decay to a Z boson and a third-generation quark in pp
             collisions at √ S = 8TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2014},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2014},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2014)104},
   Abstract = {Abstract: A search is presented for the production of new
             heavy quarks that decay to a Z boson and a third-generation
             Standard Model quark. In the case of a new charge +2/3 quark
             (T ), the decay targeted is T → Zt, while the decay
             targeted for a new charge −1/3 quark (B) is B → Zb. The
             search is performed with a dataset corresponding to 20.3
             fb−1 of pp collisions at (Formula presented.) TeV recorded
             in 2012 with the ATLAS detector at the CERN Large Hadron
             Collider. Selected events contain a high transverse momentum
             Z boson candidate reconstructed from a pair of oppositely
             charged same-flavor leptons (electrons or muons), and are
             analyzed in two channels defined by the absence or presence
             of a third lepton. Hadronic jets, in particular those with
             properties consistent with the decay of a b-hadron, are also
             required to be present in selected events. Different
             requirements are made on the jet activity in the event in
             order to enhance the sensitivity to either heavy quark pair
             production mediated by the strong interaction, or single
             production mediated by the electroweak interaction. No
             significant excess of events above the Standard Model
             expectation is observed, and lower limits are derived on the
             mass of vector-like T and B quarks under various branching
             ratio hypotheses, as well as upper limits on the magnitude
             of electroweak coupling parameters.},
   Doi = {10.1007/JHEP11(2014)104},
   Key = {fds310489}
}

@article{fds313374,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
             N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
             SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hirschbuehl, D and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
             P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
             CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
             P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
             I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
             Collaboration},
   Title = {Measurement of the single top quark production cross section
             and |Vtb| in events with one charged lepton, large missing
             transverse energy, and jets at CDF.},
   Journal = {Physical review letters},
   Volume = {113},
   Number = {26},
   Pages = {261804},
   Year = {2014},
   Month = {December},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.113.261804},
   Abstract = {We report a measurement of single top quark production in
             proton-antiproton collisions at a center-of-mass energy of
             sqrt[s]=1.96  TeV using a data set corresponding to
             7.5  fb(-1) of integrated luminosity collected by the
             Collider Detector at Fermilab. We select events consistent
             with the single top quark decay process t→Wb→ℓνb by
             requiring the presence of an electron or muon, a large
             imbalance of transverse momentum indicating the presence of
             a neutrino, and two or three jets including at least one
             originating from a bottom quark. An artificial neural
             network is used to discriminate the signal from backgrounds.
             We measure a single top quark production cross section of
             3.04(-0.53)(+0.57)  pb and set a lower limit on the
             magnitude of the coupling between the top quark and bottom
             quark |Vtb|>0.78 at the 95% credibility level.},
   Doi = {10.1103/physrevlett.113.261804},
   Key = {fds313374}
}

@article{fds310480,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amaral
             Coutinho, Y and Amelung, C and Amor Dos Santos and SP and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
             Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
             A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B},
   Title = {ATLAS Collaboration},
   Journal = {Nuclear Physics A},
   Volume = {932},
   Pages = {572-594},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1016/S0375-9474(14)00601-0},
   Doi = {10.1016/S0375-9474(14)00601-0},
   Key = {fds310480}
}

@article{fds336464,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of the total cross section from elastic
             scattering in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {Nuclear Physics B},
   Volume = {889},
   Pages = {486-548},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2014.10.019},
   Abstract = {A measurement of the total pp cross section at the LHC at
             s=7 TeV is presented. In a special run with high-β⋆ beam
             optics, an integrated luminosity of 80 μb−1 was
             accumulated in order to measure the differential elastic
             cross section as a function of the Mandelstam momentum
             transfer variable t. The measurement is performed with the
             ALFA sub-detector of ATLAS. Using a fit to the differential
             elastic cross section in the |t| range from 0.01 GeV2 to 0.1
             GeV2 to extrapolate to |t|→0, the total cross section,
             σtot(pp→X), is measured via the optical theorem to be:
             σtot(pp→X)=95.35±0.38(stat.)±1.25(exp.)±0.37(extr.)mb,
             where the first error is statistical, the second accounts
             for all experimental systematic uncertainties and the last
             is related to uncertainties in the extrapolation to |t|→0.
             In addition, the slope of the elastic cross section at small
             |t| is determined to be B=19.73±0.14(stat.)±0.26(syst.)
             GeV−2.},
   Doi = {10.1016/j.nuclphysb.2014.10.019},
   Key = {fds336464}
}

@article{fds310481,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Comprehensive measurements of t-channel single top-quark
             production cross sections at √s=7 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112006},
   Abstract = {This article presents measurements of the t-channel single
             top-quark (t) and top-antiquark (t¯) total production cross
             sections σ(tq) and σ(t¯q), their ratio
             Rt=σ(tq)/σ(t¯q), and a measurement of the inclusive
             production cross section σ(tq+t¯q) in proton-proton
             collisions at √s=7 TeV at the LHC. Differential cross
             sections for the tq and t¯q processes are measured as a
             function of the transverse momentum and the absolute value
             of the rapidity of t and t¯, respectively. The analyzed
             data set was recorded with the ATLAS detector and
             corresponds to an integrated luminosity of 4.59 fb-1.
             Selected events contain one charged lepton, large missing
             transverse momentum, and two or three jets. The cross
             sections are measured by performing a binned
             maximum-likelihood fit to the output distributions of neural
             networks. The resulting measurements are
             σ(tq)=46±1(stat)±6(syst) pb, σ(t¯q)=23±1(stat)±3(syst)
             pb, Rt=2.04±0.13(stat)±0.12(syst), and
             σ(tq+t¯q)=68±2(stat)±8(syst) pb, consistent with the
             Standard Model expectation. The uncertainty on the measured
             cross sections is dominated by systematic uncertainties,
             while the uncertainty on Rt is mainly statistical. Using the
             ratio of σ(tq+t¯q) to its theoretical prediction, and
             assuming that the top-quark-related CKM matrix elements obey
             the relation |Vtb||Vts|,|Vtd|, we determine
             |Vtb|=1.02±0.07.},
   Doi = {10.1103/PhysRevD.90.112006},
   Key = {fds310481}
}

@article{fds332377,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurement of inclusive jet charged-particle fragmentation
             functions in Pb+Pb collisions at √sNN=2.76 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {739},
   Pages = {320-342},
   Publisher = {Elsevier BV},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.10.065},
   Abstract = {Measurements of charged-particle fragmentation functions of
             jets produced in ultra-relativistic nuclear collisions can
             provide insight into the modification of parton showers in
             the hot, dense medium created in the collisions. ATLAS has
             measured jets in sNN=2.76 TeV Pb+Pb collisions at the LHC
             using a data set recorded in 2011 with an integrated
             luminosity of 0.14 nb−1. Jets were reconstructed using the
             anti-kt algorithm with distance parameter values
             R=0.2,0.3,and 0.4. Distributions of charged-particle
             transverse momentum and longitudinal momentum fraction are
             reported for seven bins in collision centrality for R=0.4
             jets with pTjet>100 GeV. Commensurate minimum pT values are
             used for the other radii. Ratios of fragment distributions
             in each centrality bin to those measured in the most
             peripheral bin are presented. These ratios show a reduction
             of fragment yield in central collisions relative to
             peripheral collisions at intermediate z values,
             0.04≲z≲0.2, and an enhancement in fragment yield for
             z≲0.04. A smaller, less significant enhancement is
             observed at large z and large pT in central
             collisions.},
   Doi = {10.1016/j.physletb.2014.10.065},
   Key = {fds332377}
}

@article{fds310483,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Measurements of spin correlation in top-antitop quark events
             from proton-proton collisions at √s =7 TeV using the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112016},
   Abstract = {Measurements of spin correlation in top quark pair
             production are presented using data collected with the ATLAS
             detector at the LHC with proton-proton collisions at a
             center-of-mass energy of 7 TeV, corresponding to an
             integrated luminosity of 4.6 fb-1. Events are selected in
             final states with two charged leptons and at least two jets
             and in final states with one charged lepton and at least
             four jets. Four different observables sensitive to different
             properties of the top quark pair production mechanism are
             used to extract the correlation between the top and antitop
             quark spins. Some of these observables are measured for the
             first time. The measurements are in good agreement with the
             Standard Model prediction at next-to-leading-order
             accuracy.},
   Doi = {10.1103/PhysRevD.90.112016},
   Key = {fds310483}
}

@article{fds310484,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Measurement of Higgs boson production in the diphoton decay
             channel in pp collisions at center-of-mass energies of 7 and
             8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112015},
   Abstract = {A measurement of the production processes of the recently
             discovered Higgs boson is performed in the two-photon final
             state using 4.5 fb-1of proton-proton collisions data at √s
             = 7 TeV and 20.3 fb-1at √s = 8 TeV collected by the ATLAS
             detector at the Large Hadron Collider. The number of
             observed Higgs boson decays to diphotons divided by the
             corresponding Standard Model prediction, called the signal
             strength, is found to be μ = 1.17 ± 0.27 at the value of
             the Higgs boson mass measured by ATLAS, mH= 125.4 GeV. The
             analysis is optimized to measure the signal strengths for
             individual Higgs boson production processes at this value of
             mH. They are found to be μggF= 1.32 ± 0.38, μVBF= 0.8 ±
             0.7, μWH= 1.0 ± 1.6, μZH= 0.1+3.7-0.1, and μtt¯H=
             1.6+2.7-1.8, for Higgs boson production through gluon
             fusion, vector-boson fusion, and in association with a W or
             Z boson or a top-quark pair, respectively. Compared with the
             previously published ATLAS analysis, the results reported
             here also benefit from a new energy calibration procedure
             for photons and the subsequent reduction of the systematic
             uncertainty on the diphoton mass resolution. No significant
             deviations from the predictions of the Standard Model are
             found.},
   Doi = {10.1103/PhysRevD.90.112015},
   Key = {fds310484}
}

@article{fds310485,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of indirect CP -violating asymmetries in D0
             →k+K- and D0 →π+π- decays at CDF},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {90},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2014},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.111103},
   Abstract = {We report a measurement of the indirect CP-violating
             asymmetries (AΓ) between effective lifetimes of anticharm
             and charm mesons reconstructed in D0→K+K- and D0→π+π-
             decays. We use the full data set of proton-antiproton
             collisions collected by the Collider Detector at Fermilab
             experiment and corresponding to 9.7fb-1 of integrated
             luminosity. The strong-interaction decay D∗+→D0π+ is
             used to identify the meson at production as D0 or D¯0. We
             statistically subtract D0 and D¯0 mesons originating from
             b-hadron decays and measure the yield asymmetry between
             anticharm and charm decays as a function of decay time. We
             measure AΓ(K+K-)=(-0.19±0.15(stat)±0.04(syst))% and
             AΓ(π+π-)=(-0.01±0.18(stat)±0.03(syst))%. The results
             are consistent with the hypothesis of CP symmetry and their
             combination yields AΓ=(-0.12±0.12)%.},
   Doi = {10.1103/PhysRevD.90.111103},
   Key = {fds310485}
}

@article{fds321455,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
             AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
             M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Bedikian, S and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
             N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
             CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet,
             D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
             R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole,
             B},
   Title = {Identification and energy calibration of hadronically
             decaying tau leptons with the ATLAS experiment in pp
             collisions at [Formula: see text][Formula: see
             text].},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {303},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3500-z},
   Abstract = {This paper describes the trigger and offline reconstruction,
             identification and energy calibration algorithms for
             hadronic decays of tau leptons employed for the data
             collected from <i>pp</i> collisions in 2012 with the ATLAS
             detector at the LHC center-of-mass energy [Formula: see
             text] [Formula: see text]. The performance of these
             algorithms is measured in most cases with [Formula: see
             text] decays to tau leptons using the full 2012 dataset,
             corresponding to an integrated luminosity of 20.3
             fb[Formula: see text]. An uncertainty on the offline
             reconstructed tau energy scale of 2-4 %, depending on
             transverse energy and pseudorapidity, is achieved using two
             independent methods. The offline tau identification
             efficiency is measured with a precision of 2.5 % for
             hadronically decaying tau leptons with one associated track,
             and of 4 % for the case of three associated tracks,
             inclusive in pseudorapidity and for a visible transverse
             energy greater than 20 [Formula: see text]. For hadronic tau
             lepton decays selected by offline algorithms, the tau
             trigger identification efficiency is measured with a
             precision of 2-8 %, depending on the transverse energy. The
             performance of the tau algorithms, both offline and at the
             trigger level, is found to be stable with respect to the
             number of concurrent proton-proton interactions and has
             supported a variety of physics results using hadronically
             decaying tau leptons at ATLAS.},
   Doi = {10.1140/epjc/s10052-015-3500-z},
   Key = {fds321455}
}

@article{fds321456,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH},
   Title = {Search for Higgs boson pair production in the [Formula: see
             text] final state from pp collisions at [Formula: see
             text] TeVwith the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {9},
   Pages = {412},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3628-x},
   Abstract = {A search for Higgs boson pair production [Formula: see text]
             is performed with 19.5 fb[Formula: see text] of
             proton-proton collision data at [Formula: see text] TeV,
             which were recorded by the ATLAS detector at the Large
             Hadron Collider in 2012. The decay products of each Higgs
             boson are reconstructed as a high-momentum [Formula: see
             text] system with either a pair of small-radius jets or a
             single large-radius jet, the latter exploiting jet
             substructure techniques and associated <i>b</i>-tagged
             track-jets. No evidence for resonant or non-resonant Higgs
             boson pair production is observed. The data are interpreted
             in the context of the Randall-Sundrum model with a warped
             extra dimension as well as the two-Higgs-doublet model. An
             upper limit on the cross-section for [Formula: see text] of
             3.2 (2.3) fb is set for a Kaluza-Klein graviton [Formula:
             see text] mass of 1.0 (1.5) TeV, at the 95 % confidence
             level. The search for non-resonant Standard Model <i>hh</i>
             production sets an observed 95 % confidence level upper
             limit on the production cross-section [Formula: see text] of
             202 fb, compared to a Standard Model prediction of
             [Formula: see text] fb.},
   Doi = {10.1140/epjc/s10052-015-3628-x},
   Key = {fds321456}
}

@article{fds321457,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Search for metastable heavy charged particles with large
             ionisation energy loss in pp collisions at [Formula:
             see text] TeV using the ATLAS experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {9},
   Pages = {407},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3609-0},
   Abstract = {Many extensions of the Standard Model predict the existence
             of charged heavy long-lived particles, such as
             <i>R</i>-hadrons or charginos. These particles, if produced
             at the Large Hadron Collider, should be moving
             non-relativistically and are therefore identifiable through
             the measurement of an anomalously large specific energy loss
             in the ATLAS pixel detector. Measuring heavy long-lived
             particles through their track parameters in the vicinity of
             the interaction vertex provides sensitivity to metastable
             particles with lifetimes from 0.6 ns to 30 ns. A search
             for such particles with the ATLAS detector at the Large
             Hadron Collider is presented, based on a data sample
             corresponding to an integrated luminosity of [Formula: see
             text] fb[Formula: see text] of <i>pp</i> collisions at
             [Formula: see text] TeV. No significant deviation from the
             Standard Model background expectation is observed, and
             lifetime-dependent upper limits on <i>R</i>-hadrons and
             chargino production are set. Gluino <i>R</i>-hadrons with
             10 ns lifetime and masses up to 1185 GeV are excluded at
             95 [Formula: see text] confidence level, and so are
             charginos with 15 ns lifetime and masses up to
             482 GeV.},
   Doi = {10.1140/epjc/s10052-015-3609-0},
   Key = {fds321457}
}

@article{fds313385,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the W W + W Z cross section and limits on
             anomalous triple gauge couplings using final states with one
             lepton, missing transverse momentum, and two jets with the
             ATLAS detector at √s = 7 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Pages = {1-42},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)049},
   Abstract = {Abstract: The production of a W boson decaying to eν or
             μν in association with a W or Z boson decaying to two jets
             is studied using 4.6 fb−1 of proton-proton collision data
             at √s =7 TeV recorded with the ATLAS detector at the LHC.
             The combined WW + WZ cross section is measured with a
             significance of 3.4σ and is found to be 68±7 (stat.)±19
             (syst.) pb, in agreement with the Standard Model expectation
             of 61.1±2.2 pb. The distribution of the transverse momentum
             of the dijet system is used to set limits on anomalous
             contributions to the triple gauge coupling vertices and on
             parameters of an effective-field-theory model.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP01(2015)049},
   Key = {fds313385}
}

@article{fds313386,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the correlation between flow harmonics of
             different order in lead-lead collisions at √sNN
             = 2.76 TeV with the ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   ISSN = {0556-2813},
   url = {http://dx.doi.org/10.1103/PhysRevC.92.034903},
   Abstract = {Correlations between the elliptic or triangular flow
             coefficients vm (m = 2 or 3) and other flow harmonics vn (n
             = 2 to 5) are measured using √sNN = 2.76 TeV Pb + Pb
             collision data collected in 2010 by the ATLAS experiment at
             the LHC, corresponding to an integrated luminosity of 7
             μb−1. The vm-vn correlations are measured in midrapidity
             as a function of centrality, and, for events within the same
             centrality interval, as a function of event ellipticity or
             triangularity defined in a forward rapidity region. For
             events within the same centrality interval, v3 is found to
             be anticorrelated with v2 and this anticorrelation is
             consistent with similar anticorrelations between the
             corresponding eccentricities, ∊2 and ∊3. However, it is
             observed that v4 increases strongly with v2, and v5
             increases strongly with both v2 and v3. The trend and
             strength of the vm-vn correlations for n = 4 and 5 are found
             to disagree with ∊m-∊n correlations predicted by
             initial-geometry models. Instead, these correlations are
             found to be consistent with the combined effects of a linear
             contribution to vn and a nonlinear term that is a function
             of v22 or of v2v3, as predicted by hydrodynamic models. A
             simple two-component fit is used to separate these two
             contributions. The extracted linear and nonlinear
             contributions to v4 and v5 are found to be consistent with
             previously measured event-plane correlations.},
   Doi = {10.1103/PhysRevC.92.034903},
   Key = {fds313386}
}

@article{fds313384,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for supersymmetry in events containing a same-flavour
             opposite-sign dilepton pair, jets, and large missing
             transverse momentum in [Formula: see text] TeV pp
             collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {318},
   Year = {2015},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3518-2},
   Abstract = {Two searches for supersymmetric particles in final states
             containing a same-flavour opposite-sign lepton pair, jets
             and large missing transverse momentum are presented. The
             proton-proton collision data used in these searches were
             collected at a centre-of-mass energy [Formula: see
             text] TeV by the ATLAS detector at the Large Hadron
             Collider and corresponds to an integrated luminosity of
             20.3 fb[Formula: see text]. Two leptonic production
             mechanisms are considered: decays of squarks and gluinos
             with <i>Z</i> bosons in the final state, resulting in a peak
             in the dilepton invariant mass distribution around the
             <i>Z</i>-boson mass; and decays of neutralinos (e.g.
             [Formula: see text]), resulting in a kinematic endpoint in
             the dilepton invariant mass distribution. For the former, an
             excess of events above the expected Standard Model
             background is observed, with a significance of three
             standard deviations. In the latter case, the data are
             well-described by the expected Standard Model background.
             The results from each channel are interpreted in the context
             of several supersymmetric models involving the production of
             squarks and gluinos.},
   Doi = {10.1140/epjc/s10052-015-3518-2},
   Key = {fds313384}
}

@article{fds321448,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurements of the top quark branching ratios into channels
             with leptons and quarks with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.072005},
   Abstract = {Measurements of the branching ratios of top quark decays
             into leptons and jets using events with tt (top antitop)
             pairs are reported. Events were recorded with the ATLAS
             detector at the LHC in pp collisions at a center-of-mass
             energy of 7 TeV. The collected data sample corresponds to an
             integrated luminosity of 4.6 fb-1. The measured top quark
             branching ratios agree with the Standard Model predictions
             within the measurement uncertainties of a few
             percent.},
   Doi = {10.1103/PhysRevD.92.072005},
   Key = {fds321448}
}

@article{fds321450,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and T. H.
             Arce and A and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for higgs bosons decaying to aa in the µµττ final
             state in pp collisions at √s = 8 TeV with the ATLAS
             experiment},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {5},
   Pages = {052002-1-052002-24},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.052002},
   Abstract = {A search for the decay to a pair of new particles of either
             the 125 GeV Higgs boson (h) or a second charge parity
             (CP)-even Higgs boson (H) is presented. The data set
             corresponds to an integrated luminosity of 20.3 fb-1 of pp
             collisions at √s = 8 TeV recorded by the ATLAS experiment
             at the LHC in 2012. The search was done in the context of
             the next-to-minimal supersymmetric standard model, in which
             the new particles are the lightest neutral pseudoscalar
             Higgs bosons (a). One of the two a bosons is required to
             decay to two muons while the other is required to decay to
             two τ leptons. No significant excess is observed above the
             expected backgrounds in the dimuon invariant mass range from
             3.7 to 50 GeV. Upper limits are placed on the production of
             h → aa relative to the standard model gg → h production,
             assuming no coupling of the a boson to quarks. The most
             stringent limit is placed at 3.5% for ma = 3.75 GeV. Upper
             limits are also placed on the production cross section of H
             → aa from 2.33 to 0.72 pb, for fixed ma = 5 GeV with mH
             ranging from 100 to 500 GeV.},
   Doi = {10.1103/PhysRevD.92.052002},
   Key = {fds321450}
}

@article{fds321454,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
   Title = {Search for a new resonance decaying to a W or
             Z boson and a Higgs boson in the [Formula: see text]
             final states with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {6},
   Pages = {263},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3474-x},
   Abstract = {A search for a new resonance decaying to a <i>W</i> or
             <i>Z</i> boson and a Higgs boson in the [Formula: see text]
             final states is performed using 20.3 fb[Formula: see text]
             of <i>pp</i> collision data recorded at [Formula: see
             text] 8 TeV with the ATLAS detector at the Large Hadron
             Collider. The search is conducted by examining the
             <i>WH</i> / <i>ZH</i> invariant mass distribution for a
             localized excess. No significant deviation from the Standard
             Model background prediction is observed. The results are
             interpreted in terms of constraints on the Minimal Walking
             Technicolor model and on a simplified approach based on a
             phenomenological Lagrangian of Heavy Vector
             Triplets.},
   Doi = {10.1140/epjc/s10052-015-3474-x},
   Key = {fds321454}
}

@article{fds313377,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
             SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
             K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
             WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
             N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G and Conventi, F and Cooke, M and Cooper,
             BD},
   Title = {Observation and measurements of the production of prompt and
             non-prompt [Formula: see text] mesons in association with a
             [Formula: see text] boson in [Formula: see text] collisions
             at [Formula: see text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {229},
   Year = {2015},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3406-9},
   Abstract = {The production of a [Formula: see text] boson in association
             with a [Formula: see text] meson in proton-proton collisions
             probes the production mechanisms of quarkonium and heavy
             flavour in association with vector bosons, and allows
             studies of multiple parton scattering. Using [Formula: see
             text] of data collected with the ATLAS experiment at the LHC
             in [Formula: see text] collisions at [Formula: see text],
             the first measurement of associated [Formula: see text]
             production is presented for both prompt and non-prompt
             [Formula: see text] production, with both signatures having
             a significance in excess of [Formula: see text]. The
             inclusive production cross-sections for [Formula: see text]
             boson production (analysed in [Formula: see text] or
             [Formula: see text] decay modes) in association with prompt
             and non-prompt [Formula: see text] are measured relative to
             the inclusive production rate of [Formula: see text] bosons
             in the same fiducial volume to be [Formula: see text] and
             [Formula: see text] respectively. Normalised differential
             production cross-section ratios are also determined as a
             function of the [Formula: see text] transverse momentum. The
             fraction of signal events arising from single and double
             parton scattering is estimated, and a lower limit of
             [Formula: see text] at [Formula: see text] confidence level
             is placed on the effective cross-section regulating double
             parton interactions.},
   Doi = {10.1140/epjc/s10052-015-3406-9},
   Key = {fds313377}
}

@article{fds321447,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for photonic signatures of gauge-mediated
             supersymmetry in 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.072001},
   Abstract = {A search is presented for photonic signatures motivated by
             generalized models of gauge-mediated supersymmetry breaking.
             This search makes use of 20.3 fb-1 of proton-proton
             collision data at √s = 8 TeV recorded by the ATLAS
             detector at the LHC, and explores models dominated by both
             strong and electroweak production of supersymmetric partner
             states. Four experimental signatures incorporating an
             isolated photon and significant missing transverse momentum
             are explored. These signatures include events with an
             additional photon, lepton, b-quark jet, or jet activity not
             associated with any specific underlying quark flavor. No
             significant excess of events is observed above the Standard
             Model prediction and model-dependent 95% confidence-level
             exclusion limits are set.},
   Doi = {10.1103/PhysRevD.92.072001},
   Key = {fds321447}
}

@article{fds310416,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Ålkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Erratum: Search for production of WW/WZ resonances decaying
             to a lepton, neutrino and jets in pp collisions at √s = 8
             TeV with the ATLAS detector (The European Physical Journal C
             (2015) 75 (209) DOI: 10.1140/epjc/s10052-015-3425-6)},
   Journal = {European Physical Journal C},
   Volume = {75},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3593-4},
   Doi = {10.1140/epjc/s10052-015-3593-4},
   Key = {fds310416}
}

@article{fds310430,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
             LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for massive supersymmetric particles decaying to many
             jets using the ATLAS detector in pp collisions at s =8
             TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.112016},
   Abstract = {Results of a search for decays of massive particles to fully
             hadronic final states are presented. This search uses 20.3
             fb-1 of data collected by the ATLAS detector in s=8 TeV
             proton-proton collisions at the LHC. Signatures based on
             high jet multiplicities without requirements on the missing
             transverse momentum are used to search for
             R-parity-violating supersymmetric gluino pair production
             with subsequent decays to quarks. The analysis is performed
             using a requirement on the number of jets, in combination
             with separate requirements on the number of b-tagged jets,
             as well as a topological observable formed from the scalar
             sum of the mass values of large-radius jets in the event.
             Results are interpreted in the context of all possible
             branching ratios of direct gluino decays to various quark
             flavors. No significant deviation is observed from the
             expected Standard Model backgrounds estimated using jet
             counting as well as data-driven templates of the
             total-jet-mass spectra. Gluino pair decays to ten or more
             quarks via intermediate neutralinos are excluded for a
             gluino with mass mg<1 TeV for a neutralino mass mχ10=500
             GeV. Direct gluino decays to six quarks are excluded for
             mg<917 GeV for light-flavor final states, and results for
             various flavor hypotheses are presented.},
   Doi = {10.1103/PhysRevD.91.112016},
   Key = {fds310430}
}

@article{fds310444,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Search for anomalous production of prompt same-sign lepton
             pairs and pair-produced doubly charged Higgs bosons with s
             =8 TeV pp collisions using the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP03(2015)041},
   Abstract = {Abstract: A low-background inclusive search for new physics
             in events with same-sign dileptons is presented. The search
             uses proton-proton collisions corresponding to 20.3 fb−1
             of integrated luminosity taken in 2012 at a centre-of-mass
             energy of 8 TeV with the ATLAS detector at the LHC. Pairs of
             isolated leptons with the same electric charge and large
             transverse momenta of the type e±e±, e±μ±, and μ±μ±
             are selected and their invariant mass distribution is
             examined. No excess of events above the expected level of
             Standard Model background is found. The results are used to
             set upper limits on the cross-sections for processes beyond
             the Standard Model. Limits are placed as a function of the
             dilepton invariant mass within a fiducial region
             corresponding to the signal event selection criteria.
             Exclusion limits are also derived for a specific model of
             doubly charged Higgs boson production.[Figure not available:
             see fulltext.]},
   Doi = {10.1007/JHEP03(2015)041},
   Key = {fds310444}
}

@article{fds310453,
   Author = {ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Determination of spin and parity of the Higgs boson in the
             [Formula: see text] decay channel with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {231},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3436-3},
   Abstract = {Studies of the spin and parity quantum numbers of the Higgs
             boson in the [Formula: see text] final state are presented,
             based on proton-proton collision data collected by the ATLAS
             detector at the Large Hadron Collider, corresponding to an
             integrated luminosity of 20.3 fb[Formula: see text] at a
             centre-of-mass energy of [Formula: see text] TeV. The
             Standard Model spin-parity [Formula: see text] hypothesis is
             compared with alternative hypotheses for both spin and CP.
             The case where the observed resonance is a mixture of the
             Standard-Model-like Higgs boson and CP-even ([Formula: see
             text]) or CP-odd ([Formula: see text]) Higgs boson in
             scenarios beyond the Standard Model is also studied. The
             data are found to be consistent with the Standard Model
             prediction and limits are placed on alternative spin and CP
             hypotheses, including CP mixing in different
             scenarios.},
   Doi = {10.1140/epjc/s10052-015-3436-3},
   Key = {fds310453}
}

@article{fds310454,
   Author = {Atlas Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
             J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
             Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
             O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
             K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
             E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
             P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
             GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
             SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
             P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
             K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
             B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
             B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
             P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
             CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
             D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
             S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH},
   Title = {Jet energy measurement and its systematic uncertainty in
             proton-proton collisions at [Formula: see text] TeV with
             the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Pages = {17},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3190-y},
   Abstract = {The jet energy scale (JES) and its systematic uncertainty
             are determined for jets measured with the ATLAS detector
             using proton-proton collision data with a centre-of-mass
             energy of [Formula: see text] TeV corresponding to an
             integrated luminosity of [Formula: see text][Formula: see
             text]. Jets are reconstructed from energy deposits forming
             topological clusters of calorimeter cells using the
             anti-[Formula: see text] algorithm with distance parameters
             [Formula: see text] or [Formula: see text], and are
             calibrated using MC simulations. A residual JES correction
             is applied to account for differences between data and MC
             simulations. This correction and its systematic uncertainty
             are estimated using a combination of in situ techniques
             exploiting the transverse momentum balance between a jet and
             a reference object such as a photon or a [Formula: see text]
             boson, for [Formula: see text] and pseudorapidities
             [Formula: see text]. The effect of multiple proton-proton
             interactions is corrected for, and an uncertainty is
             evaluated using in situ techniques. The smallest JES
             uncertainty of less than 1 % is found in the central
             calorimeter region ([Formula: see text]) for jets with
             [Formula: see text]. For central jets at lower [Formula: see
             text], the uncertainty is about 3 %. A consistent JES
             estimate is found using measurements of the calorimeter
             response of single hadrons in proton-proton collisions and
             test-beam data, which also provide the estimate for
             [Formula: see text] TeV. The calibration of forward jets is
             derived from dijet [Formula: see text] balance measurements.
             The resulting uncertainty reaches its largest value of 6 %
             for low-[Formula: see text] jets at [Formula: see text].
             Additional JES uncertainties due to specific event
             topologies, such as close-by jets or selections of event
             samples with an enhanced content of jets originating from
             light quarks or gluons, are also discussed. The magnitude of
             these uncertainties depends on the event sample used in a
             given physics analysis, but typically amounts to
             0.5-3 %.},
   Doi = {10.1140/epjc/s10052-014-3190-y},
   Key = {fds310454}
}

@article{fds310459,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Performance of the ATLAS muon trigger in pp collisions at
             [Formula: see text] TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {3},
   Pages = {120},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3325-9},
   Abstract = {The performance of the ATLAS muon trigger system is
             evaluated with proton-proton collision data collected in
             2012 at the Large Hadron Collider at a centre-of-mass energy
             of 8 TeV. It is primarily evaluated using events containing
             a pair of muons from the decay of [Formula: see text]
             bosons. The efficiency of the single-muon trigger is
             measured for muons with transverse momentum [Formula: see
             text] GeV, with a statistical uncertainty of less than
             0.01 % and a systematic uncertainty of 0.6 %. The
             [Formula: see text] range for efficiency determination is
             extended by using muons from decays of [Formula: see text]
             mesons, [Formula: see text] bosons, and top quarks. The muon
             trigger shows highly uniform and stable performance. The
             performance is compared to the prediction of a detailed
             simulation.},
   Doi = {10.1140/epjc/s10052-015-3325-9},
   Key = {fds310459}
}

@article{fds310460,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, M and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
             AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
             M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
             SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie,
             MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck,
             HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall,
             AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci,
             F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan,
             JG},
   Title = {Search for dark matter in events with heavy quarks and
             missing transverse momentum in [Formula: see text]
             collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {2},
   Pages = {92},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3306-z},
   Abstract = {This article reports on a search for dark matter pair
             production in association with bottom or top quarks in
             [Formula: see text] of [Formula: see text] collisions
             collected at [Formula: see text] TeV by the ATLAS detector
             at the LHC. Events with large missing transverse momentum
             are selected when produced in association with high-momentum
             jets of which one or more are identified as jets containing
             [Formula: see text]-quarks. Final states with top quarks are
             selected by requiring a high jet multiplicity and in some
             cases a single lepton. The data are found to be consistent
             with the Standard Model expectations and limits are set on
             the mass scale of effective field theories that describe
             scalar and tensor interactions between dark matter and
             Standard Model particles. Limits on the dark-matter-nucleon
             cross-section for spin-independent and spin-dependent
             interactions are also provided. These limits are
             particularly strong for low-mass dark matter. Using a
             simplified model, constraints are set on the mass of dark
             matter and of a coloured mediator suitable to explain a
             possible signal of annihilating dark matter.},
   Doi = {10.1140/epjc/s10052-015-3306-z},
   Key = {fds310460}
}

@article{fds310461,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
             SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
             O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
             V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurements of the [Formula: see text] production cross
             sections in association with jets with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {2},
   Pages = {82},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3262-7},
   Abstract = {This paper presents cross sections for the production of a
             [Formula: see text] boson in association with jets, measured
             in proton-proton collisions at [Formula: see text] with the
             ATLAS experiment at the large hadron collider. With an
             integrated luminosity of [Formula: see text], this data set
             allows for an exploration of a large kinematic range,
             including jet production up to a transverse momentum of
             [Formula: see text] and multiplicities up to seven
             associated jets. The production cross sections for [Formula:
             see text] bosons are measured in both the electron and muon
             decay channels. Differential cross sections for many
             observables are also presented including measurements of the
             jet observables such as the rapidities and the transverse
             momenta as well as measurements of event observables such as
             the scalar sums of the transverse momenta of the jets. The
             measurements are compared to numerous QCD predictions
             including next-to-leading-order perturbative calculations,
             resummation calculations and Monte Carlo
             generators.},
   Doi = {10.1140/epjc/s10052-015-3262-7},
   Key = {fds310461}
}

@article{fds310462,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
             I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos,
             G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil,
             HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian,
             S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
             WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
             V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
             S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S},
   Title = {Search for invisible particles produced in association with
             single-top-quarks in proton-proton collisions at [Formula:
             see text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {2},
   Pages = {79},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-014-3233-4},
   Abstract = {A search for the production of single-top-quarks in
             association with missing energy is performed in
             proton-proton collisions at a centre-of-mass energy of
             [Formula: see text] with the ATLAS experiment at the large
             hadron collider using data collected in 2012, corresponding
             to an integrated luminosity of [Formula: see
             text] fb[Formula: see text]. In this search, the [Formula:
             see text] boson from the top quark is required to decay into
             an electron or a muon and a neutrino. No deviation from the
             standard model prediction is observed, and upper limits are
             set on the production cross-section for resonant and
             non-resonant production of an invisible exotic state in
             association with a right-handed top quark. In the case of
             resonant production, for a spin-[Formula: see text]
             resonance with a mass of [Formula: see text] GeV, an
             effective coupling strength above [Formula: see text] is
             excluded at 95[Formula: see text] confidence level for the
             top quark and an invisible spin-[Formula: see text] state
             with mass between [Formula: see text] and [Formula: see
             text] GeV. In the case of non-resonant production, an
             effective coupling strength above [Formula: see text] is
             excluded at 95[Formula: see text] confidence level for the
             top quark and an invisible spin-[Formula: see text] state
             with mass between [Formula: see text] and [Formula: see
             text] GeV.},
   Doi = {10.1140/epjc/s10052-014-3233-4},
   Key = {fds310462}
}

@article{fds310463,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca,
             D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Search for production of [Formula: see text] resonances
             decaying to a lepton, neutrino and jets in [Formula: see
             text] collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {209},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3425-6},
   Abstract = {A search is presented for narrow diboson resonances decaying
             to [Formula: see text] or [Formula: see text] in the final
             state where one [Formula: see text] boson decays
             leptonically (to an electron or a muon plus a neutrino) and
             the other [Formula: see text] boson decays hadronically. The
             analysis is performed using an integrated luminosity of
             20.3 fb[Formula: see text] of [Formula: see text]
             collisions at [Formula: see text] TeV collected by the
             ATLAS detector at the large hadron collider. No evidence for
             resonant diboson production is observed, and resonance
             masses below 700 and 1490 GeV are excluded at 95 %
             confidence level for the spin-2 Randall-Sundrum bulk
             graviton [Formula: see text] with coupling constant of 1.0
             and the extended gauge model [Formula: see text] boson
             respectively.},
   Doi = {10.1140/epjc/s10052-015-3425-6},
   Key = {fds310463}
}

@article{fds310464,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
   Title = {Search for direct pair production of a chargino and a
             neutralino decaying to the 125 GeV Higgs boson in [Formula:
             see text] TeV [Formula: see text] collisions with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {208},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3408-7},
   Abstract = {A search is presented for the direct pair production of a
             chargino and a neutralino [Formula: see text], where the
             chargino decays to the lightest neutralino and the [Formula:
             see text] boson, [Formula: see text], while the neutralino
             decays to the lightest neutralino and the 125 GeV Higgs
             boson, [Formula: see text]. The final states considered for
             the search have large missing transverse momentum, an
             isolated electron or muon, and one of the following: either
             two jets identified as originating from bottom quarks, or
             two photons, or a second electron or muon with the same
             electric charge. The analysis is based on 20.3 [Formula:
             see text] of [Formula: see text] proton-proton collision
             data delivered by the Large Hadron Collider and recorded
             with the ATLAS detector. Observations are consistent with
             the Standard Model expectations, and limits are set in the
             context of a simplified supersymmetric model.},
   Doi = {10.1140/epjc/s10052-015-3408-7},
   Key = {fds310464}
}

@article{fds310465,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for [Formula: see text] decays in [Formula: see text]
             collisions at [Formula: see text] = 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {4},
   Pages = {165},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3372-2},
   Abstract = {A search for a massive [Formula: see text] gauge boson
             decaying to a top quark and a bottom quark is performed with
             the ATLAS detector in [Formula: see text] collisions at the
             LHC. The dataset was taken at a centre-of-mass energy of
             [Formula: see text] and corresponds to [Formula: see text]
             of integrated luminosity. This analysis is done in the
             hadronic decay mode of the top quark, where novel jet
             substructure techniques are used to identify jets from
             high-momentum top quarks. This allows for a search for
             high-mass [Formula: see text] bosons in the range
             1.5-3.0 [Formula: see text]. [Formula: see text]-tagging is
             used to identify jets originating from [Formula: see
             text]-quarks. The data are consistent with Standard Model
             background-only expectations, and upper limits at 95 %
             confidence level are set on the [Formula: see text] cross
             section times branching ratio ranging from [Formula: see
             text] to [Formula: see text] for left-handed [Formula: see
             text] bosons, and ranging from [Formula: see text] to
             [Formula: see text] for [Formula: see text] bosons with
             purely right-handed couplings. Upper limits at 95 %
             confidence level are set on the [Formula: see text]-boson
             coupling to [Formula: see text] as a function of the
             [Formula: see text] mass using an effective field theory
             approach, which is independent of details of particular
             models predicting a [Formula: see text] boson.},
   Doi = {10.1140/epjc/s10052-015-3372-2},
   Key = {fds310465}
}

@article{fds310466,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Measurement of three-jet production cross-sections in
             [Formula: see text] collisions at 7 [Formula: see text]
             centre-of-mass energy using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {5},
   Pages = {228},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3363-3},
   Abstract = {Double-differential three-jet production cross-sections are
             measured in proton-proton collisions at a centre-of-mass
             energy of [Formula: see text] using the ATLAS detector at
             the large hadron collider. The measurements are presented as
             a function of the three-jet mass [Formula: see text], in
             bins of the sum of the absolute rapidity separations between
             the three leading jets [Formula: see text]. Invariant masses
             extending up to 5  TeV are reached for [Formula: see
             text]. These measurements use a sample of data recorded
             using the ATLAS detector in 2011, which corresponds to an
             integrated luminosity of [Formula: see text]. Jets are
             identified using the anti-[Formula: see text] algorithm with
             two different jet radius parameters, [Formula: see text] and
             [Formula: see text]. The dominant uncertainty in these
             measurements comes from the jet energy scale.
             Next-to-leading-order QCD calculations corrected to account
             for non-perturbative effects are compared to the
             measurements. Good agreement is found between the data and
             the theoretical predictions based on most of the available
             sets of parton distribution functions, over the full
             kinematic range, covering almost seven orders of magnitude
             in the measured cross-section values.},
   Doi = {10.1140/epjc/s10052-015-3363-3},
   Key = {fds310466}
}

@article{fds310467,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
             Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
             V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
             A},
   Title = {Measurement of the top-quark mass in the fully hadronic
             decay channel from ATLAS data at [Formula: see
             text].},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {4},
   Pages = {158},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3373-1},
   Abstract = {The mass of the top quark is measured in a data set
             corresponding to 4.6 [Formula: see text] of proton-proton
             collisions with centre-of-mass energy [Formula: see
             text] TeV collected by the ATLAS detector at the LHC.
             Events consistent with hadronic decays of top-antitop quark
             pairs with at least six jets in the final state are
             selected. The substantial background from multijet
             production is modelled with data-driven methods that utilise
             the number of identified [Formula: see text]-quark jets and
             the transverse momentum of the sixth leading jet, which have
             minimal correlation. The top-quark mass is obtained from
             template fits to the ratio of three-jet to dijet mass. The
             three-jet mass is calculated from the three jets produced in
             a top-quark decay. Using these three jets the dijet mass is
             obtained from the two jets produced in the [Formula: see
             text] boson decay. The top-quark mass obtained from this fit
             is thus less sensitive to the uncertainty in the energy
             measurement of the jets. A binned likelihood fit yields a
             top-quark mass of [Formula: see text].},
   Doi = {10.1140/epjc/s10052-015-3373-1},
   Key = {fds310467}
}

@article{fds310468,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for new phenomena in final states with an energetic
             jet and large missing transverse momentum in pp
             collisions at [Formula: see text]TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {299},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3517-3},
   Abstract = {Results of a search for new phenomena in final states with
             an energetic jet and large missing transverse momentum are
             reported. The search uses 20.3 fb[Formula: see text] of
             [Formula: see text] TeV data collected in 2012 with the
             ATLAS detector at the LHC. Events are required to have at
             least one jet with [Formula: see text] GeV and no leptons.
             Nine signal regions are considered with increasing missing
             transverse momentum requirements between [Formula: see
             text] GeV and [Formula: see text] GeV. Good agreement is
             observed between the number of events in data and Standard
             Model expectations. The results are translated into
             exclusion limits on models with either large extra spatial
             dimensions, pair production of weakly interacting dark
             matter candidates, or production of very light gravitinos in
             a gauge-mediated supersymmetric model. In addition, limits
             on the production of an invisibly decaying Higgs-like boson
             leading to similar topologies in the final state are
             presented.},
   Doi = {10.1140/epjc/s10052-015-3517-3},
   Key = {fds310468}
}

@article{fds310469,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Search for the b¯b decay of the Standard Model Higgs boson
             in associated (W/Z)H production with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)069},
   Abstract = {Abstract: A search for the (Formula presented.) decay of the
             Standard Model Higgs boson is performed with the ATLAS
             experiment using the full dataset recorded at the LHC in Run
             1. The integrated luminosities used are 4.7 and 20.3 fb−1
             from pp collisions at (Formula presented.) and 8 TeV,
             respectively. The processes considered are associated (W/Z)H
             production, where W → eν/μν, Z → ee/μμ and Z →
             νν. The observed (expected) deviation from the
             background-only hypothesis corresponds to a significance of
             1.4 (2.6) standard deviations and the ratio of the measured
             signal yield to the Standard Model expectation is found to
             be μ = 0.52 ± 0.32 (stat.) ± 0.24 (syst.) for a Higgs
             boson mass of 125.36 GeV. The analysis procedure is
             validated by a measurement of the yield of (W/Z)Z production
             with (Formula presented.) in the same final states as for
             the Higgs boson search, from which the ratio of the observed
             signal yield to the Standard Model expectation is found to
             be 0.74 ± 0.09 (stat.) ± 0.14 (syst.).[Figure not
             available: see fulltext.].},
   Doi = {10.1007/JHEP01(2015)069},
   Key = {fds310469}
}

@article{fds310474,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Constraints on the off-shell Higgs boson signal strength in
             the high-mass ZZ and WW final states with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {335},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3542-2},
   Abstract = {Measurements of the <i>ZZ</i> and <i>WW</i> final states in
             the mass range above the [Formula: see text] and [Formula:
             see text] thresholds provide a unique opportunity to measure
             the off-shell coupling strength of the Higgs boson. This
             paper presents constraints on the off-shell Higgs boson
             event yields normalised to the Standard Model prediction
             (signal strength) in the [Formula: see text], [Formula: see
             text] and [Formula: see text] final states. The result is
             based on <i>pp</i> collision data collected by the ATLAS
             experiment at the LHC, corresponding to an integrated
             luminosity of 20.3 fb[Formula: see text] at a collision
             energy of [Formula: see text] TeV. Using the [Formula: see
             text] method, the observed 95 [Formula: see text]
             confidence level (CL) upper limit on the off-shell signal
             strength is in the range 5.1-8.6, with an expected range of
             6.7-11.0. In each case the range is determined by varying
             the unknown [Formula: see text] and [Formula: see text]
             background K-factor from higher-order quantum chromodynamics
             corrections between half and twice the value of the known
             signal K-factor. Assuming the relevant Higgs boson couplings
             are independent of the energy scale of the Higgs boson
             production, a combination with the on-shell measurements
             yields an observed (expected) 95 [Formula: see text] CL
             upper limit on [Formula: see text] in the range 4.5-7.5
             (6.5-11.2) using the same variations of the background
             K-factor. Assuming that the unknown [Formula: see text]
             background K-factor is equal to the signal K-factor, this
             translates into an observed (expected) 95 [Formula: see
             text] CL upper limit on the Higgs boson total width of 22.7
             (33.0) MeV.},
   Doi = {10.1140/epjc/s10052-015-3542-2},
   Key = {fds310474}
}

@article{fds310475,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for the Standard Model Higgs boson produced in
             association with top quarks and decaying into [Formula: see
             text] in [Formula: see text] collisions at [Formula: see
             text] with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {349},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3543-1},
   Abstract = {A search for the Standard Model Higgs boson produced in
             association with a top-quark pair, [Formula: see text], is
             presented. The analysis uses 20.3 fb<sup>-1</sup> of
             <i>pp</i> collision data at [Formula: see text], collected
             with the ATLAS detector at the Large Hadron Collider during
             2012. The search is designed for the [Formula: see text]
             decay mode and uses events containing one or two electrons
             or muons. In order to improve the sensitivity of the search,
             events are categorised according to their jet and
             <i>b</i>-tagged jet multiplicities. A neural network is used
             to discriminate between signal and background events, the
             latter being dominated by [Formula: see text]+jets
             production. In the single-lepton channel, variables
             calculated using a matrix element method are included as
             inputs to the neural network to improve discrimination of
             the irreducible [Formula: see text] background. No
             significant excess of events above the background
             expectation is found and an observed (expected) limit of 3.4
             (2.2) times the Standard Model cross section is obtained at
             95 % confidence level. The ratio of the measured [Formula:
             see text] signal cross section to the Standard Model
             expectation is found to be [Formula: see text] assuming a
             Higgs boson mass of 125[Formula: see text].},
   Doi = {10.1140/epjc/s10052-015-3543-1},
   Key = {fds310475}
}

@article{fds310476,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
   Title = {Search for invisible decays of the Higgs boson produced in
             association with a hadronically decaying vector boson in
             pp collisions at [Formula: see text] TeV with the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {337},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3551-1},
   Abstract = {A search for Higgs boson decays to invisible particles is
             performed using 20.3 [Formula: see text] of <i>pp</i>
             collision data at a centre-of-mass energy of 8 TeV recorded
             by the ATLAS detector at the Large Hadron Collider. The
             process considered is Higgs boson production in association
             with a vector boson ([Formula: see text] or <i>Z</i>) that
             decays hadronically, resulting in events with two or more
             jets and large missing transverse momentum. No excess of
             candidates is observed in the data over the background
             expectation. The results are used to constrain <i>VH</i>
             production followed by <i>H</i> decaying to invisible
             particles for the Higgs boson mass range [Formula: see
             text] GeV. The 95 % confidence-level observed upper limit
             on [Formula: see text] varies from 1.6 pb at 115 GeV to
             0.13 pb at 300 GeV. Assuming Standard Model production and
             including the [Formula: see text] contribution as signal,
             the results also lead to an observed upper limit of 78 % at
             95 % confidence level on the branching ratio of Higgs
             bosons decays to invisible particles at a mass of
             125 GeV.},
   Doi = {10.1140/epjc/s10052-015-3551-1},
   Key = {fds310476}
}

@article{fds310477,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
   Title = {Measurement of the top quark mass in the [Formula: see text]
             and [Formula: see text] channels using [Formula: see
             text] [Formula: see text] ATLAS data.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {7},
   Pages = {330},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3544-0},
   Doi = {10.1140/epjc/s10052-015-3544-0},
   Key = {fds310477}
}

@article{fds310478,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
             C},
   Title = {Search for heavy long-lived multi-charged particles in
             pp collisions at [Formula: see text] TeV using the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {75},
   Number = {8},
   Pages = {362},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3534-2},
   Abstract = {A search for heavy long-lived multi-charged particles is
             performed using the ATLAS detector at the LHC. Data
             collected in 2012 at [Formula: see text] TeV from <i>pp</i>
             collisions corresponding to an integrated luminosity of
             20.3 fb[Formula: see text]are examined. Particles producing
             anomalously high ionisation, consistent with long-lived
             massive particles with electric charges from [Formula: see
             text] to [Formula: see text] are searched for. No signal
             candidate events are observed, and 95 % confidence level
             cross-section upper limits are interpreted as lower mass
             limits for a Drell-Yan production model. The mass limits
             range between 660 and 785 GeV.},
   Doi = {10.1140/epjc/s10052-015-3534-2},
   Key = {fds310478}
}

@article{fds310455,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {Search for s-channel single top-quark production in
             proton-proton collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {740},
   Pages = {118-136},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.11.042},
   Abstract = {This Letter presents a search at the LHC for s-channel
             single top-quark production in proton-proton collisions at a
             centre-of-mass energy of 8 TeV. The analyzed data set was
             recorded by the ATLAS detector and corresponds to an
             integrated luminosity of 20.3 fb-1. Selected events contain
             one charged lepton, large missing transverse momentum and
             exactly two b-tagged jets. A multivariate event classifier
             based on boosted decision trees is developed to discriminate
             s-channel single top-quark events from the main background
             contributions. The signal extraction is based on a binned
             maximum-likelihood fit of the output classifier
             distribution. The analysis leads to an upper limit on the
             s-channel single top-quark production cross-section of 14.6
             pb at the 95% confidence level. The fit gives a
             cross-section of σs = 5.0 ± 4.3 pb, consistent with the
             Standard Model expectation.},
   Doi = {10.1016/j.physletb.2014.11.042},
   Key = {fds310455}
}

@article{fds310456,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for the Xb and other hidden-beauty states
             in the π+πϒ(1S) channel at
             ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {740},
   Pages = {199-217},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.11.055},
   Abstract = {This Letter presents a search for a hidden-beauty
             counterpart of the X(3872) in the mass ranges of
             10.05–10.31 GeV and 10.40–11.00 GeV, in the channel
             Xb→π+π−ϒ(1S)(→μ+μ−), using 16.2 fb−1 of s=8
             TeV pp collision data collected by the ATLAS detector at the
             LHC. No evidence for new narrow states is found, and upper
             limits are set on the product of the Xb cross section and
             branching fraction, relative to those of the ϒ(2S), at the
             95% confidence level using the CLS approach. These limits
             range from 0.8% to 4.0%, depending on mass. For masses above
             10.1 GeV, the expected upper limits from this analysis are
             the most restrictive to date. Searches for production of the
             ϒ(13DJ), ϒ(10860), and ϒ(11020) states also reveal no
             significant signals.},
   Doi = {10.1016/j.physletb.2014.11.055},
   Key = {fds310456}
}

@article{fds310457,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Search for H→γγ produced in association with top quarks
             and constraints on the Yukawa coupling between the top quark
             and the Higgs boson using data taken at 7 TeV and 8 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {740},
   Pages = {222-242},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2014.11.049},
   Abstract = {A search is performed for Higgs bosons produced in
             association with top quarks using the diphoton decay mode of
             the Higgs boson. Selection requirements are optimized
             separately for leptonic and fully hadronic final states from
             the top quark decays. The dataset used corresponds to an
             integrated luminosity of 4.5 fb−1 of proton–proton
             collisions at a center-of-mass energy of 7 TeV and 20.3
             fb−1 at 8 TeV recorded by the ATLAS detector at the CERN
             Large Hadron Collider. No significant excess over the
             background prediction is observed and upper limits are set
             on the tt¯H production cross section. The observed
             exclusion upper limit at 95% confidence level is 6.7 times
             the predicted Standard Model cross section value. In
             addition, limits are set on the strength of the Yukawa
             coupling between the top quark and the Higgs boson, taking
             into account the dependence of the tt¯H and tH cross
             sections as well as the H→γγ branching fraction on the
             Yukawa coupling. Lower and upper limits at 95% confidence
             level are set at −1.3 and +8.0 times the Yukawa coupling
             strength in the Standard Model.},
   Doi = {10.1016/j.physletb.2014.11.049},
   Key = {fds310457}
}

@article{fds310479,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JJA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of differential production cross sections for Z
             /γ∗ bosons in association with jets in p p ¯ collisions
             at s =1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.012002},
   Abstract = {Differential cross sections for the production of Z bosons
             or off-shell photons γ∗ in association with jets are
             measured in proton-antiproton collisions at center-of-mass
             energy s=1.96TeV using the full data set collected with the
             Collider Detector at Fermilab in Tevatron run II and
             corresponding to 9.6fb-1 of integrated luminosity. Results
             include first measurements at CDF of differential cross
             sections in events with a Z/γ∗ boson and three or more
             jets, the inclusive cross section for production of Z/γ∗
             and four or more jets, and cross sections as functions of
             various angular observables in lower jet-multiplicity final
             states. Measured cross sections are compared to several
             theoretical predictions.},
   Doi = {10.1103/PhysRevD.91.012002},
   Key = {fds310479}
}

@article{fds310472,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the tt¯ production cross-section as a
             function of jet multiplicity and jet transverse momentum in
             7 TeV proton-proton collisions with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)020},
   Abstract = {Abstract: The tt¯$$ t\overline{t} $$ production
             cross-section dependence on jet multiplicity and jet
             transverse momentum is reported for proton-proton collisions
             at a centre-of-mass energy of 7 TeV in the single-lepton
             channel. The data were collected with the ATLAS detector at
             the CERN Large Hadron Collider and comprise the full 2011
             data sample corresponding to an integrated luminosity of 4.6
             fb−1. Differential cross-sections are presented as a
             function of the jet multiplicity for up to eight jets using
             jet transverse momentum thresholds of 25, 40, 60, and 80
             GeV, and as a function of jet transverse momentum up to the
             fifth jet. The results are shown after background
             subtraction and corrections for all known detector effects,
             within a kinematic range closely matched to the experimental
             acceptance. Several QCD-based Monte Carlo models are
             compared with the results. Sensitivity to the parton shower
             modelling is found at the higher jet multiplicities, at high
             transverse momentum of the leading jet and in the transverse
             momentum spectrum of the fifth leading jet. The
             MC@NLO+HERWIG MC is found to predict too few events at
             higher jet multiplicities.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP01(2015)020},
   Key = {fds310472}
}

@article{fds310473,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Searches for heavy long-lived charged particles with the
             ATLAS detector in proton-proton collisions at √s = 8
             Tev},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {1},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2015)068},
   Abstract = {Abstract: Searches for heavy long-lived charged particles
             are performed using a data sample of 19.1 fb−1 from
             proton-proton collisions at a centre-of-mass energy of s=8$$
             \sqrt{s}=8 $$ TeV collected by the ATLAS detector at the
             Large Hadron Collider. No excess is observed above the
             estimated background and limits are placed on the mass of
             long-lived particles in various supersymmetric models.
             Long-lived tau sleptons in models with gauge-mediated
             symmetry breaking are excluded up to masses between 440 and
             385 GeV for tan β between 10 and 50, with a 290 GeV limit
             in the case where only direct tau slepton production is
             considered. In the context of simplified LeptoSUSY models,
             where sleptons are stable and have a mass of 300 GeV, squark
             and gluino masses are excluded up to a mass of 1500 and 1360
             GeV, respectively. Directly produced charginos, in
             simplified models where they are nearly degenerate to the
             lightest neutralino, are excluded up to a mass of 620 GeV.
             R-hadrons, composites containing a gluino, bottom squark or
             top squark, are excluded up to a mass of 1270, 845 and 900
             GeV, respectively, using the full detector; and up to a mass
             of 1260, 835 and 870 GeV using an approach disregarding
             information from the muon spectrometer.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP01(2015)068},
   Key = {fds310473}
}

@article{fds310470,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Measurements of Higgs boson production and couplings in the
             four-lepton channel in pp collisions at center-of-mass
             energies of 7 and 8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.012006},
   Abstract = {The final ATLAS Run 1 measurements of Higgs boson production
             and couplings in the decay channel H → ZZ∗ →
             l+l-l'+l'-, where l, l' = e or μ, are presented. These
             measurements were performed using pp collision data
             corresponding to integrated luminosities of 4.5 and 20.3
             fb-1 at center-of-mass energies of 7 and 8 TeV,
             respectively, recorded with the ATLAS detector at the LHC.
             The H → ZZ∗ → 4l signal is observed with a
             significance of 8.1 standard deviations, with an expectation
             of 6.2 standard deviations, at mH = 125.36 GeV, the combined
             ATLAS measurement of the Higgs boson mass from the H →
             γγ and H → ZZ∗ → 4l channels. The production rate
             relative to the Standard Model expectation, the signal
             strength, is measured in four different production
             categories in the H → ZZ∗ → 4l channel. The measured
             signal strength, at this mass, and with all categories
             combined, is 1.44+0.40-0.33. The signal strength for Higgs
             boson production in gluon fusion or in association with tt
             or bb pairs is found to be 1.7+0.5-0.4, while the signal
             strength for vector-boson fusion combined with WH/ZH
             associated production is found to be 0.3+1.6-0.9.},
   Doi = {10.1103/PhysRevD.91.012006},
   Key = {fds310470}
}

@article{fds310471,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for new phenomena in events with a photon and missing
             transverse momentum in pp collisions at √s =8 TeV with the
             ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.012008},
   Abstract = {Results of a search for new phenomena in events with an
             energetic photon and large missing transverse momentum with
             the ATLAS experiment at the LHC are reported. Data were
             collected in proton-proton collisions at a center-of-mass
             energy of 8 TeV and correspond to an integrated luminosity
             of 20.3 fb-1. The observed data are well described by the
             expected Standard Model backgrounds. The expected (observed)
             upper limit on the fiducial cross section for the production
             of events with a photon and large missing transverse
             momentum is 6.1 (5.3) fb at 95% confidence level. Exclusion
             limits are presented on models of new phenomena with large
             extra spatial dimensions, supersymmetric quarks, and direct
             pair production of dark-matter candidates.},
   Doi = {10.1103/PhysRevD.91.012008},
   Key = {fds310471}
}

@article{fds310448,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
             M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, MF and Besson, N and Betancourt,
             C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
             M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
             CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
             V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
             A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
             EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
             JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
             S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
   Title = {Search for Higgs boson pair production in the γγbb[over
             ¯] final state using pp collision data at
             sqrt[s]=8  TeV from the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {8},
   Pages = {081802},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.114.081802},
   Abstract = {Searches are performed for resonant and nonresonant Higgs
             boson pair production in the γγbb[over ¯] final state
             using 20  fb^{-1} of proton-proton collisions at a
             center-of-mass energy of 8 TeV recorded with the ATLAS
             detector at the CERN Large Hadron Collider. A 95% confidence
             level upper limit on the cross section times branching ratio
             of nonresonant production is set at 2.2 pb, while the
             expected limit is 1.0 pb. The difference derives from a
             modest excess of events, corresponding to 2.4 standard
             deviations from the background-only hypothesis. The limit
             observed in the search for a narrow X→hh resonance ranges
             between 0.7 and 3.5 pb as a function of the resonance
             mass.},
   Doi = {10.1103/physrevlett.114.081802},
   Key = {fds310448}
}

@article{fds310449,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
             Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
             RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
             R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
             M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
             K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
             CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
             R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
             R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
   Title = {Measurements of the Nuclear Modification Factor for Jets in
             Pb+Pb Collisions at √(s)NN]=2.76  TeV with the ATLAS
             detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {7},
   Pages = {072302},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/physrevlett.114.072302},
   Abstract = {Measurements of inclusive jet production are performed in pp
             and Pb+Pb collisions at √(s)NN=2.76  TeV with the
             ATLAS detector at the LHC, corresponding to integrated
             luminosities of 4.0 and 0.14  nb(-1), respectively. The
             jets are identified with the anti-k(t) algorithm with R=0.4,
             and the spectra are measured over the kinematic range of jet
             transverse momentum 32<p(T)<500  GeV and absolute
             rapidity |y|<2.1 and as a function of collision centrality.
             The nuclear modification factor R(AA) is evaluated, and jets
             are found to be suppressed by approximately a factor of 2 in
             central collisions compared to pp collisions. The R(AA)
             shows a slight increase with p(T) and no significant
             variation with rapidity.},
   Doi = {10.1103/physrevlett.114.072302},
   Key = {fds310449}
}

@article{fds310451,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
             O},
   Title = {Measurement of the inclusive jet cross-section in
             proton-proton collisions at √s=7 TeV using 4.5
             fb−1 of data with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {2},
   Pages = {1-54},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2015)153},
   Abstract = {Abstract: The inclusive jet cross-section is measured in
             proton-proton collisions at a centre-of-mass energy of 7 TeV
             using a data set corresponding to an integrated luminosity
             of 4.5 fb−1 collected with the ATLAS detector at the Large
             Hadron Collider in 2011. Jets are identified using the
             anti-kt algorithm with radius parameter values of 0.4 and
             0.6. The double-differential cross-sections are presented as
             a function of the jet transverse momentum and the jet
             rapidity, covering jet transverse momenta from 100 GeV to 2
             TeV. Next-to-leading-order QCD calculations corrected for
             non-perturbative effects and electroweak effects, as well as
             Monte Carlo simulations with next-to-leading-order matrix
             elements interfaced to parton showering, are compared to the
             measured cross-sections. A quantitative comparison of the
             measured cross-sections to the QCD calculations using
             several sets of parton distribution functions is
             performed.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP02(2015)153},
   Key = {fds310451}
}

@article{fds310450,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of the transverse polarization of Λ and Λ ¯
             hyperons produced in proton-proton collisions at √s = 7
             TeV using the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.032004},
   Abstract = {The transverse polarization of Λ and Λ¯ hyperons produced
             in proton-proton collisions at a center-of-mass energy of 7
             TeV is measured. The analysis uses 760 μb-1 of minimum bias
             data collected by the ATLAS detector at the LHC in the year
             2010. The measured transverse polarization averaged over
             Feynman xF from 5×10-5 to 0.01 and transverse momentum pT
             from 0.8 to 15 GeV is -0.010±0.005(stat)±0.004(syst) for
             Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also
             measured as a function of xF and pT, but no significant
             dependence on these variables is observed. Prior to this
             measurement, the polarization was measured at fixed-target
             experiments with center-of-mass energies up to about 40 GeV.
             The ATLAS results are compatible with the extrapolation of a
             fit from previous measurements to the xF range covered by
             this measurement.},
   Doi = {10.1103/PhysRevD.91.032004},
   Key = {fds310450}
}

@article{fds310452,
   Author = {Aaltonen, T and Alon, R and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
             A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Duchovni, E and Ebina, K and Edgar, R and Elagin,
             A},
   Title = {Studies of high-transverse momentum jet substructure and top
             quarks produced in 1.96 TeV proton-antiproton
             collisions},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {3},
   Year = {2015},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.032006},
   Abstract = {Results of a study of the substructure of the highest
             transverse momentum (pT) jets observed by the CDF
             Collaboration are presented. Events containing at least one
             jet with pT>400GeV/c in a sample corresponding to an
             integrated luminosity of 5.95fb-1, collected in 1.96 TeV
             proton-antiproton collisions at the Fermilab Tevatron
             collider, are selected. A study of the jet mass, angularity,
             and planar-flow distributions is presented, and the
             measurements are compared with predictions of perturbative
             quantum chromodynamics. A search for boosted top-quark
             production is also described, leading to a 95% confidence
             level upper limit of 38 fb on the production cross section
             of top quarks with pT>400GeV/c.},
   Doi = {10.1103/PhysRevD.91.032006},
   Key = {fds310452}
}

@article{fds310447,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
   Title = {Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ
             with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {12},
   Pages = {121801},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1103/physrevlett.114.121801},
   Abstract = {A search for the decays of the Higgs and Z bosons to J/ψγ
             and ϒ(nS)γ (n=1,2,3) is performed with pp collision data
             samples corresponding to integrated luminosities of up to
             20.3  fb^{-1} collected at sqrt[s]=8  TeV with the
             ATLAS detector at the CERN Large Hadron Collider. No
             significant excess of events is observed above expected
             backgrounds and 95% C.L. upper limits are placed on the
             branching fractions. In the J/ψγ final state the limits
             are 1.5×10^{-3} and 2.6×10^{-6} for the Higgs and Z boson
             decays, respectively, while in the ϒ(1S,2S,3S)γ final
             states the limits are (1.3,1.9,1.3)×10^{-3} and
             (3.4,6.5,5.4)×10^{-6}, respectively.},
   Doi = {10.1103/physrevlett.114.121801},
   Key = {fds310447}
}

@article{fds310446,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Simultaneous measurements of the tt¯, W+W-, and Z/γ∗
             →ττ production cross-sections in pp collisions at √s
             =7 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.052005},
   Abstract = {Simultaneous measurements of the tt¯, W+W-, and
             Z/γ∗→ττ production cross-sections using an integrated
             luminosity of 4.6 fb-1 of pp collisions at √s=7 TeV
             collected by the ATLAS detector at the LHC are presented.
             Events are selected with two high transverse momentum
             leptons consisting of an oppositely charged electron and
             muon pair. The three processes are separated using the
             distributions of the missing transverse momentum of events
             with zero and greater than zero jet multiplicities.
             Measurements of the fiducial cross-section are presented
             along with results that quantify for the first time the
             underlying correlations in the predicted and measured
             cross-sections due to proton parton distribution functions.
             These results indicate that the correlated
             next-to-leading-order predictions for tt¯ and
             Z/γ∗→ττ underestimate the data, while those at
             next-to-next-to-leading-order generally describe the data
             well. The full cross-sections are measured to be
             σ(tt¯)=181.2±2.8-9.5+9.7±3.3±3.3 pb,
             σ(W+W-)=53.3±2.7-8.0+7.3±1.0±0.5 pb, and
             σ(Z/γ∗→ττ)=1174±24-87+72±21±9 pb, where the cited
             uncertainties are due to statistics, systematic effects,
             luminosity and the LHC beam energy measurement,
             respectively. The W+W- measurement includes the small
             contribution from Higgs boson decays, H→W+W-.},
   Doi = {10.1103/PhysRevD.91.052005},
   Key = {fds310446}
}

@article{fds310445,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for new phenomena in the dijet mass distribution
             using pp collision data at √s =8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.052007},
   Abstract = {Dijet events produced in LHC proton-proton collisions at a
             center-of-mass energy s=8 TeV are studied with the ATLAS
             detector using the full 2012 data set, with an integrated
             luminosity of 20.3 fb-1. Dijet masses up to about 4.5 TeV
             are probed. No resonancelike features are observed in the
             dijet mass spectrum. Limits on the cross section times
             acceptance are set at the 95% credibility level for various
             hypotheses of new phenomena in terms of mass or energy
             scale, as appropriate. This analysis excludes excited quarks
             with a mass below 4.06 TeV, color-octet scalars with a mass
             below 2.70 TeV, heavy W′ bosons with a mass below 2.45
             TeV, chiral W∗ bosons with a mass below 1.75 TeV, and
             quantum black holes with six extra space-time dimensions
             with threshold mass below 5.66 TeV.},
   Doi = {10.1103/PhysRevD.91.052007},
   Key = {fds310445}
}

@article{fds313376,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
             S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
             H},
   Title = {Search for charged Higgs bosons decaying via H±
             → τ±ν in fully hadronic final states using
             pp collision data at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2015)088},
   Abstract = {Abstract: The results of a search for charged Higgs bosons
             decaying to a τ lepton and a neutrino, H± → τ±ν, are
             presented. The analysis is based on 19.5 fb−1 of
             proton-proton collision data at s$$ \sqrt{s} $$ = 8 TeV
             collected by the ATLAS experiment at the Large Hadron
             Collider. Charged Higgs bosons are searched for in events
             consistent with top-quark pair production or in associated
             production with a top quark, depending on the considered H±
             mass. The final state is characterised by the presence of a
             hadronic τ decay, missing transverse momentum, b-tagged
             jets, a hadronically decaying W boson, and the absence of
             any isolated electrons or muons with high transverse
             momenta. The data are consistent with the expected
             background from Standard Model processes. A statistical
             analysis leads to 95% confidence-level upper limits on the
             product of branching ratios ℬ(t → bH±) × ℬ(H± →
             τ±ν), between 0.23% and 1.3% for charged Higgs boson
             masses in the range 80-160GeV. It also leads to 95%
             confidence-level upper limits on the production cross
             section times branching ratio, σ(pp → tH± + X) ×
             ℬ(H± → τ±ν), between 0.76 pb and 4.5 fb, for
             charged Higgs boson masses ranging from 180 GeV to 1000 GeV.
             In the context of different scenarios of the Minimal
             Supersymmetric Standard Model, these results exclude nearly
             all values of tan β above one for charged Higgs boson
             masses between 80 GeV and 160 GeV, and exclude a region of
             parameter space with high tan β for H± masses between 200
             GeV and 250 GeV.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP03(2015)088},
   Key = {fds313376}
}

@article{fds310437,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
             C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
             BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
   Title = {Search for Scalar Charm Quark Pair Production in pp
             Collisions at sqrt[s]=8  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {16},
   Pages = {161801},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.161801},
   Abstract = {The results of a dedicated search for pair production of
             scalar partners of charm quarks are reported. The search is
             based on an integrated luminosity of 20.3  fb^{-1} of pp
             collisions at sqrt[s]=8  TeV recorded with the ATLAS
             detector at the LHC. The search is performed using events
             with large missing transverse momentum and at least two
             jets, where the two leading jets are each tagged as
             originating from c quarks. Events containing isolated
             electrons or muons are vetoed. In an R-parity-conserving
             minimal supersymmetric scenario in which a single
             scalar-charm state is kinematically accessible, and where it
             decays exclusively into a charm quark and a neutralino, 95%
             confidence-level upper limits are obtained in the
             scalar-charm-neutralino mass plane such that, for neutralino
             masses below 200 GeV, scalar-charm masses up to 490 GeV
             are excluded.},
   Doi = {10.1103/physrevlett.114.161801},
   Key = {fds310437}
}

@article{fds310438,
   Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
             T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
             R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
             D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
             O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
             D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox,
             CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson,
             R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de
             Barbaro, P and de Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
             SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto,
             F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
             PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field,
             R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest,
             R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov, V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini,
             P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin,
             D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald,
             MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr,
             RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays,
             C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
             La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
             A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
             AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich,
             I and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg,
             J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster,
             M and Lannon, K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee,
             SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis,
             JD and Li, D and Li, H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour, J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega, J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett, J and Neu, C and Neustroev, P and Nguyen, HT},
   Title = {Tevatron constraints on models of the Higgs boson with
             exotic spin and parity using decays to bottom-antibottom
             quark pairs.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {15},
   Pages = {151802},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.151802},
   Abstract = {Combined constraints from the CDF and D0 Collaborations on
             models of the Higgs boson with exotic spin J and parity P
             are presented and compared with results obtained assuming
             the standard model value JP=0+. Both collaborations analyzed
             approximately 10  fb(-) of proton-antiproton collisions
             with a center-of-mass energy of 1.96 TeV collected at the
             Fermilab Tevatron. Two models predicting exotic Higgs bosons
             with JP=0- and JP=2+ are tested. The kinematic properties of
             exotic Higgs boson production in association with a vector
             boson differ from those predicted for the standard model
             Higgs boson. Upper limits at the 95% credibility level on
             the production rates of the exotic Higgs bosons, expressed
             as fractions of the standard model Higgs boson production
             rate, are set at 0.36 for both the JP=0- hypothesis and the
             JP=2+ hypothesis. If the production rate times the branching
             ratio to a bottom-antibottom pair is the same as that
             predicted for the standard model Higgs boson, then the
             exotic bosons are excluded with significances of 5.0
             standard deviations and 4.9 standard deviations for the
             JP=0- and JP=2+ hypotheses, respectively.},
   Doi = {10.1103/physrevlett.114.151802},
   Key = {fds310438}
}

@article{fds310439,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
             N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
             Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
             SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes,
             RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori,
             M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
             JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
             M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
             G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
             A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
             S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
             P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
             L and Margaroli, F and Marino, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
             C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
             L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
             C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
             K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo
             Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
             L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
             WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
             M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
             S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
             D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
             F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
             SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
             W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
             Collaboration)},
   Title = {Constraints on models of the Higgs boson with exotic spin
             and parity using decays to bottom-antibottom quarks in the
             full CDF data set.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {14},
   Pages = {141802},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.141802},
   Abstract = {A search for particles with the same mass and couplings as
             those of the standard model Higgs boson but different spin
             and parity quantum numbers is presented. We test two
             specific alternative Higgs boson hypotheses: a pseudoscalar
             Higgs boson with spin-parity J^{P}=0^{-} and a gravitonlike
             Higgs boson with J^{P}=2^{+}, assuming for both a mass of
             125  GeV/c^{2}. We search for these exotic states
             produced in association with a vector boson and decaying
             into a bottom-antibottom quark pair. The vector boson is
             reconstructed through its decay into an electron or muon
             pair, or an electron or muon and a neutrino, or it is
             inferred from an imbalance in total transverse momentum. We
             use expected kinematic differences between events containing
             exotic Higgs bosons and those containing standard model
             Higgs bosons. The data were collected by the CDF experiment
             at the Tevatron proton-antiproton collider, operating at a
             center-of-mass energy of sqrt[s]=1.96  TeV, and
             correspond to an integrated luminosity of 9.45  fb^{-1}.
             We exclude deviations from the predictions of the standard
             model with a Higgs boson of mass 125  GeV/c^{2} at the
             level of 5 standard deviations, assuming signal strengths
             for exotic boson production equal to the prediction for the
             standard model Higgs boson, and set upper limits of
             approximately 30% relative to the standard model rate on the
             possible rate of production of each exotic
             state.},
   Doi = {10.1103/physrevlett.114.141802},
   Key = {fds310439}
}

@article{fds310440,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli,
             F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak,
             L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
             K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi,
             M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov,
             AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
             FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks,
             T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
             A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
             CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
             MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T},
   Title = {Measurement of spin correlation in top-antitop quark events
             and search for top squark pair production in pp collisions
             at √s=8  TeV using the ATLAS detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {14},
   Pages = {142001},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/physrevlett.114.142001},
   Abstract = {A measurement of spin correlation in tt[over ¯] production
             is presented using data collected with the ATLAS detector at
             the Large Hadron Collider in proton-proton collisions at a
             center-of-mass energy of 8 TeV, corresponding to an
             integrated luminosity of 20.3  fb^{-1}. The correlation
             between the top and antitop quark spins is extracted from
             dilepton tt[over ¯] events by using the difference in the
             azimuthal angle between the two charged leptons in the
             laboratory frame. In the helicity basis the measured degree
             of correlation corresponds to A_{helicity}=0.38±0.04, in
             agreement with the standard model prediction. A search is
             performed for pair production of top squarks with masses
             close to the top quark mass decaying to predominantly
             right-handed top quarks and a light neutralino, the lightest
             supersymmetric particle. Top squarks with masses between the
             top quark mass and 191 GeV are excluded at the 95%
             confidence level.},
   Doi = {10.1103/physrevlett.114.142001},
   Key = {fds310440}
}

@article{fds310441,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {Search for squarks and gluinos in events with isolated
             leptons, jets and missing transverse momentum at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {4},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2015)116},
   Abstract = {The results of a search for supersymmetry in final states
             containing at least one isolated lepton (electron or muon),
             jets and large missing transverse momentum with the ATLAS
             detector at the Large Hadron Collider are reported. The
             search is based on proton-proton collision data at a
             centre-of-mass energy √ = 8 TeV collected in 2012,
             corresponding to an integrated luminosity of 20 fb−1. No
             significant excess above the Standard Model expectation is
             observed. Limits are set on supersymmetric particle masses
             for various supersymmetric models. Depending on the model,
             the search excludes gluino masses up to 1.32 TeV and squark
             masses up to 840 GeV. Limits are also set on the parameters
             of a minimal universal extra dimension model, excluding a
             compactification radius of 1/Rc = 950 GeV for a cut-off
             scale times radius (ΛRc) of approximately
             30.},
   Doi = {10.1007/JHEP04(2015)116},
   Key = {fds310441}
}

@article{fds310442,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
             KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H},
   Title = {Evidence for the Higgs-boson Yukawa coupling to tau leptons
             with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {4},
   Pages = {1-74},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2015)117},
   Abstract = {Abstract: Results of a search for H → ττ decays are
             presented, based on the full set of proton-proton collision
             data recorded by the ATLAS experiment at the LHC during 2011
             and 2012. The data correspond to integrated luminosities of
             4.5 fb−1 and 20.3 fb−1 at centre-of-mass energies of
             √s = 7 TeV and √s = 8 TeV respectively. All combinations
             of leptonic (τ→ℓνν¯ with ℓ = e, μ) and hadronic
             (τ → hadrons ν) tau decays are considered. An excess of
             events over the expected background from other Standard
             Model processes is found with an observed (expected)
             significance of 4.5 (3.4) standard deviations. This excess
             provides evidence for the direct coupling of the recently
             discovered Higgs boson to fermions. The measured signal
             strength, normalised to the Standard Model expectation, of
             μ = 1. 43− 0.37+ 0.43 is consistent with the predicted
             Yukawa coupling strength in the Standard Model.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP04(2015)117},
   Key = {fds310442}
}

@article{fds325314,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Search for pair-produced long-lived neutral particles
             decaying to jets in the ATLAS hadronic calorimeter in pp
             collisions at s=8TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {743},
   Pages = {15-34},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.02.015},
   Abstract = {The ATLAS detector at the Large Hadron Collider at CERN is
             used to search for the decay of a scalar boson to a pair of
             long-lived particles, neutral under the Standard Model gauge
             group, in 20.3fb-1 of data collected in proton-proton
             collisions at s=8TeV. This search is sensitive to long-lived
             particles that decay to Standard Model particles producing
             jets at the outer edge of the ATLAS electromagnetic
             calorimeter or inside the hadronic calorimeter. No
             significant excess of events is observed. Limits are
             reported on the product of the scalar boson production cross
             section times branching ratio into long-lived neutral
             particles as a function of the proper lifetime of the
             particles. Limits are reported for boson masses from 100 GeV
             to 900 GeV, and a long-lived neutral particle mass from 10
             GeV to 150 GeV.},
   Doi = {10.1016/j.physletb.2015.02.015},
   Key = {fds325314}
}

@article{fds310458,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
   Title = {Search for W ′ → t b ¯ in the lepton plus jets final
             state in proton–proton collisions at a centre-of-mass
             energy of s = 8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {743},
   Pages = {235-255},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.02.051},
   Abstract = {A search for new charged massive gauge bosons, called W′,
             is performed with the ATLAS detector at the LHC, in
             proton–proton collisions at a centre-of-mass energy of s=8
             TeV, using a dataset corresponding to an integrated
             luminosity of 20.3 fb−1. This analysis searches for W′
             bosons in the W′→tb¯ decay channel in final states with
             electrons or muons, using a multivariate method based on
             boosted decision trees. The search covers masses between 0.5
             and 3.0 TeV, for right-handed or left-handed W′ bosons. No
             significant deviation from the Standard Model expectation is
             observed and limits are set on the W′→tb¯ cross-section
             times branching ratio and on the W′-boson effective
             couplings as a function of the W′-boson mass using the CLs
             procedure. For a left-handed (right-handed) W′ boson,
             masses below 1.70 (1.92) TeV are excluded at 95% confidence
             level.},
   Doi = {10.1016/j.physletb.2015.02.051},
   Key = {fds310458}
}

@article{fds310443,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Observation of top-quark pair production in association with
             a photon and measurement of the t t ¯ γ production cross
             section in pp collisions at √s =7 TeV using the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {April},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.072007},
   Abstract = {A search is performed for top-quark pairs (tt¯) produced
             together with a photon (γ) with transverse energy greater
             than 20 GeV using a sample of tt¯ candidate events in final
             states with jets, missing transverse momentum, and one
             isolated electron or muon. The data set used corresponds to
             an integrated luminosity of 4.59 fb-1 of proton-proton
             collisions at a center-of-mass energy of 7 TeV recorded by
             the ATLAS detector at the CERN Large Hadron Collider. In
             total, 140 and 222 tt¯γ candidate events are observed in
             the electron and muon channels, to be compared to the
             expectation of 79±26 and 120±39 non-tt¯γ background
             events, respectively. The production of tt¯γ events is
             observed with a significance of 5.3 standard deviations away
             from the null hypothesis. The tt¯γ production cross
             section times the branching ratio (BR) of the single-lepton
             decay channel is measured in a fiducial kinematic region
             within the ATLAS acceptance. The measured value is
             σtt¯γfid×BR=63±8(stat)-13+17(syst)±1(lumi) fb per
             lepton flavor, in good agreement with the leading-order
             theoretical calculation normalized to the
             next-to-leading-order theoretical prediction of 48±10
             fb.},
   Doi = {10.1103/PhysRevD.91.072007},
   Key = {fds310443}
}

@article{fds310433,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
   Title = {Combined Measurement of the Higgs Boson Mass in pp
             Collisions at sqrt[s]=7 and 8 TeV with the ATLAS and CMS
             Experiments.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {19},
   Pages = {191803},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1103/physrevlett.114.191803},
   Abstract = {A measurement of the Higgs boson mass is presented based on
             the combined data samples of the ATLAS and CMS experiments
             at the CERN LHC in the H→γγ and H→ZZ→4ℓ decay
             channels. The results are obtained from a simultaneous fit
             to the reconstructed invariant mass peaks in the two
             channels and for the two experiments. The measured masses
             from the individual channels and the two experiments are
             found to be consistent among themselves. The combined
             measured mass of the Higgs boson is m_{H}=125.09±0.21
             (stat)±0.11 (syst) GeV.},
   Doi = {10.1103/physrevlett.114.191803},
   Key = {fds310433}
}

@article{fds310434,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for a CP-odd Higgs boson decaying to Zh in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {744},
   Pages = {163-183},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.03.054},
   Abstract = {A search for a heavy, CP-odd Higgs boson, A, decaying into a
             Z boson and a 125 GeV Higgs boson, h, with the ATLAS
             detector at the LHC is presented. The search uses
             proton–proton collision data at a centre-of-mass energy of
             8 TeV corresponding to an integrated luminosity of 20.3
             fb−1. Decays of CP-even h bosons to ττ or bb pairs with
             the Z boson decaying to electron or muon pairs are
             considered, as well as h→bb decays with the Z boson
             decaying to neutrinos. No evidence for the production of an
             A boson in these channels is found and the 95% confidence
             level upper limits derived for σ(gg→A)×BR(A→Zh)×BR(h→ff¯)
             are 0.098–0.013 pb for f=τ and 0.57–0.014 pb for f=b in
             a range of mA=220–1000 GeV. The results are combined and
             interpreted in the context of two-Higgs-doublet
             models.},
   Doi = {10.1016/j.physletb.2015.03.054},
   Key = {fds310434}
}

@article{fds310435,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
   Title = {Measurement of the charge asymmetry in dileptonic decays of
             top quark pairs in pp collisions at √s = 7 TeV using the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2015)061},
   Abstract = {A measurement of the top-antitop (tt¯) charge asymmetry is
             presented using data corresponding to an integrated
             luminosity of 4.6 fb−1 of LHC pp collisions at a
             centreof-mass energy of 7 TeV collected by the ATLAS
             detector. Events with two charged leptons, at least two jets
             and large missing transverse momentum are selected. Two
             observables are studied: ACℓℓ based on the identified
             charged leptons, and (Formula Presented.), based on the
             reconstructed tt final state. The asymmetries are measured
             to be (Formula Presented.). The measured values are in
             agreement with the Standard Model predictions.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP05(2015)061},
   Key = {fds310435}
}

@article{fds310436,
   Author = {Aaltonen, T and Albrow, MG and Amerio, S and Amidei, D and Anastassov,
             A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
             T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri,
             A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
             B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
             A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
             F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
             DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
             B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher,
             R},
   Title = {Measurement of central exclusive π+π- production in p p ¯
             collisions at s =0.9 and 1.96 TeV at CDF MEASUREMENT of
             CENTRAL EXCLUSIVE π+π- ... T. AALTONEN et
             al.},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.091101},
   Abstract = {We measure exclusive π+π- production in proton-antiproton
             collisions at center-of-mass energies s=0.9 and 1.96 TeV in
             the Collider Detector at Fermilab. We select events with two
             oppositely charged particles, assumed to be pions, with
             pseudorapidity |η|<1.3 and with no other particles detected
             in |η|<5.9. We require the π+π- system to have rapidity
             |y|<1.0. The production mechanism of these events is
             expected to be dominated by double pomeron exchange, which
             constrains the quantum numbers of the central state. The
             data are potentially valuable for isoscalar meson
             spectroscopy and for understanding the pomeron in a region
             of transition between nonperturbative and perturbative
             quantum chromodynamics. The data extend up to dipion mass
             M(π+π-)=5000MeV/c2 and show resonance structures
             attributed to f0 and f2(1270) mesons. From the π+π- and
             K+K- spectra, we place upper limits on exclusive χc0(3415)
             production.},
   Doi = {10.1103/PhysRevD.91.091101},
   Key = {fds310436}
}

@article{fds310427,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
   Title = {Search for a Charged Higgs Boson Produced in the
             Vector-Boson Fusion Mode with Decay H(±)→W(±)Z using pp
             Collisions at √s=8  TeV with the ATLAS
             Experiment.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {23},
   Pages = {231801},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.114.231801},
   Abstract = {A search for a charged Higgs boson, H(±), decaying to a
             W(±) boson and a Z boson is presented. The search is based
             on 20.3  fb(-1) of proton-proton collision data at a
             center-of-mass energy of 8 TeV recorded with the ATLAS
             detector at the LHC. The H(±) boson is assumed to be
             produced via vector-boson fusion and the decays W(±)→qq'
             and Z→e(+)e(-)/μ(+)μ(-) are considered. The search is
             performed in a range of charged Higgs boson masses from 200
             to 1000 GeV. No evidence for the production of an H(±)
             boson is observed. Upper limits of 31-1020 fb at 95% C.L.
             are placed on the cross section for vector-boson fusion
             production of an H(±) boson times its branching fraction to
             W(±)Z. The limits are compared with predictions from the
             Georgi-Machacek Higgs triplet model.},
   Doi = {10.1103/physrevlett.114.231801},
   Key = {fds310427}
}

@article{fds310428,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
             P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
   Title = {Search for New Phenomena in Dijet Angular Distributions in
             Proton-Proton Collisions at sqrt[s]=8 TeV Measured with the
             ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {114},
   Number = {22},
   Pages = {221802},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/physrevlett.114.221802},
   Abstract = {A search for new phenomena in LHC proton-proton collisions
             at a center-of-mass energy of sqrt[s]=8 TeV was performed
             with the ATLAS detector using an integrated luminosity of
             17.3 fb^{-1}. The angular distributions are studied in
             events with at least two jets; the highest dijet mass
             observed is 5.5 TeV. All angular distributions are
             consistent with the predictions of the standard model. In a
             benchmark model of quark contact interactions, a
             compositeness scale below 8.1 TeV in a destructive
             interference scenario and 12.0 TeV in a constructive
             interference scenario is excluded at 95% C.L.; median
             expected limits are 8.9 TeV for the destructive interference
             scenario and 14.1 TeV for the constructive interference
             scenario.},
   Doi = {10.1103/physrevlett.114.221802},
   Key = {fds310428}
}

@article{fds310431,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G},
   Title = {Search for vectorlike B quarks in events with one isolated
             lepton, missing transverse momentum, and jets at s =8 TeV
             with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.112011},
   Abstract = {A search has been performed for pair production of heavy
             vectorlike down-type (B) quarks. The analysis explores the
             lepton-plus-jets final state, characterized by events with
             one isolated charged lepton (electron or muon), significant
             missing transverse momentum, and multiple jets. One or more
             jets are required to be tagged as arising from b quarks, and
             at least one pair of jets must be tagged as arising from the
             hadronic decay of an electroweak boson. The analysis uses
             the full data sample of pp collisions recorded in 2012 by
             the ATLAS detector at the LHC, operating at a center-of-mass
             energy of 8 TeV, corresponding to an integrated luminosity
             of 20.3 fb-1. No significant excess of events is observed
             above the expected background. Limits are set on vectorlike
             B production, as a function of the B branching ratios,
             assuming the allowable decay modes are B→Wt/Zb/Hb. In the
             chiral limit with a branching ratio of 100% for the decay
             B→Wt, the observed (expected) 95% C.L. lower limit on the
             vectorlike B mass is 810 GeV (760 GeV). In the case where
             the vectorlike B quark has branching ratio values
             corresponding to those of an SU(2) singlet state, the
             observed (expected) 95% C.L. lower limit on the vectorlike B
             mass is 640 GeV (505 GeV). The same analysis, when used to
             investigate pair production of a colored, charge 5/3 exotic
             fermion T5/3, with subsequent decay T5/3→Wt, sets an
             observed (expected) 95% C.L. lower limit on the T5/3 mass of
             840 GeV (780 GeV).},
   Doi = {10.1103/PhysRevD.91.112011},
   Key = {fds310431}
}

@article{fds310432,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the production and differential cross
             sections of W+W- bosons in association
             with jets in pp¯ collisions at √s = 1.96TeV},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.111101},
   Abstract = {We present a measurement of the W-boson-pair production
             cross section in pp¯ collisions at 1.96 TeV center-of-mass
             energy and the first measurement of the differential cross
             section as a function of jet multiplicity and leading-jet
             energy. The W+W- cross section is measured in the final
             state comprising two charged leptons and neutrinos, where
             either charged lepton can be an electron or a muon. Using
             data collected by the CDF experiment corresponding to
             9.7fb-1 of integrated luminosity, a total of 3027 collision
             events consistent with W+W- production are observed with an
             estimated background contribution of 1790 ± 190 events. The
             measured total cross section is σ(pp¯ → W+W-)= 14.0 ±
             0.6 (stat)-1.0+1.2 (syst) ± 0.8 (lumi) pb, consistent with
             the standard model prediction.},
   Doi = {10.1103/PhysRevD.91.111101},
   Key = {fds310432}
}

@article{fds310429,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of the top pair production cross section in 8
             TeV proton-proton collisions using kinematic information in
             the lepton + jets final state with ATLAS},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {91},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.91.112013},
   Abstract = {A measurement is presented of the (formula presented)
             inclusive production cross section in pp collisions at a
             center-of-mass energy of (formula presented) using data
             collected by the ATLAS detector at the CERN Large Hadron
             pffiffi Collider. The measurement was performed in the
             lepton + jets final state using a data set corresponding to
             an integrated luminosity of 20.3 fb-1. The cross section was
             obtained using a likelihood discriminant fit and b-jet
             identification was used to improve the signal-to-background
             ratio. The inclusive tt production cross section was
             measured to be (formula presented) pb assuming a top-quark
             mass of 172.5 GeV, in good agreement with the theoretical
             prediction of (formula presented) pb. The (formula
             presented) production cross section in the fiducial region
             determined by the detector acceptance is also
             reported.},
   Doi = {10.1103/PhysRevD.91.112013},
   Key = {fds310429}
}

@article{fds321453,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {Differential top-antitop cross-section measurements as a
             function of observables constructed from final-state
             particles using pp collisions at √s = 7 TeV in the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {6},
   Pages = {1-56},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2015)100},
   Abstract = {Abstract: Various differential cross-sections are measured
             in top-quark pair (tt) events produced in proton-proton
             collisions at a centre-of-mass energy of √s = 7 TeV at the
             LHC with the ATLAS detector. These differential
             cross-sections are presented in a data set corresponding to
             an integrated luminosity of 4.6 fb−1. The differential
             cross-sections are presented in terms of kinematic
             variables, such as momentum, rapidity and invariant mass, of
             a top-quark proxy referred to as the pseudo-top-quark as
             well as the pseudo-top-quark pair system. The dependence of
             the measurement on theoretical models is minimal. The
             measurements are performed on tt events in the lepton+jets
             channel, requiring exactly one charged lepton and at least
             four jets with at least two of them tagged as originating
             from a b-quark. The hadronic and leptonic pseudo-top-quarks
             are defined via the leptonic or hadronic decay mode of the W
             boson produced by the top-quark decay in events with a
             single charged lepton. Differential cross-section
             measurements of the pseudo-top-quark variables are compared
             with several Monte Carlo models that implement
             next-to-leading order or leading-order multi-leg
             matrix-element calculations.},
   Doi = {10.1007/JHEP06(2015)100},
   Key = {fds321453}
}

@article{fds310421,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
             M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
             GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
             Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
             A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
             R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
             AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan,
             M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
             T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell,
             SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Evidence of Wγγ Production in pp Collisions at
             sqrt[s]=8  TeV and Limits on Anomalous Quartic Gauge
             Couplings with the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {3},
   Pages = {031802},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.115.031802},
   Abstract = {This Letter reports evidence of triple gauge boson
             production pp→W(ℓν)γγ+X, which is accessible for the
             first time with the 8 TeV LHC data set. The fiducial cross
             section for this process is measured in a data sample
             corresponding to an integrated luminosity of
             20.3  fb^{-1}, collected by the ATLAS detector in 2012.
             Events are selected using the W boson decay to eν or μν
             as well as requiring two isolated photons. The measured
             cross section is used to set limits on anomalous quartic
             gauge couplings in the high diphoton mass
             region.},
   Doi = {10.1103/physrevlett.115.031802},
   Key = {fds310421}
}

@article{fds310422,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
             P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
             D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
             C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
             N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
   Title = {Search for a Heavy Neutral Particle Decaying to eμ, eτ, or
             μτ in pp Collisions at sqrt[s]=8  TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {3},
   Pages = {031801},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/physrevlett.115.031801},
   Abstract = {This Letter presents a search for a heavy neutral particle
             decaying into an opposite-sign different-flavor dilepton
             pair, e^{±}μ^{∓}, e^{±}τ^{∓}, or μ^{±}τ^{∓}
             using 20.3  fb^{-1} of pp collision data at
             sqrt[s]=8  TeV collected by the ATLAS detector at the
             LHC. The numbers of observed candidate events are compatible
             with the standard model expectations. Limits are set on the
             cross section of new phenomena in two scenarios: the
             production of ν[over ˜]_{τ} in R-parity-violating
             supersymmetric models and the production of a
             lepton-flavor-violating Z^{'} vector boson.},
   Doi = {10.1103/physrevlett.115.031801},
   Key = {fds310422}
}

@article{fds316165,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
             H},
   Title = {Search for heavy Majorana neutrinos with the ATLAS detector
             in pp collisions at √s = 8 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2015)162},
   Abstract = {Abstract: A search for heavy Majorana neutrinos in events
             containing a pair of high-pT leptons of the same charge and
             high-pT jets is presented. The search uses 20.3 fb−1 of pp
             collision data collected with the ATLAS detector at the CERN
             Large Hadron Collider with a centre-of-mass energy of 221as
             = 8 TeV. The data are found to be consistent with the
             background-only hypothesis based on the Standard Model
             expectation. In the context of a Type-I seesaw mechanism,
             limits are set on the production cross-section times
             branching ratio for production of heavy Majorana neutrinos
             in the mass range between 100 and 500 GeV. The limits are
             subsequently interpreted as limits on the mixing between the
             heavy Majorana neutrinos and the Standard Model neutrinos.
             In the context of a left-right symmetric model, limits on
             the production cross-section times branching ratio are set
             with respect to the masses of heavy Majorana neutrinos and
             heavy gauge bosons WR and Z′.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP07(2015)162},
   Key = {fds316165}
}

@article{fds310424,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {A search for high-mass resonances decaying to
             τ+τ in pp collisions at √s =8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2015)157},
   Abstract = {Abstract: A search for high-mass resonances decaying into
             τ+τ− final states using proton-proton collisions at
             s=8$$ \sqrt{s}=8 $$ TeV produced by the Large Hadron
             Collider is presented. The data were recorded with the ATLAS
             detector and correspond to an integrated luminosity of
             19.5–20.3 fb−1. No statistically significant excess
             above the Standard Model expectation is observed; 95%
             credibility upper limits are set on the cross section times
             branching fraction of Z′ resonances decaying into τ+τ−
             pairs as a function of the resonance mass. As a result, Z′
             bosons of the Sequential Standard Model with masses less
             than 2.02 TeV are excluded at 95% credibility. The impact of
             the fermionic couplings on the Z′ acceptance is
             investigated and limits are also placed on a Z′ model that
             exhibits enhanced couplings to third-generation
             fermions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP07(2015)157},
   Key = {fds310424}
}

@article{fds310423,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Observation and measurement of Higgs boson decays to
             WWwith the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.012006},
   Abstract = {We report the observation of Higgs boson decays to
             WW∗based on an excess over background of 6.1 standard
             deviations in the dilepton final state, where the Standard
             Model expectation is 5.8 standard deviations. Evidence for
             the vector-boson fusion (VBF) production process is obtained
             with a significance of 3.2 standard deviations. The results
             are obtained from a data sample corresponding to an
             integrated luminosity of 25 fb-1from √s = 7 and 8 TeV pp
             collisions recorded by the ATLAS detector at the LHC. For a
             Higgs boson mass of 125.36 GeV, the ratio of the measured
             value to the expected value of the total production cross
             section times branching fraction is 1.09+0.16-0.15(stat)+0.17-0.14(syst).
             The corresponding ratios for the gluon fusion and
             vector-boson fusion production mechanisms are 1.02 ±
             0.19(stat)+0.22-0.18(syst) and 1.27+0.44-0.40(stat)+0.30-0.21(syst),
             respectively. At √s = 8 TeV, the total production cross
             sections are measured to be σ(gg→H→WW∗)=4.6±0.9(stat)+0.8-0.7(syst)
             pb and σ(VBF H → WW∗)=0.51+0.17-0.15(stat)+0.13-0.08(syst)pb.
             The fiducial cross section is determined for the
             gluon-fusion process in exclusive final states with zero or
             one associated jet.},
   Doi = {10.1103/PhysRevD.92.012006},
   Key = {fds310423}
}

@article{fds310425,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for long-lived, weakly interacting particles that
             decay to displaced hadronic jets in proton-proton collisions
             at s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.012010},
   Abstract = {A search for the decay of neutral, weakly interacting,
             long-lived particles using data collected by the ATLAS
             detector at the LHC is presented. This analysis uses the
             full data set recorded in 2012: 20.3 fb-1 of proton-proton
             collision data at s=8 TeV. The search employs techniques for
             reconstructing decay vertices of long-lived particles
             decaying to jets in the inner tracking detector and muon
             spectrometer. Signal events require at least two
             reconstructed vertices. No significant excess of events over
             the expected background is found, and limits as a function
             of proper lifetime are reported for the decay of the Higgs
             boson and other scalar bosons to long-lived particles and
             for Hidden Valley Z′ and Stealth SUSY benchmark models.
             The first search results for displaced decays in Z′ and
             Stealth SUSY models are presented. The upper bounds of the
             excluded proper lifetimes are the most stringent to
             date.},
   Doi = {10.1103/PhysRevD.92.012010},
   Key = {fds310425}
}

@article{fds310426,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for low-scale gravity signatures in multi-jet final
             states with the ATLAS detector at √s =
             8TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {7},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1007/JHEP07(2015)032},
   Abstract = {A search for evidence of physics beyond the Standard Model
             in final states with multiple high-transverse-momentum jets
             is performed using 20.3 fb−1 of proton-proton collision
             data at (Formula presented.) = 8 TeV recorded by the ATLAS
             detector at the LHC. No significant excess of events beyond
             Standard Model expectations is observed, and upper limits on
             the visible cross sections for non-Standard Model production
             of multi-jet final states are set. A wide variety of models
             for black hole and string ball production and decay are
             considered, and the upper limit on the cross section times
             acceptance is as low as 0.16 fb at the 95% confidence level.
             For these models, excluded regions are also given as
             function of the main model parameters.},
   Doi = {10.1007/JHEP07(2015)032},
   Key = {fds310426}
}

@article{fds310410,
   Author = {Oh, SH and Tepera, B and Wang, C},
   Title = {Performance of a multianode straw tube detector},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {797},
   Pages = {285-289},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {July},
   url = {http://dx.doi.org/10.1016/j.nima.2015.06.052},
   Abstract = {Abstract We report on the performance of a multianode straw
             tube detector using cosmic rays. It is constructed inside a
             5 cm diameter straw tube with twelve anode wires. A
             calibration technique and track reconstruction algorithm is
             developed for this type of detector, and we calculate the
             resolution from the residual distribution and show that
             ∼170 μm resolution is not difficult to achieve. The
             technique is general and especially useful for detectors
             with complex electric fields with or without the magnetic
             field.},
   Doi = {10.1016/j.nima.2015.06.052},
   Key = {fds310410}
}

@article{fds310413,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
             AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
             MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
             G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
             B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
             P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura,
             AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro,
             F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton,
             AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista,
             SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
   Title = {Measurements of the Total and Differential Higgs Boson
             Production Cross Sections Combining the H→γγ and
             H→ZZ^{*}→4ℓ Decay Channels at sqrt[s]=8  TeV with
             the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {9},
   Pages = {091801},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.115.091801},
   Abstract = {Measurements of the total and differential cross sections of
             Higgs boson production are performed using 20.3  fb^{-1}
             of pp collisions produced by the Large Hadron Collider at a
             center-of-mass energy of sqrt[s]=8  TeV and recorded by
             the ATLAS detector. Cross sections are obtained from
             measured H→γγ and H→ZZ^{*}→4ℓ event yields, which
             are combined accounting for detector efficiencies, fiducial
             acceptances, and branching fractions. Differential cross
             sections are reported as a function of Higgs boson
             transverse momentum, Higgs boson rapidity, number of jets in
             the event, and transverse momentum of the leading jet. The
             total production cross section is determined to be
             σ_{pp→H}=33.0±5.3 (stat)±1.6 (syst)  pb. The
             measurements are compared to state-of-the-art
             predictions.},
   Doi = {10.1103/physrevlett.115.091801},
   Key = {fds310413}
}

@article{fds310414,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzà, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
             A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bianchi, L and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
             J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
             Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
             AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da
             Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
             DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
             DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
             Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
             P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
             CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
             P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
             I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
             I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino,
             G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos,
             F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
             J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
             Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
             P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
             P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
   Title = {Search for Resonances Decaying to Top and Bottom Quarks with
             the CDF Experiment.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {6},
   Pages = {061801},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/physrevlett.115.061801},
   Abstract = {We report on a search for charged massive resonances
             decaying to top (t) and bottom (b) quarks in the full data
             set of proton-antiproton collisions at a center-of-mass
             energy of √[s]=1.96  TeV collected by the CDF II
             detector at the Tevatron, corresponding to an integrated
             luminosity of 9.5  fb(-1). No significant excess above
             the standard model background prediction is observed. We set
             95% Bayesian credibility mass-dependent upper limits on the
             heavy charged-particle production cross section times
             branching ratio to tb. Using a standard model extension with
             a W'→tb and left-right-symmetric couplings as a benchmark
             model, we constrain the W' mass and couplings in the
             300-900  GeV/c(2) range. The limits presented here are
             the most stringent for a charged resonance with mass in the
             range 300-600  GeV/c(2) decaying to top and bottom
             quarks.},
   Doi = {10.1103/physrevlett.115.061801},
   Key = {fds310414}
}

@article{fds310417,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for type-III seesaw heavy leptons in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032001},
   Abstract = {A search for the pair production of heavy leptons (N0,L±)
             predicted by the type-III seesaw theory formulated to
             explain the origin of small neutrino masses is presented.
             The decay channels N0→W±l (=e,μ,τ) and L±→W±ν
             (ν=νe,νμ,ντ) are considered. The analysis is performed
             using the final state that contains two leptons (electrons
             or muons), two jets from a hadronically decaying W boson and
             large missing transverse momentum. The data used in the
             measurement correspond to an integrated luminosity of 20.3
             fb-1 of pp collisions at s=8 TeV collected by the ATLAS
             detector at the LHC. No evidence of heavy lepton pair
             production is observed. Heavy leptons with masses below
             325-540 GeV are excluded at the 95% confidence level,
             depending on the theoretical scenario considered.},
   Doi = {10.1103/PhysRevD.92.032001},
   Key = {fds310417}
}

@article{fds310420,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {Measurement of the top-quark mass in the tt¯ dilepton
             channel using the full CDF Run II data set},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032003},
   Abstract = {We present a measurement of the top-quark mass in events
             containing two leptons (electrons or muons) with a large
             transverse momentum, two or more energetic jets, and a
             transverse-momentum imbalance. We use the full
             proton-antiproton collision data set collected by the CDF
             experiment during the Fermilab Tevatron Run II at
             center-of-mass energy s=1.96 TeV, corresponding to an
             integrated luminosity of 9.1 fb-1. A special observable is
             exploited for an optimal reduction of the dominant
             systematic uncertainty, associated with the knowledge of the
             absolute energy of the hadronic jets. The distribution of
             this observable in the selected events is compared to
             simulated distributions of tt¯ dilepton signal and
             background. We measure a value for the top-quark mass of
             171.5±1.9 (stat)±2.5 (syst) GeV/c2.},
   Doi = {10.1103/PhysRevD.92.032003},
   Key = {fds310420}
}

@article{fds315126,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {A search for tt resonances using lepton-plus-jets events in
             proton-proton collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)148},
   Abstract = {Abstract: A search for new particles that decay into top
             quark pairs is reported. The search is performed with the
             ATLAS experiment at the LHC using an integrated luminosity
             of 20.3 fb−1 of proton-proton collision data collected at
             a centre-of-mass energy of √s=8 TeV. The lepton-plus-jets
             final state is used, where the top pair decays to
             W+bW−b¯, with one W boson decaying leptonically and the
             other hadronically. The invariant mass spectrum of top quark
             pairs is examined for local excesses or deficits that are
             inconsistent with the Standard Model predictions. No
             evidence for a top quark pair resonance is found, and 95%
             confidence-level limits on the production rate are
             determined for massive states in benchmark models. The upper
             limits on the cross-section times branching ratio of a
             narrow Z′ boson decaying to top pairs range from 4.2 pb to
             0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A
             narrow leptophobic topcolour Z′ boson with mass below 1.8
             TeV is excluded. Upper limits are set on the cross-section
             times branching ratio for a broad colour-octet resonance
             with Γ/m = 15% decaying to tt¯. These range from 4.8 pb to
             0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein
             excitation of the gluon in a Randall-Sundrum model is
             excluded for masses below 2.2 TeV.},
   Doi = {10.1007/JHEP08(2015)148},
   Key = {fds315126}
}

@article{fds321451,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
             Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
             S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
             J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
             M},
   Title = {Search for new phenomena in events with three or more
             charged leptons in pp collisions at √s=8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)138},
   Abstract = {Abstract: A generic search for anomalous production of
             events with at least three charged leptons is presented. The
             data sample consists of pp collisions at √s=8 TeV
             collected in 2012 by the ATLAS experiment at the CERN Large
             Hadron Collider, and corresponds to an integrated luminosity
             of 20.3 fb−1. Events are required to have at least three
             selected lepton candidates, at least two of which must be
             electrons or muons, while the third may be a hadronically
             decaying tau. Selected events are categorized based on their
             lepton flavour content and signal regions are constructed
             using several kinematic variables of interest. No
             significant deviations from Standard Model predictions are
             observed. Model-independent upper limits on contributions
             from beyond the Standard Model phenomena are provided for
             each signal region, along with prescription to re-interpret
             the limits for any model. Constraints are also placed on
             models predicting doubly charged Higgs bosons and excited
             leptons. For doubly charged Higgs bosons decaying to eτ or
             μτ, lower limits on the mass are set at 400 GeV at 95%
             confidence level. For excited leptons, constraints are
             provided as functions of both the mass of the excited state
             and the compositeness scale Λ, with the strongest mass
             constraints arising in regions where the mass equals Λ. In
             such scenarios, lower mass limits are set at 3.0 TeV for
             excited electrons and muons, 2.5 TeV for excited taus, and
             1.6 TeV for every excited-neutrino flavour.},
   Doi = {10.1007/JHEP08(2015)138},
   Key = {fds321451}
}

@article{fds321452,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Study of (W/Z)H production and Higgs boson couplings using
             H→ W W decays with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)137},
   Abstract = {Abstract: A search for Higgs boson production in association
             with a W or Z boson, in the H→ W W∗ decay channel, is
             performed with a data sample collected with the ATLAS
             detector at the LHC in proton-proton collisions at
             centre-of-mass energies √s=7$$ \sqrt{s}=7 $$ TeV and 8
             TeV, corresponding to integrated luminosities of 4.5 fb−1
             and 20.3 fb−1, respectively. The WH production mode is
             studied in two-lepton and three-lepton final states, while
             two- lepton and four-lepton final states are used to search
             for the ZH production mode. The observed significance, for
             the combined W H and ZH production, is 2.5 standard
             deviations while a significance of 0.9 standard deviations
             is expected in the Standard Model Higgs boson hypothesis.
             The ratio of the combined W H and ZH signal yield to the
             Standard Model expectation, μV H , is found to be μV H =
             3.0− 1.1+ 1.3(stat.)− 0.7+ 1.0(sys.) for the Higgs boson
             mass of 125.36 GeV. The W H and ZH production modes are also
             combined with the gluon fusion and vector boson fusion
             production modes studied in the H → W W∗ → ℓνℓν
             decay channel, resulting in an overall observed significance
             of 6.5 standard deviations and μggF + VBF + VH = 1. 16−
             0.15+ 0.16(stat.)− 0.15+ 0.18(sys.). The results are
             interpreted in terms of scaling factors of the Higgs boson
             couplings to vector bosons (κV ) and fermions (κF ); the
             combined results are: |κV| = 1.06− 0.10+ 0.10, |κF| = 0.
             85− 0.20+ 0.26.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP08(2015)137},
   Key = {fds321452}
}

@article{fds310415,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for high-mass diphoton resonances in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032004},
   Abstract = {This article describes a search for high-mass resonances
             decaying to a pair of photons using a sample of 20.3 fb-1 of
             pp collisions at s=8 TeV recorded with the ATLAS detector at
             the Large Hadron Collider. The data are found to be in
             agreement with the Standard Model prediction, and limits are
             reported in the framework of the Randall-Sundrum model. This
             theory leads to the prediction of graviton states, the
             lightest of which could be observed at the Large Hadron
             Collider. A lower limit of 2.66 (1.41) TeV at 95% confidence
             level is set on the mass of the lightest graviton for
             couplings of k/M¯Pl=0.1 (0.01).},
   Doi = {10.1103/PhysRevD.92.032004},
   Key = {fds310415}
}

@article{fds310419,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Elagin, A and Erbacher, R and Errede,
             S},
   Title = {First measurement of the forward-backward asymmetry in
             bottom-quark pair production at high mass},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.032006},
   Abstract = {We measure the particle-level forward-backward production
             asymmetry in bb¯ pairs with masses (mbb¯) larger than 150
             GeV/c2, using events with hadronic jets and employing jet
             charge to distinguish b from b¯. The measurement uses 9.5
             fb-1 of pp¯ collisions at a center-of-mass energy of 1.96
             TeV recorded by the CDF II detector. The asymmetry as a
             function of mbb¯ is consistent with zero, as well as with
             the predictions of the standard model. The measurement
             disfavors a simple model including an axigluon with a mass
             of 200 GeV/c2, whereas a model containing a heavier 345
             GeV/c2 axigluon is not excluded.},
   Doi = {10.1103/PhysRevD.92.032006},
   Key = {fds310419}
}

@article{fds310418,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for production of vector-like quark pairs and of four
             top quarks in the lepton-plus-jets final state in pp
             collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2015)105},
   Abstract = {A search for pair production of vector-like quarks, both
             up-type (T) and down-type (B), as well as for four-top-quark
             production, is presented. The search is based on pp
             collisions at (Formula presented.) TeV recorded in 2012 with
             the ATLAS detector at the CERN Large Hadron Collider and
             corresponding to an integrated luminosity of 20.3 fb−1.
             Data are analysed in the lepton-plus-jets final state,
             characterised by an isolated electron or muon with high
             transverse momentum, large missing transverse momentum and
             multiple jets. Dedicated analyses are performed targeting
             three cases: a T quark with significant branching ratio to a
             W boson and a b-quark (TT¯→Wb+X), and both a T quark and
             a B quark with significant branching ratio to a Higgs boson
             and a third-generation quark (TT¯→Ht+XandBB¯→Hb+X
             respectively). No significant excess of events above the
             Standard Model expectation is observed, and 95% CL lower
             limits are derived on the masses of the vector-like T and B
             quarks under several branching ratio hypotheses assuming
             contributions from T → Wb, Zt, Ht and B → Wt, Zb, Hb
             decays. The 95% CL observed lower limits on the T quark mass
             range between 715 GeV and 950 GeV for all possible values of
             the branching ratios into the three decay modes, and are the
             most stringent constraints to date. Additionally, the most
             restrictive upper bounds on four-top-quark production are
             set in a number of new physics scenarios.},
   Doi = {10.1007/JHEP08(2015)105},
   Key = {fds310418}
}

@article{fds321449,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Search for Dark Matter in Events with Missing Transverse
             Momentum and a Higgs Boson Decaying to Two Photons in pp
             Collisions at sqrt[s]=8 TeV with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {13},
   Pages = {131801},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.115.131801},
   Abstract = {Results of a search for new phenomena in events with large
             missing transverse momentum and a Higgs boson decaying to
             two photons are reported. Data from proton-proton collisions
             at a center-of-mass energy of 8 TeV and corresponding to an
             integrated luminosity of 20.3 fb^{-1} have been collected
             with the ATLAS detector at the LHC. The observed data are
             well described by the expected standard model backgrounds.
             Upper limits on the cross section of events with large
             missing transverse momentum and a Higgs boson candidate are
             also placed. Exclusion limits are presented for models of
             physics beyond the standard model featuring dark-matter
             candidates.},
   Doi = {10.1103/physrevlett.115.131801},
   Key = {fds321449}
}

@article{fds310411,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Centrality and rapidity dependence of inclusive jet
             production in √sNN =5 .02 TeV proton–lead collisions
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {748},
   Pages = {392-413},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.07.023},
   Abstract = {Measurements of the centrality and rapidity dependence of
             inclusive jet production in sNN=5.02 TeV proton–lead
             (p+Pb) collisions and the jet cross-section in s=2.76 TeV
             proton–proton collisions are presented. These quantities
             are measured in datasets corresponding to an integrated
             luminosity of 27.8 nb−1 and 4.0 pb−1, respectively,
             recorded with the ATLAS detector at the Large Hadron
             Collider in 2013. The p+Pb collision centrality was
             characterised using the total transverse energy measured in
             the pseudorapidity interval −4.9 <η <−3.2 in the
             direction of the lead beam. Results are presented for the
             double-differential per-collision yields as a function of
             jet rapidity and transverse momentum (pT) for minimum-bias
             and centrality-selected p+Pb collisions, and are compared to
             the jet rate from the geometric expectation. The total jet
             yield in minimum-bias events is slightly enhanced above the
             expectation in a pT-dependent manner but is consistent with
             the expectation within uncertainties. The ratios of jet
             spectra from different centrality selections show a strong
             modification of jet production at all pT at forward
             rapidities and for large pT at mid-rapidity, which manifests
             as a suppression of the jet yield in central events and an
             enhancement in peripheral events. These effects imply that
             the factorisation between hard and soft processes is
             violated at an unexpected level in proton–nucleus
             collisions. Furthermore, the modifications at forward
             rapidities are found to be a function of the total jet
             energy only, implying that the violations may have a simple
             dependence on the hard parton–parton kinematics.},
   Doi = {10.1016/j.physletb.2015.07.023},
   Key = {fds310411}
}

@article{fds310412,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Erratum to: Search for new phenomena in final states with an
             energetic jet and large missing transverse momentum in pp
             collisions at √s=8 TeV with the ATLAS detector (Eur. Phys.
             J. C (2015) 75:299, 10.1140/epjc/s10052-015-3517-3)},
   Journal = {European Physical Journal C},
   Volume = {75},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {September},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3639-7},
   Doi = {10.1140/epjc/s10052-015-3639-7},
   Key = {fds310412}
}

@article{fds336463,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the associated production of the Higgs boson with
             a top quark pair in multilepton final states with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {749},
   Pages = {519-541},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.07.079},
   Abstract = {A search for the associated production of the Higgs boson
             with a top quark pair is performed in multilepton final
             states using 20.3 fb−1 of proton–proton collision data
             recorded by the ATLAS experiment at s=8 TeV at the Large
             Hadron Collider. Five final states, targeting the decays
             H→WW⁎, ττ, and ZZ⁎, are examined for the presence of
             the Standard Model (SM) Higgs boson: two same-charge light
             leptons (e or μ) without a hadronically decaying τ lepton;
             three light leptons; two same-charge light leptons with a
             hadronically decaying τ lepton; four light leptons; and one
             light lepton and two hadronically decaying τ leptons. No
             significant excess of events is observed above the
             background expectation. The best fit for the tt¯H
             production cross section, assuming a Higgs boson mass of 125
             GeV, is 2.1−1.2+1.4 times the SM expectation, and the
             observed (expected) upper limit at the 95% confidence level
             is 4.7 (2.4) times the SM rate. The p-value for
             compatibility with the background-only hypothesis is 1.8σ;
             the expectation in the presence of a Standard Model signal
             is 0.9σ.},
   Doi = {10.1016/j.physletb.2015.07.079},
   Key = {fds336463}
}

@article{fds310409,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of exclusive γγ→ℓ+
             production in proton–proton collisions at √s=7 TeV with
             the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {749},
   Pages = {242-261},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.07.069},
   Abstract = {This Letter reports a measurement of the exclusive
             γγ→ℓ+ℓ− (ℓ=e, μ) cross-section in
             proton–proton collisions at a centre-of-mass energy of 7
             TeV by the ATLAS experiment at the LHC, based on an
             integrated luminosity of 4.6 fb−1. For the electron or
             muon pairs satisfying exclusive selection criteria, a fit to
             the dilepton acoplanarity distribution is used to extract
             the fiducial cross-sections. The cross-section in the
             electron channel is determined to be σγγ→e+e−excl.=0.428
             ± 0.035 (stat.) ± 0.018 (syst.) pb for a phase–space
             region with invariant mass of the electron pairs greater
             than 24 GeV, in which both electrons have transverse
             momentum pT>12 GeV and pseudorapidity |η|<2.4. For muon
             pairs with invariant mass greater than 20 GeV, muon
             transverse momentum pT>10 GeV and pseudorapidity |η|<2.4,
             the cross-section is determined to be σγγ→μ+μ−excl.=0.628
             ± 0.032 (stat.) ± 0.021 (syst.) pb. When proton absorptive
             effects due to the finite size of the proton are taken into
             account in the theory calculation, the measured
             cross-sections are found to be consistent with the theory
             prediction.},
   Doi = {10.1016/j.physletb.2015.07.069},
   Key = {fds310409}
}

@article{fds313383,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of differential J/ψ production cross sections
             and forward-backward ratios in p + Pb collisions with the
             ATLAS detector},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {92},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {October},
   ISSN = {0556-2813},
   url = {http://dx.doi.org/10.1103/PhysRevC.92.034904},
   Abstract = {Measurements of differential cross sections for J/ψ
             production in p + Pb collisions at (√SNN at the CERN Large
             Hadron Collider with the ATLAS detector are presented. The
             data set used corresponds to an integrated luminosity of
             28.1 nb−1. The J/ψ mesons are reconstructed in the dimuon
             decay channel over the transverse momentum range 8 < pT < 30
             GeV and over the center-of-mass rapidity range −2.87 <
             y∗ < 1.94. Prompt J/ψ are separated from J/ψ resulting
             from b-hadron decays through an analysis of the distance
             between the J/ψ decay vertex and the event primary vertex.
             The differential cross section for production of nonprompt
             J/ψ is compared to a FONLL calculation that does not
             include nuclear effects. Forward-backward production ratios
             are presented and compared to theoretical predictions. These
             results complement previously published results by covering
             a region of higher transverse momentum and more central
             rapidity. They thus constrain the kinematic dependence of
             nuclear modifications of charmonium and b-quark production
             in p + Pb collisions.},
   Doi = {10.1103/PhysRevC.92.034904},
   Key = {fds313383}
}

@article{fds316864,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of colour flow with the jet pull angle in tt-
             events using the ATLAS detector at √s=8
             TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {750},
   Pages = {475-493},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {November},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.09.051},
   Abstract = {The distribution and orientation of energy inside jets is
             predicted to be an experimental handle on colour connections
             between the hard-scatter quarks and gluons initiating the
             jets. This Letter presents a measurement of the distribution
             of one such variable, the jet pull angle. The pull angle is
             measured for jets produced in tt- events with one W boson
             decaying leptonically and the other decaying to jets using
             20.3 fb-1 of data recorded with the ATLAS detector at a
             centre-of-mass energy of s=8 TeV at the LHC. The jet pull
             angle distribution is corrected for detector resolution and
             acceptance effects and is compared to various
             models.},
   Doi = {10.1016/j.physletb.2015.09.051},
   Key = {fds316864}
}

@article{fds321446,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åesson, TPA and Akimov, AV and Alberghi,
             GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and varez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of transverse energy-energy correlations in
             multi-jet events in pp collisions at s=7 TeV using the ATLAS
             detector and determination of the strong coupling constant
             as(mZ)},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {750},
   Pages = {427-447},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.09.050},
   Abstract = {High transverse momentum jets produced in pp collisions at a
             centre of mass energy of 7 TeV are used to measure the
             transverse energy-energy correlation function and its
             associated azimuthal asymmetry. The data were recorded with
             the ATLAS detector at the LHC in the year 2011 and
             correspond to an integrated luminosity of 158 pb-1. The
             selection criteria demand the average transverse momentum of
             the two leading jets in an event to be larger than 250 GeV.
             The data at detector level are well described by Monte Carlo
             event generators. They are unfolded to the particle level
             and compared with theoretical calculations at
             next-to-leading-order accuracy. The agreement between data
             and theory is good and provides a precision test of
             perturbative Quantum Chromodynamics at large momentum
             transfers. From this comparison, the strong coupling
             constant given at the Z boson mass is determined to be
             as(mZ)=0.1173±0.0010 (exp.) -0.0026+0.0065
             (theo.).},
   Doi = {10.1016/j.physletb.2015.09.050},
   Key = {fds321446}
}

@article{fds313382,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of four-jet differential cross sections in
             √s=8 TeV proton-proton collisions using the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {12},
   Pages = {1-76},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2015)105},
   Abstract = {Differential cross sections for the production of at least
             four jets have been measured in proton-proton collisions at
             (Formula presented.) TeV at the Large Hadron Collider using
             the ATLAS detector. Events are selected if the four anti-ktR
             = 0.4 jets with the largest transverse momentum (pT) within
             the rapidity range |y| < 2.8 are well separated (ΔR4jmin >
             0.65), all have pT > 64 GeV, and include at least one jet
             with pT > 100 GeV. The dataset corresponds to an integrated
             luminosity of 20.3 fb−1. The cross sections, corrected for
             detector effects, are compared to leading-order and
             next-to-leading-order calculations as a function of the jet
             momenta, invariant masses, minimum and maximum opening
             angles and other kinematic variables.},
   Doi = {10.1007/JHEP12(2015)105},
   Key = {fds313382}
}

@article{fds313381,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
   Title = {Determination of the Ratio of b-Quark Fragmentation
             Fractions f(s)/f(d) in pp Collisions at √s=7  TeV with
             the ATLAS Detector.},
   Journal = {Physical review letters},
   Volume = {115},
   Number = {26},
   Pages = {262001},
   Year = {2015},
   Month = {December},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.115.262001},
   Abstract = {With an integrated luminosity of 2.47  fb(-1) recorded
             by the ATLAS experiment at the LHC, the exclusive decays
             B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0) of B mesons
             produced in pp collisions at √s=7  TeV are used to
             determine the ratio of fragmentation fractions f(s)/f(d).
             From the observed B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0)
             yields, the quantity (f(s)/f(d))[B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
             is measured to be 0.199±0.004(stat)±0.008(syst). Using a
             recent theory prediction for [B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
             yields (f(s)/f(d))=0.240±0.004(stat)±0.010(syst)±0.017(th).
             This result is based on a new approach that provides a
             significant improvement of the world average.},
   Doi = {10.1103/physrevlett.115.262001},
   Key = {fds313381}
}

@article{fds313379,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
             G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
             Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for high-mass diboson resonances with boson-tagged
             jets in proton-proton collisions at √s = 8TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {12},
   Pages = {1-39},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2015)055},
   Abstract = {Abstract: A search is performed for narrow resonances
             decaying into WW, WZ, or ZZ boson pairs using 20.3 fb−1 of
             proton-proton collision data at a centre-of-mass energy of
             s=8$$ \sqrt{s}=8 $$ TeV recorded with the ATLAS detector at
             the Large Hadron Collider. Diboson resonances with masses in
             the range from 1.3 to 3.0 TeV are sought after using the
             invariant mass distribution of dijets where both jets are
             tagged as a boson jet, compatible with a highly boosted W or
             Z boson decaying to quarks, using jet mass and substructure
             properties. The largest deviation from a smoothly falling
             background in the observed dijet invariant mass distribution
             occurs around 2 TeV in the WZ channel, with a global
             significance of 2.5 standard deviations. Exclusion limits at
             the 95% confidence level are set on the production cross
             section times branching ratio for the WZ final state of a
             new heavy gauge boson, W′, and for the WW and ZZ final
             states of Kaluza-Klein excitations of the graviton in a bulk
             Randall-Sundrum model, as a function of the resonance mass.
             W′ bosons with couplings predicted by the extended gauge
             model in the mass range from 1.3 to 1.5 TeV are excluded at
             95% confidence level.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP12(2015)055},
   Key = {fds313379}
}

@article{fds313378,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for flavour-changing neutral current top quark decays
             t → Hq in pp collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2015},
   Number = {12},
   Pages = {1-65},
   Publisher = {Springer Nature},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1007/JHEP12(2015)061},
   Abstract = {Abstract: A search for flavour-changing neutral current
             decays of a top quark to an uptype quark (q = u, c) and the
             Standard Model Higgs boson, where the Higgs boson decays
             to(Formula Presented.), is presented. The analysis searches
             for top quark pair events in which one top quark decays to
             Wb, with the W boson decaying leptonically, and the other
             top quark decays to Hq. The search is based on pp collisions
             at (Formula Presented.) TeV recorded in 2012 with the ATLAS
             detector at the CERN Large Hadron Collider and uses an
             integrated luminosity of 20.3 fb−1. Data are analysed in
             the lepton-plus-jets final state, characterised by an
             isolated electron or muon and at least four jets. The search
             exploits the high multiplicity of b-quark jets
             characteristic of signal events, and employs a likelihood
             discriminant that uses the kinematic differences between the
             signal and the background, which is dominated by (Formula
             Presented.) decays. No significant excess of events above
             the background expectation is found, and observed (expected)
             95% CL upper limits of 0.56% (0.42%) and 0.61% (0.64%) are
             derived for the t → Hc and t → Hu branching ratios
             respectively. The combination of this search with other
             ATLAS searches in the H → γγ and H → WW*, ττ decay
             modes significantly improves the sensitivity, yielding
             observed (expected) 95% CL upper limits on the t → Hc and
             t → Hu branching ratios of 0.46% (0.25%) and 0.45% (0.29%)
             respectively. The corresponding combined observed (expected)
             upper limits on the |λtcH| and |λtuH| couplings are 0.13
             (0.10) and 0.13 (0.10) respectively. These are the most
             restrictive direct bounds on tqH interactions measured so
             far.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP12(2015)061},
   Key = {fds313378}
}

@article{fds310482,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
             MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
             P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F},
   Title = {Search for nonpointing and delayed photons in the diphoton
             and missing transverse momentum final state in 8 TeV pp
             collisions at the LHC using the ATLAS detector SEARCH for
             NONPOINTING and DELAYED PHOTONS in ⋯ G. AAD et
             al.},
   Journal = {Zeitschrift fur Antikes Christentum},
   Volume = {19},
   Number = {3},
   Pages = {1DUMMY},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1103/PhysRevD.90.112005},
   Abstract = {© 2014 CERN. © 2014 CERN, for the ATLAS Collaboration.
             Published by the American Physical Society under the terms
             of the »http://creativecommons.org/licenses/by/3.0/»
             Creative Commons Attribution 3.0 License. Further
             distribution of this work must maintain attribution to the
             author(s) and the published article's title, journal
             citation, and DOI.A search has been performed, using the
             full 20.3 fb-1 data sample of 8 TeV proton-proton collisions
             collected in 2012 with the ATLAS detector at the LHC, for
             photons originating from a displaced vertex due to the decay
             of a neutral long-lived particle into a photon and an
             invisible particle. The analysis investigates the diphoton
             plus missing transverse momentum final state, and is
             therefore most sensitive to pair production of long-lived
             particles. The analysis technique exploits the capabilities
             of the ATLAS electromagnetic calorimeter to make precise
             measurements of the flight direction, as well as the time of
             flight, of photons. No excess is observed over the Standard
             Model predictions for background. Exclusion limits are set
             within the context of gauge mediated supersymmetry breaking
             models, with the lightest neutralino being the
             next-to-lightest supersymmetric particle and decaying into a
             photon and gravitino with a lifetime in the range from 250
             ps to about 100 ns.},
   Doi = {10.1103/PhysRevD.90.112005},
   Key = {fds310482}
}

@article{fds336462,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the branching ratio Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {751},
   Pages = {63-80},
   Publisher = {Elsevier BV},
   Year = {2015},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.10.009},
   Abstract = {An observation of the Λb0→ψ(2S)Λ0 decay and a
             comparison of its branching fraction with that of the
             Λb0→J/ψΛ0 decay has been made with the ATLAS detector
             in proton–proton collisions at s=8 TeV at the LHC using an
             integrated luminosity of 20.6 fb−1. The J/ψ and ψ(2S)
             mesons are reconstructed in their decays to a muon pair,
             while the Λ0→pπ− decay is exploited for the Λ0 baryon
             reconstruction. The Λb0 baryons are reconstructed with
             transverse momentum pT>10 GeV and pseudorapidity |η|<2.1.
             The measured branching ratio of the Λb0→ψ(2S)Λ0 and
             Λb0→J/ψΛ0 decays is Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)=0.501±0.033(stat)±0.019(syst),
             lower than the expectation from the covariant quark
             model.},
   Doi = {10.1016/j.physletb.2015.10.009},
   Key = {fds336462}
}

@article{fds313380,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Search for pair production of a new heavy quark that decays
             into a W boson and a light quark in pp collisions at s =8
             TeV with the ATLAS detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {92},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2015},
   Month = {December},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.92.112007},
   Abstract = {A search is presented for pair production of a new heavy
             quark (Q) that decays into a W boson and a light quark (q)
             in the final state where one W boson decays leptonically (to
             an electron or muon plus a neutrino) and the other W boson
             decays hadronically. The analysis is performed using an
             integrated luminosity of 20.3 fb-1 of pp collisions at s=8
             TeV collected by the ATLAS detector at the LHC. No evidence
             of QQ¯ production is observed. New chiral quarks with
             masses below 690 GeV are excluded at 95% confidence level,
             assuming BR(Q→Wq)=1. Results are also interpreted in the
             context of vectorlike quark models, resulting in the limits
             on the mass of a vectorlike quark in the two-dimensional
             plane of BR(Q→Wq) versus BR(Q→Hq).},
   Doi = {10.1103/PhysRevD.92.112007},
   Key = {fds313380}
}

@article{fds321754,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
             VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurement of the [Formula: see text] dijet cross section
             in pp collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {670},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4521-y},
   Abstract = {The dijet production cross section for jets containing a
             b-hadron (b-jets) has been measured in proton-proton
             collisions with a centre-of-mass energy of [Formula: see
             text] TeV, using the ATLAS detector at the LHC. The data
             used correspond to an integrated luminosity of [Formula: see
             text]. The cross section is measured for events with two
             identified b-jets with a transverse momentum [Formula: see
             text] GeV and a minimum separation in the [Formula: see
             text]-[Formula: see text] plane of [Formula: see text]. At
             least one of the jets in the event is required to have
             [Formula: see text] GeV. The cross section is measured
             differentially as a function of dijet invariant mass, dijet
             transverse momentum, boost of the dijet system, and the
             rapidity difference, azimuthal angle and angular distance
             between the b-jets. The results are compared to different
             predictions of leading order and next-to-leading order
             perturbative quantum chromodynamics matrix elements
             supplemented with models for parton-showers and
             hadronization.},
   Doi = {10.1140/epjc/s10052-016-4521-y},
   Key = {fds321754}
}

@article{fds321756,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
             VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Measurement of the photon identification efficiencies with
             the ATLAS detector using LHC Run-1 data.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {666},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4507-9},
   Abstract = {The algorithms used by the ATLAS Collaboration to
             reconstruct and identify prompt photons are described.
             Measurements of the photon identification efficiencies are
             reported, using 4.9 fb[Formula: see text] of pp collision
             data collected at the LHC at [Formula: see text] [Formula:
             see text] and 20.3 fb[Formula: see text] at [Formula: see
             text] [Formula: see text]. The efficiencies are measured
             separately for converted and unconverted photons, in four
             different pseudorapidity regions, for transverse momenta
             between 10 [Formula: see text] and 1.5 [Formula: see
             text]. The results from the combination of three data-driven
             techniques are compared to the predictions from a simulation
             of the detector response, after correcting the
             electromagnetic shower momenta in the simulation for the
             average differences observed with respect to data.
             Data-to-simulation efficiency ratios used as correction
             factors in physics measurements are determined to account
             for the small residual efficiency differences. These factors
             are measured with uncertainties between 0.5% and 10% in
             7 [Formula: see text] data and between 0.5% and 5.6% in
             8 [Formula: see text] data, depending on the photon
             transverse momentum and pseudorapidity.},
   Doi = {10.1140/epjc/s10052-016-4507-9},
   Key = {fds321756}
}

@article{fds321383,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
             F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
             VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Luminosity determination in pp collisions at [Formula: see
             text] = 8 TeV using the ATLAS detector at the
             LHC.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {653},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4466-1},
   Abstract = {The luminosity determination for the ATLAS detector at the
             LHC during pp collisions at [Formula: see text] 8 TeV in
             2012 is presented. The evaluation of the luminosity scale is
             performed using several luminometers, and comparisons
             between these luminosity detectors are made to assess the
             accuracy, consistency and long-term stability of the
             results. A luminosity uncertainty of [Formula: see text] is
             obtained for the [Formula: see text] of pp collision data
             delivered to ATLAS at [Formula: see text] 8 TeV in
             2012.},
   Doi = {10.1140/epjc/s10052-016-4466-1},
   Key = {fds321383}
}

@article{fds321385,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
             B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Baarreiro Guimrães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Binet,
             S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {Search for minimal supersymmetric standard model Higgs
             Bosons H / A and for a [Formula: see text] boson in the
             [Formula: see text] final state produced in pp collisions at
             [Formula: see text] TeV with the ATLAS detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {11},
   Pages = {585},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4400-6},
   Abstract = {A search for neutral Higgs bosons of the minimal
             supersymmetric standard model (MSSM) and for a heavneutral
             [Formula: see text] boson is performed using a data sample
             corresponding to an integrated luminosity of
             3.2 fb[Formula: see text] from proton-proton collisions at
             [Formula: see text]  [Formula: see text] recorded by the
             ATLAS detector at the LHC. The heavy resonance is assumed to
             decay to a [Formula: see text] pair with at least one
             [Formula: see text] lepton decaying to final states with
             hadrons and a neutrino. The search is performed in the mass
             range of 0.2-1.2  [Formula: see text] for the MSSM neutral
             Higgs bosons and 0.5-2.5  [Formula: see text] for the
             heavy neutral [Formula: see text] boson. The data are in
             good agreement with the background predicted by the Standard
             Model. The results are interpreted in MSSM and [Formula: see
             text] benchmark scenarios. The most stringent constraints on
             the MSSM [Formula: see text]-[Formula: see text] space
             exclude at 95 % confidence level (CL) [Formula: see text]
             for [Formula: see text] [Formula: see text] in the
             [Formula: see text] MSSM scenario. For the Sequential
             Standard Model, a [Formula: see text] mass up to
             1.90  [Formula: see text] is excluded at 95 % CL and
             masses up to 1.82-2.17  [Formula: see text] are excluded
             for a [Formula: see text] of the strong flavour
             model.},
   Doi = {10.1140/epjc/s10052-016-4400-6},
   Key = {fds321385}
}

@article{fds323483,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli,
             A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
             LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
   Title = {Search for the Higgs boson produced in association with a W
             boson and decaying to four b-quarks via two spin-zero
             particles in pp collisions at 13 TeV with the ATLAS
             detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {11},
   Pages = {605},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4418-9},
   Abstract = {This paper presents a dedicated search for exotic decays of
             the Higgs boson to a pair of new spin-zero particles,
             [Formula: see text], where the particle a decays to b-quarks
             and has a mass in the range of 20-60 GeV. The search is
             performed in events where the Higgs boson is produced in
             association with a [Formula: see text] boson, giving rise to
             a signature of a lepton (electron or muon), missing
             transverse momentum, and multiple jets from b-quark decays.
             The analysis is based on the full dataset of pp collisions
             at [Formula: see text] recorded in 2015 by the ATLAS
             detector at the CERN Large Hadron Collider, corresponding to
             an integrated luminosity of 3.2 [Formula: see text]. No
             significant excess of events above the Standard Model
             prediction is observed, and a [Formula: see text]
             confidence-level upper limit is derived for the product of
             the production cross section for [Formula: see text] times
             the branching ratio for the decay [Formula: see text]. The
             upper limit ranges from 6.2 pb for an a-boson mass
             [Formula: see text] to 1.5 pb for [Formula: see
             text].},
   Doi = {10.1140/epjc/s10052-016-4418-9},
   Key = {fds323483}
}

@article{fds327377,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
             YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
             S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {Search for squarks and gluinos in events with hadronically
             decaying tau leptons, jets and missing transverse momentum
             in proton-proton collisions at [Formula: see text] TeV
             recorded with the ATLAS detector.},
   Journal = {Eur Phys J C Part Fields},
   Volume = {76},
   Number = {12},
   Pages = {683},
   Year = {2016},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4481-2},
   Abstract = {A search for supersymmetry in events with large missing
             transverse momentum, jets, and at least one hadronically
             decaying tau lepton has been performed using
             3.2 fb[Formula: see text] of proton-proton collision data
             at [Formula: see text] recorded by the ATLAS detector at the
             Large Hadron Collider in 2015. Two exclusive final states
             are considered, with either exactly one or at least two tau
             leptons. No excess over the Standard Model prediction is
             observed in the data. Results are interpreted in the context
             of gauge-mediated supersymmetry breaking and a simplified
             model of gluino pair production with tau-rich cascade
             decays, substantially improving on previous limits. In the
             GMSB model considered, supersymmetry-breaking scale
             ([Formula: see text]) values below [Formula: see text] are
             excluded at the 95% confidence level, corresponding to
             gluino masses below [Formula: see text]. For large values of
             [Formula: see text], values of [Formula: see text] up to
             [Formula: see text] and gluino masses up to [Formula: see
             text] are excluded. In the simplified model, gluino masses
             are excluded up to [Formula: see text] for neutralino masses
             around [Formula: see text]. Neutralino masses below
             [Formula: see text] are excluded for all gluino masses
             between 800 and [Formula: see text], while the strongest
             exclusion of [Formula: see text] is achieved for gluino
             masses around [Formula: see text].},
   Doi = {10.1140/epjc/s10052-016-4481-2},
   Key = {fds327377}
}

@article{fds321392,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Measurement of the total cross section from elastic
             scattering in pp collisions at √s=8 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {158-178},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.020},
   Abstract = {A measurement of the total pp cross section at the LHC at
             s=8 TeV is presented. An integrated luminosity of 500
             μb−1 was accumulated in a special run with high-β⋆
             beam optics to measure the differential elastic cross
             section as a function of the Mandelstam momentum transfer
             variable t. The measurement is performed with the ALFA
             sub-detector of ATLAS. Using a fit to the differential
             elastic cross section in the −t range from 0.014 GeV2 to
             0.1 GeV2 to extrapolate t→0, the total cross section,
             σtot(pp→X), is measured via the optical theorem to be
             σtot(pp→X)=96.07±0.18(stat.)±0.85(exp.)±0.31(extr.)mb,
             where the first error is statistical, the second accounts
             for all experimental systematic uncertainties and the last
             is related to uncertainties in the extrapolation t→0. In
             addition, the slope of the exponential function describing
             the elastic cross section at small t is determined to be
             B=19.74±0.05(stat.)±0.23(syst.)GeV−2.},
   Doi = {10.1016/j.physletb.2016.08.020},
   Key = {fds321392}
}

@article{fds321393,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
             M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
             W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
             AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {The performance of the jet trigger for the ATLAS detector
             during 2011 data taking.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {526},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4325-0},
   Abstract = {The performance of the jet trigger for the ATLAS detector at
             the LHC during the 2011 data taking period is described.
             During 2011 the LHC provided proton-proton collisions with a
             centre-of-mass energy of 7 TeV and heavy ion collisions
             with a 2.76 TeV per nucleon-nucleon collision energy. The
             ATLAS trigger is a three level system designed to reduce the
             rate of events from the 40 MHz nominal maximum bunch
             crossing rate to the approximate 400 Hz which can be
             written to offline storage. The ATLAS jet trigger is the
             primary means for the online selection of events containing
             jets. Events are accepted by the trigger if they contain one
             or more jets above some transverse energy threshold. During
             2011 data taking the jet trigger was fully efficient for
             jets with transverse energy above 25 GeV for triggers
             seeded randomly at Level 1. For triggers which require a jet
             to be identified at each of the three trigger levels, full
             efficiency is reached for offline jets with transverse
             energy above 60 GeV. Jets reconstructed in the final
             trigger level and corresponding to offline jets with
             transverse energy greater than 60 GeV, are reconstructed
             with a resolution in transverse energy with respect to
             offline jets, of better than 4 % in the central region and
             better than 2.5 % in the forward direction.},
   Doi = {10.1140/epjc/s10052-016-4325-0},
   Key = {fds321393}
}

@article{fds321394,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
             K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
             P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
             M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
             W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
             F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
             S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
             D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
             MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
             I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro,
             NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri,
             A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
             CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
   Title = {Search for gluinos in events with an isolated lepton, jets
             and missing transverse momentum at [Formula: see text] = 13
             Te V with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {565},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4397-x},
   Abstract = {The results of a search for gluinos in final states with an
             isolated electron or muon, multiple jets and large missing
             transverse momentum using proton-proton collision data at a
             centre-of-mass energy of [Formula: see text] are presented.
             The dataset used was recorded in 2015 by the ATLAS
             experiment at the Large Hadron Collider and corresponds to
             an integrated luminosity of 3.2 fb[Formula: see text]. Six
             signal selections are defined that best exploit the signal
             characteristics. The data agree with the Standard Model
             background expectation in all six signal selections, and the
             largest deviation is a 2.1 standard deviation excess. The
             results are interpreted in a simplified model where
             pair-produced gluinos decay via the lightest chargino to the
             lightest neutralino. In this model, gluinos are excluded up
             to masses of approximately 1.6 Te V depending on the mass
             spectrum of the simplified model, thus surpassing the limits
             of previous searches.},
   Doi = {10.1140/epjc/s10052-016-4397-x},
   Key = {fds321394}
}

@article{fds321395,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
             C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
             Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Search for bottom squark pair production in proton-proton
             collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {547},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4382-4},
   Abstract = {The result of a search for pair production of the
             supersymmetric partner of the Standard Model bottom quark
             ([Formula: see text]) is reported. The search uses
             3.2 fb[Formula: see text]  of <i>pp</i> collisions at
             [Formula: see text] TeV collected by the ATLAS experiment
             at the Large Hadron Collider in 2015. Bottom squarks are
             searched for in events containing large missing transverse
             momentum and exactly two jets identified as originating from
             <i>b</i>-quarks. No excess above the expected Standard Model
             background yield is observed. Exclusion limits at 95 %
             confidence level on the mass of the bottom squark are
             derived in phenomenological supersymmetric
             <i>R</i>-parity-conserving models in which the [Formula: see
             text] is the lightest squark and is assumed to decay
             exclusively via [Formula: see text], where [Formula: see
             text] is the lightest neutralino. The limits significantly
             extend previous results; bottom squark masses up to 800
             (840) GeV are excluded for the [Formula: see text] mass
             below 360 (100) GeV whilst differences in mass above
             100 GeV between the [Formula: see text] and the [Formula:
             see text] are excluded up to a [Formula: see text] mass of
             500 GeV.},
   Doi = {10.1140/epjc/s10052-016-4382-4},
   Key = {fds321395}
}

@article{fds321632,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for a high-mass Higgs boson decaying to a W boson
             pair in pp collisions at (Formula presented.) TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {1},
   Pages = {1-66},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2016)032},
   Abstract = {Abstract: A search for a high-mass Higgs boson H is
             performed in the H → WW → ℓνℓν and H → WW →
             ℓνqq decay channels using pp collision data corresponding
             to an integrated luminosity of 20.3 fb−1 collected at
             s=8(Formula presented.) TeV by the ATLAS detector at the
             Large Hadron Collider. No evidence of a high-mass Higgs
             boson is found. Limits on σH × BR(H → WW) as a function
             of the Higgs boson mass mH are determined in three different
             scenarios: one in which the heavy Higgs boson has a narrow
             width compared to the experimental resolution, one for a
             width increasing with the boson mass and modeled by the
             complex-pole scheme following the same behavior as in the
             Standard Model, and one for intermediate widths. The upper
             range of the search is mH = 1500 GeV for the narrow-width
             scenario and mH = 1000 GeV for the other two scenarios. The
             lower edge of the search range is 200–300 GeV and depends
             on the analysis channel and search scenario. For each signal
             interpretation, individual and combined limits from the two
             WW decay channels are presented. At mH = 1500 GeV, the
             highest-mass point tested, σH × BR(H → WW) for a
             narrow-width Higgs boson is constrained to be less than 22
             fb and 6.6 fb at 95% CL for the gluon fusion and
             vector-boson fusion production modes, respectively.[Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP01(2016)032},
   Key = {fds321632}
}

@article{fds321629,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
   Title = {Search for flavour-changing neutral current top-quark decays
             to [Formula: see text] in [Formula: see text] collision data
             collected with the ATLAS detector at [Formula: see
             text] TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {12},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3851-5},
   Abstract = {A search for the flavour-changing neutral-current decay
             [Formula: see text] is presented. Data collected by the
             ATLAS detector during 2012 from proton-proton collisions at
             the Large Hadron Collider at a centre-of-mass energy of
             [Formula: see text] TeV, corresponding to an integrated
             luminosity of 20.3 fb[Formula: see text], are analysed.
             Top-quark pair-production events with one top quark decaying
             through the [Formula: see text] ([Formula: see text])
             channel and the other through the dominant Standard Model
             mode [Formula: see text] are considered as signal. Only the
             decays of the <i>Z</i> boson to charged leptons and leptonic
             <i>W</i> boson decays are used. No evidence for a signal is
             found and an observed (expected) upper limit on the
             [Formula: see text] branching ratio of [Formula: see text]
             ([Formula: see text]) is set at the 95 % confidence
             level.},
   Doi = {10.1140/epjc/s10052-015-3851-5},
   Key = {fds321629}
}

@article{fds321630,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
             C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P},
   Title = {Measurements of fiducial cross-sections for [Formula: see
             text] production with one or two additional b-jets in
             pp collisions at [Formula: see text]=8 TeV using the
             ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {11},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3852-4},
   Abstract = {Fiducial cross-sections for [Formula: see text] production
             with one or two additional <i>b</i>-jets are reported, using
             an integrated luminosity of 20.3 fb[Formula: see text] of
             proton-proton collisions at a centre-of-mass energy of 8
             TeV at the Large Hadron Collider, collected with the ATLAS
             detector. The cross-section times branching ratio for
             [Formula: see text] events with at least one additional
             <i>b</i>-jet is measured to be 950 [Formula: see text]
             70 (stat.) [Formula: see text] (syst.) fb in the
             lepton-plus-jets channel and 50 [Formula: see text]
             10 (stat.) [Formula: see text] (syst.) fb in the
             [Formula: see text] channel. The cross-section times
             branching ratio for events with at least two additional
             <i>b</i>-jets is measured to be 19.3 [Formula: see text]
             3.5 (stat.) [Formula: see text] 5.7 (syst.) fb in the
             dilepton channel ([Formula: see text], [Formula: see text],
             and  <i>ee</i>) using a method based on tight selection
             criteria, and 13.5 [Formula: see text] 3.3 (stat.) [Formula:
             see text] 3.6 (syst.) fb using a looser selection that
             allows the background normalisation to be extracted from
             data. The latter method also measures a value of 1.30
             [Formula: see text] 0.33 (stat.) [Formula: see text]
             0.28 (syst.)% for the ratio of [Formula: see text]
             production with two additional <i>b</i>-jets to [Formula:
             see text] production with any two additional jets. All
             measurements are in good agreement with recent theory
             predictions.},
   Doi = {10.1140/epjc/s10052-015-3852-4},
   Key = {fds321630}
}

@article{fds321631,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
             Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
             M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
             R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
             P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
             S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
             Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
             S},
   Title = {Measurements of the Higgs boson production and decay rates
             and coupling strengths using pp collision data at
             [Formula: see text] and 8 TeV in the ATLAS
             experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {6},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3769-y},
   Abstract = {Combined analyses of the Higgs boson production and decay
             rates as well as its coupling strengths to vector bosons and
             fermions are presented. The combinations include the results
             of the analyses of the [Formula: see text] and [Formula: see
             text] decay modes, and the constraints on the associated
             production with a pair of top quarks and on the off-shell
             coupling strengths of the Higgs boson. The results are based
             on the LHC proton-proton collision datasets, with integrated
             luminosities of up to 4.7 [Formula: see text] at [Formula:
             see text] TeV and 20.3 [Formula: see text] at [Formula: see
             text] TeV, recorded by the ATLAS detector in 2011 and 2012.
             Combining all production modes and decay channels, the
             measured signal yield, normalised to the Standard Model
             expectation, is [Formula: see text]. The observed Higgs
             boson production and decay rates are interpreted in a
             leading-order coupling framework, exploring a wide range of
             benchmark coupling models both with and without assumptions
             on the Higgs boson width and on the Standard Model particle
             content in loop processes. The data are found to be
             compatible with the Standard Model expectations for a Higgs
             boson at a mass of 125.36 GeV for all models
             considered.},
   Doi = {10.1140/epjc/s10052-015-3769-y},
   Key = {fds321631}
}

@article{fds321635,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Search for direct top squark pair production in final states
             with two tau leptons in pp collisions at [Formula:
             see text] TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {81},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3897-z},
   Abstract = {A search for direct pair production of the supersymmetric
             partner of the top quark, decaying via a scalar tau to a
             nearly massless gravitino, has been performed using
             20 fb[Formula: see text] of proton-proton collision data at
             [Formula: see text]. The data were collected by the ATLAS
             experiment at the LHC in 2012. Top squark candidates are
             searched for in events with either two hadronically decaying
             tau leptons, one hadronically decaying tau and one light
             lepton, or two light leptons. No significant excess over the
             Standard Model expectation is found. Exclusion limits at
             [Formula: see text] confidence level are set as a function
             of the top squark and scalar tau masses. Depending on the
             scalar tau mass, ranging from the [Formula: see text] LEP
             limit to the top squark mass, lower limits between 490 and
             [Formula: see text] are placed on the top squark mass within
             the model considered.},
   Doi = {10.1140/epjc/s10052-016-3897-z},
   Key = {fds321635}
}

@article{fds323678,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
             C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
             CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
             JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Measurement of the charge asymmetry in top-quark pair
             production in the lepton-plus-jets final state in pp
             collision data at [Formula: see text] with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {87},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3910-6},
   Abstract = {This paper reports inclusive and differential measurements
             of the [Formula: see text] charge asymmetry [Formula: see
             text] in [Formula: see text] of [Formula: see text][Formula:
             see text] collisions recorded by the ATLAS experiment at the
             Large Hadron Collider at CERN. Three differential
             measurements are performed as a function of the invariant
             mass, transverse momentum and longitudinal boost of the
             [Formula: see text] system. The [Formula: see text] pairs
             are selected in the single-lepton channels (<i>e</i> or
             [Formula: see text]) with at least four jets, and a
             likelihood fit is used to reconstruct the [Formula: see
             text] event kinematics. A Bayesian unfolding procedure is
             performed to infer the asymmetry at parton level from the
             observed data distribution. The inclusive [Formula: see
             text] charge asymmetry is measured to be [Formula: see text]
             (stat. [Formula: see text] syst.). The inclusive and
             differential measurements are compatible with the values
             predicted by the Standard Model.},
   Doi = {10.1140/epjc/s10052-016-3910-6},
   Key = {fds323678}
}

@article{fds321755,
   Author = {Aad, G and Abbott, B and Abdinov, O and Abdallah, J and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
             K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
             LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
             OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
             AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
             O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
             L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
             CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou,
             Y},
   Title = {Test of CP invariance in vector-boson fusion production of
             the Higgs boson using the Optimal Observable method
             in the ditau decay channel with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {12},
   Pages = {658},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4499-5},
   Abstract = {A test of CP invariance in Higgs boson production via
             vector-boson fusion using the method of the <i>Optimal
             Observable</i> is presented. The analysis exploits the decay
             mode of the Higgs boson into a pair of [Formula: see text]
             leptons and is based on 20.3 [Formula: see text] of
             proton-proton collision data at [Formula: see text] =
             8 [Formula: see text] collected by the ATLAS experiment at
             the LHC. Contributions from CP-violating interactions
             between the Higgs boson and electroweak gauge bosons are
             described in an effective field theory framework, in which
             the strength of CP violation is governed by a single
             parameter [Formula: see text]. The mean values and
             distributions of CP-odd observables agree with the
             expectation in the Standard Model and show no sign of CP
             violation. The CP-mixing parameter [Formula: see text] is
             constrained to the interval [Formula: see text] at 68%
             confidence level, consistent with the Standard Model
             expectation of [Formula: see text].},
   Doi = {10.1140/epjc/s10052-016-4499-5},
   Key = {fds321755}
}

@article{fds315127,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
   Title = {Search for new phenomena in events with at least three
             photons collected in pp collisions at [Formula: see
             text] = 8 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {4},
   Pages = {210},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4034-8},
   Abstract = {Results of a search for new phenomena in events with at
             least three photons are reported. Data from proton-proton
             collisions at a centre-of-mass energy of 8 TeV,
             corresponding to an integrated luminosity of 20.3
             fb[Formula: see text], were collected with the ATLAS
             detector at the LHC. The observed data are well described by
             the Standard Model. Limits at the 95 % confidence level on
             new phenomena are presented based on the rate of events in
             an inclusive signal region and a restricted signal region
             targeting the rare decay [Formula: see text], as well as
             di-photon and tri-photon resonance searches. For a Standard
             Model Higgs boson decaying to four photons via a pair of
             intermediate pseudoscalar particles (<i>a</i>), limits are
             found to be [Formula: see text] for 10 GeV [Formula: see
             text] 62 GeV. Limits are also presented for Higgs boson-like
             scalars (<i>H</i>) for [Formula: see text] 125 GeV, and for
             a [Formula: see text] decaying to three photons via
             [Formula: see text]. Additionally, the observed limit on the
             branching ratio of the <i>Z</i> boson decay to three photons
             is found to be BR[Formula: see text], a result five times
             stronger than the previous result from LEP.},
   Doi = {10.1140/epjc/s10052-016-4034-8},
   Key = {fds315127}
}

@article{fds321386,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa,
             M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton,
             AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates,
             RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
             F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
             PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker,
             M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
             A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
             G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
             L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
             I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Brown, J and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Campana,
             S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
             MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
             I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo,
             F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G},
   Title = {Performance of pile-up mitigation techniques for jets in
             [Formula: see text] collisions at [Formula: see text] TeV
             using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {11},
   Pages = {581},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4395-z},
   Abstract = {The large rate of multiple simultaneous proton-proton
             interactions, or pile-up, generated by the Large Hadron
             Collider in Run 1 required the development of many new
             techniques to mitigate the adverse effects of these
             conditions. This paper describes the methods employed in the
             ATLAS experiment to correct for the impact of pile-up on jet
             energy and jet shapes, and for the presence of spurious
             additional jets, with a primary focus on the large
             20.3 [Formula: see text] data sample collected at a
             centre-of-mass energy of [Formula: see text]. The energy
             correction techniques that incorporate sophisticated
             estimates of the average pile-up energy density and tracking
             information are presented. Jet-to-vertex association
             techniques are discussed and projections of performance for
             the future are considered. Lastly, the extension of these
             techniques to mitigate the effect of pile-up on jet shapes
             using subtraction and grooming procedures is
             presented.},
   Doi = {10.1140/epjc/s10052-016-4395-z},
   Key = {fds321386}
}

@article{fds321426,
   Author = {Atlas Collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
             J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
             T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
             Kuutmann, E and Berger, N and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro,
             R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
             J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Search for squarks and gluinos in final states with jets and
             missing transverse momentum at [Formula: see text] =13
             [Formula: see text]with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {7},
   Pages = {392},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4184-8},
   Abstract = {A search for squarks and gluinos in final states containing
             hadronic jets, missing transverse momentum but no electrons
             or muons is presented. The data were recorded in 2015 by the
             ATLAS experiment in [Formula: see text] proton-proton
             collisions at the Large Hadron Collider. No excess above the
             Standard Model background expectation was observed in
             3.2 [Formula: see text] of analyzed data. Results are
             interpreted within simplified models that assume
             <i>R</i>-parity is conserved and the neutralino is the
             lightest supersymmetric particle. An exclusion limit at the
             95 % confidence level on the mass of the gluino is set at
             1.51 [Formula: see text] for a simplified model
             incorporating only a gluino octet and the lightest
             neutralino, assuming the lightest neutralino is massless.
             For a simplified model involving the strong production of
             mass-degenerate first- and second-generation squarks, squark
             masses below 1.03 [Formula: see text] are excluded for a
             massless lightest neutralino. These limits substantially
             extend the region of supersymmetric parameter space excluded
             by previous measurements with the ATLAS detector.},
   Doi = {10.1140/epjc/s10052-016-4184-8},
   Key = {fds321426}
}

@article{fds321427,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi,
             S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
             T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
   Title = {Charged-particle distributions in pp interactions at
             [Formula: see text] measured with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {7},
   Pages = {403},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4203-9},
   Abstract = {This paper presents measurements of distributions of charged
             particles which are produced in proton-proton collisions at
             a centre-of-mass energy of [Formula: see text] and recorded
             by the ATLAS detector at the LHC. A special dataset recorded
             in 2012 with a small number of interactions per beam
             crossing (below 0.004) and corresponding to an integrated
             luminosity of 160 [Formula: see text] was used. A
             minimum-bias trigger was utilised to select a data sample of
             more than 9 million collision events. The multiplicity,
             pseudorapidity, and transverse momentum distributions of
             charged particles are shown in different regions of
             kinematics and charged-particle multiplicity, including
             measurements of final states at high multiplicity. The
             results are corrected for detector effects and are compared
             to the predictions of various Monte Carlo event generator
             models which simulate the full hadronic final
             state.},
   Doi = {10.1140/epjc/s10052-016-4203-9},
   Key = {fds321427}
}

@article{fds321415,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
             K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
             LB and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
             VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
             G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
             JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
             L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
             F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
             D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
             LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
             F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
             D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella,
             G},
   Title = {Search for single production of vector-like quarks decaying
             into Wb in pp collisions at [Formula: see
             text] TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {8},
   Pages = {442},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4281-8},
   Abstract = {A search for singly produced vector-like <i>Q</i> quarks,
             where <i>Q</i> can be either a <i>T</i> quark with charge
             [Formula: see text] or a <i>Y</i> quark with charge
             [Formula: see text], is performed in proton-proton
             collisions recorded with the ATLAS detector at the LHC. The
             dataset corresponds to an integrated luminosity of 20.3
             fb[Formula: see text] and was produced with a centre-of-mass
             energy of [Formula: see text] TeV. This analysis targets
             [Formula: see text] decays where the <i>W</i> boson decays
             leptonically. A veto on massive large-radius jets is used to
             reject the dominant [Formula: see text] background. The
             reconstructed <i>Q</i>-candidate mass, ranging from 0.4 to
             1.2 TeV, is used in the search to discriminate signal from
             background processes. No significant deviation from the
             Standard Model expectation is observed, and limits are set
             on the [Formula: see text] cross-section times branching
             ratio. The results are also interpreted as limits on the
             <i>QWb</i> coupling and the mixing with the Standard Model
             sector for a singlet <i>T</i> quark or a <i>Y</i> quark from
             a doublet. <i>T</i> quarks with masses below 0.95 TeV are
             excluded at 95 % confidence level, assuming a unit coupling
             and a BR[Formula: see text], whereas the expected limit is
             1.10 TeV.},
   Doi = {10.1140/epjc/s10052-016-4281-8},
   Key = {fds321415}
}

@article{fds321403,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
             B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
             YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
             S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
             O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M},
   Title = {Search for supersymmetry in a final state containing two
             photons and missing transverse momentum in [Formula: see
             text] = 13 TeV [Formula: see text] collisions at the LHC
             using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {9},
   Pages = {517},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4344-x},
   Abstract = {A search has been made for supersymmetry in a final state
             containing two photons and missing transverse momentum using
             the ATLAS detector at the Large Hadron Collider. The search
             makes use of [Formula: see text] of proton-proton collision
             data collected at a centre-of-mass energy of 13 TeV in
             2015. Using a combination of data-driven and
             Monte-Carlo-based approaches, the Standard Model background
             is estimated to be [Formula: see text] events. No events are
             observed in the signal region; considering the expected
             background and its uncertainty, this observation implies a
             model-independent 95 % CL upper limit of 0.93 fb (3.0
             events) on the visible cross section due to physics beyond
             the Standard Model. In the context of a generalized model of
             gauge-mediated supersymmetry breaking with a bino-like
             next-to-lightest supersymmetric particle, this leads to a
             lower limit of 1650 GeV on the mass of a degenerate octet
             of gluino states, independent of the mass of the lighter
             bino-like neutralino.},
   Doi = {10.1140/epjc/s10052-016-4344-x},
   Key = {fds321403}
}

@article{fds321404,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
             N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
             F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
             JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
             Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
             EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
             C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
             R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
             SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
             P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
             S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
   Title = {Study of the rare decays of [Formula: see text] and
             [Formula: see text] into muon pairs from data collected
             during the LHC Run 1 with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {9},
   Pages = {513},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4338-8},
   Abstract = {A study of the decays [Formula: see text] and [Formula: see
             text] has been performed using data corresponding to an
             integrated luminosity of 25 fb[Formula: see text] of 7 and
             8 TeV proton-proton collisions collected with the ATLAS
             detector during the LHC Run 1. For the [Formula: see text]
             dimuon decay, an upper limit on the branching fraction is
             set at [Formula: see text] at 95 % confidence level. For
             [Formula: see text], the branching fraction [Formula: see
             text] is measured. The results are consistent with the
             Standard Model expectation with a <i>p</i> value of 4.8 %,
             corresponding to 2.0 standard deviations.},
   Doi = {10.1140/epjc/s10052-016-4338-8},
   Key = {fds321404}
}

@article{fds321406,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
             C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
             P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
             LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
             OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
             AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
             O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
             Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
             D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
             TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
             I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey,
             P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio,
             D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
             A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez,
             SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
             S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
             A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
             HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
             Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M and Clark, A},
   Title = {Charged-particle distributions at low transverse momentum in
             [Formula: see text] TeV pp interactions measured
             with the ATLAS detector at the LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {9},
   Pages = {502},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4335-y},
   Abstract = {Measurements of distributions of charged particles produced
             in proton-proton collisions with a centre-of-mass energy of
             13 TeV are presented. The data were recorded by the ATLAS
             detector at the LHC and correspond to an integrated
             luminosity of 151 [Formula: see text]. The particles are
             required to have a transverse momentum greater than 100 MeV
             and an absolute pseudorapidity less than 2.5. The
             charged-particle multiplicity, its dependence on transverse
             momentum and pseudorapidity and the dependence of the mean
             transverse momentum on multiplicity are measured in events
             containing at least two charged particles satisfying the
             above kinematic criteria. The results are corrected for
             detector effects and compared to the predictions from
             several Monte Carlo event generators.},
   Doi = {10.1140/epjc/s10052-016-4335-y},
   Key = {fds321406}
}

@article{fds316868,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the production cross-section of a single top
             quark in association with a W boson at 8 TeV with the ATLAS
             experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {1},
   Pages = {1-48},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2016)064},
   Abstract = {The cross-section for the production of a single top quark
             in association with a W boson in proton-proton collisions at
             √s = 8TeV is measured. The dataset corresponds to an
             integrated luminosity of 20.3 fb−1, collected by the ATLAS
             detector in 2012 at the Large Hadron Collider at CERN.
             Events containing two leptons and one central b-jet are
             selected. The W t signal is separated from the backgrounds
             using boosted decision trees, each of which combines a
             number of discriminating variables into one classifier.
             Production of W t events is observed with a significance of
             7.7σ. The cross-section is extracted in a profile
             likelihood fit to the classifier output distributions. The W
             t cross-section, inclusive of decay modes, is measured to be
             23.0 ± 1.3(stat.)− 3.5+ 3.2(syst.)±1.1(lumi.) pb. The
             measured cross-section is used to extract a value for the
             CKM matrix element |Vtb| of 1.01 ± 0.10 and a lower limit
             of 0.80 at the 95% confidence level. The cross-section for
             the production of a top quark and a W boson is also measured
             in a fiducial acceptance requiring two leptons with pT> 25
             GeV and |η| < 2.5, one jet with pT> 20 GeV and |η| < 2.5,
             and ETmiss > 20 GeV, including both W t and top-quark pair
             events as signal. The measured value of the fiducial
             cross-section is 0.85 ± 0.01(stat.)− 0.07+
             0.07(syst.)±0.03(lumi.) pb.},
   Doi = {10.1007/JHEP01(2016)064},
   Key = {fds316868}
}

@article{fds321396,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerny, K and Cerqueira,
             AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
             YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez
             Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
             H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
             Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
             V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Measurements of top-quark pair differential cross-sections
             in the lepton+jets channel in pp collisions at
             [Formula: see text] using the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {538},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4366-4},
   Abstract = {Measurements of normalized differential cross-sections of
             top-quark pair production are presented as a function of
             the top-quark, [Formula: see text] system and event-level
             kinematic observables in proton-proton collisions at
             a centre-of-mass energy of [Formula: see text]. The
             observables have been chosen to emphasize the [Formula: see
             text] production process and to be sensitive to effects of
             initial- and final-state radiation, to the different parton
             distribution functions, and to non-resonant processes and
             higher-order corrections. The dataset corresponds to an
             integrated luminosity of 20.3 fb[Formula: see text],
             recorded in 2012 with the ATLAS detector at the CERN Large
             Hadron Collider. Events are selected in the lepton+jets
             channel, requiring exactly one charged lepton and at least
             four jets with at least two of the jets tagged as
             originating from a <i>b</i>-quark. The measured spectra are
             corrected for detector effects and are compared to several
             Monte Carlo simulations. The results are in fair agreement
             with the predictions over a wide kinematic range.
             Nevertheless, most generators predict a harder top-quark
             transverse momentum distribution at high values than what is
             observed in the data. Predictions beyond NLO accuracy
             improve the agreement with data at high top-quark transverse
             momenta. Using the current settings and parton distribution
             functions, the rapidity distributions are not well modelled
             by any generator under consideration. However, the level of
             agreement is improved when more recent sets of parton
             distribution functions are used.},
   Doi = {10.1140/epjc/s10052-016-4366-4},
   Key = {fds321396}
}

@article{fds316161,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
             Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
             S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
             D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
             JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
             V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
             SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
             M},
   Title = {Search for supersymmetry at [Formula: see text] TeV in
             final states with jets and two same-sign leptons or three
             leptons with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {259},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4095-8},
   Abstract = {A search for strongly produced supersymmetric particles is
             conducted using signatures involving multiple energetic jets
             and either two isolated leptons (<i>e</i> or [Formula: see
             text]) with the same electric charge or at least three
             isolated leptons. The search also utilises <i>b</i>-tagged
             jets, missing transverse momentum and other observables to
             extend its sensitivity. The analysis uses a data sample of
             proton-proton collisions at [Formula: see text] TeV
             recorded with the ATLAS detector at the Large Hadron
             Collider in 2015 corresponding to a total integrated
             luminosity of 3.2 fb[Formula: see text]. No significant
             excess over the Standard Model expectation is observed. The
             results are interpreted in several simplified supersymmetric
             models and extend the exclusion limits from previous
             searches. In the context of exclusive production and
             simplified decay modes, gluino masses are excluded at
             [Formula: see text] confidence level up to 1.1-1.3 TeV for
             light neutralinos (depending on the decay channel), and
             bottom squark masses are also excluded up to 540 GeV. In the
             former scenarios, neutralino masses are also excluded up to
             550-850 GeV for gluino masses around 1 TeV.},
   Doi = {10.1140/epjc/s10052-016-4095-8},
   Key = {fds316161}
}

@article{fds321440,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Search for an additional, heavy Higgs boson in the [Formula:
             see text] decay channel at [Formula: see text] in [Formula:
             see text] collision data with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {45},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3820-z},
   Abstract = {A search is presented for a high-mass Higgs boson in the
             [Formula: see text], [Formula: see text], [Formula: see
             text], and [Formula: see text] decay modes using the ATLAS
             detector at the CERN Large Hadron Collider. The search uses
             proton-proton collision data at a centre-of-mass energy of
             8 TeV corresponding to an integrated luminosity of
             20.3 fb[Formula: see text]. The results of the search are
             interpreted in the scenario of a heavy Higgs boson with a
             width that is small compared with the experimental mass
             resolution. The Higgs boson mass range considered extends up
             to [Formula: see text] for all four decay modes and down to
             as low as 140 [Formula: see text], depending on the decay
             mode. No significant excess of events over the Standard
             Model prediction is found. A simultaneous fit to the four
             decay modes yields upper limits on the production
             cross-section of a heavy Higgs boson times the branching
             ratio to [Formula: see text] boson pairs. 95 % confidence
             level upper limits range from 0.53 pb at [Formula: see
             text] GeV to 0.008 pb at [Formula: see text] GeV for the
             gluon-fusion production mode and from 0.31 pb at [Formula:
             see text] GeV to 0.009 pb at [Formula: see text] GeV for
             the vector-boson-fusion production mode. The results are
             also interpreted in the context of Type-I and Type-II
             two-Higgs-doublet models.},
   Doi = {10.1140/epjc/s10052-015-3820-z},
   Key = {fds321440}
}

@article{fds321441,
   Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and CabreraUrbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace,
             N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
   Title = {Searches for scalar leptoquarks in pp collisions at
             [Formula: see text] = 8 TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Pages = {5},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-015-3823-9},
   Abstract = {Searches for pair-produced scalar leptoquarks are performed
             using 20 fb[Formula: see text] of proton-proton collision
             data provided by the LHC and recorded by the ATLAS detector
             at [Formula: see text] TeV. Events with two electrons
             (muons) and two or more jets in the final state are used to
             search for first (second)-generation leptoquarks. The
             results from two previously published ATLAS analyses are
             interpreted in terms of third-generation leptoquarks
             decaying to [Formula: see text] and [Formula: see text]
             final states. No statistically significant excess above the
             Standard Model expectation is observed in any channel and
             scalar leptoquarks are excluded at 95 % CL with masses up
             to [Formula: see text] 1050 GeV for first-generation
             leptoquarks, [Formula: see text] 1000 GeV for
             second-generation leptoquarks, [Formula: see text] 625 GeV
             for third-generation leptoquarks in the [Formula: see
             text] channel, and 200 [Formula: see text] 640 GeV in
             the [Formula: see text] channel.},
   Doi = {10.1140/epjc/s10052-015-3823-9},
   Key = {fds321441}
}

@article{fds321400,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for scalar leptoquarks in pp collisions at √S =
             13TeV with the ATLAS experiment},
   Journal = {New Journal of Physics},
   Volume = {18},
   Number = {9},
   Pages = {1-25},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1367-2630/18/9/093016},
   Abstract = {An inclusive search for a new-physics signature of
             lepton-jet resonances has been performed by the ATLAS
             experiment. Scalar leptoquarks, pair-produced in pp
             collisions at s √S13 TeV at the large hadron collider,
             have been considered. An integrated luminosity of 3.2
             fb−1, corresponding to the full 2015 dataset was used.
             First (second) generation leptoquarks were sought in events
             with two electrons (muons) and two or more jets. The
             observed event yield in each channel is consistent with
             Standard Model background expectations. The observed
             (expected) lower limits on the leptoquark mass at 95%
             confidence level are 1100 and 1050 GeV (1160 and 1040 GeV)
             for first and second generation leptoquarks, respectively,
             assuming a branching ratio into a charged lepton and a quark
             of 100%. Upper limits on the aforementioned branching ratio
             are also given as a function of leptoquark mass. Compared
             with the results of earlier ATLAS searches, the sensitivity
             is increased for leptoquark masses above 860 GeV, and the
             observed exclusion limits confirm and extend the published
             results.},
   Doi = {10.1088/1367-2630/18/9/093016},
   Key = {fds321400}
}

@article{fds323677,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
             SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
             K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
             A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
             T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
             S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
             JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
             Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
             Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
             MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Measurement of the differential cross-sections of prompt and
             non-prompt production of [Formula: see text] and [Formula:
             see text] in pp collisions at [Formula: see text] and
             8 TeV with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {283},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4050-8},
   Abstract = {The production rates of prompt and non-prompt [Formula: see
             text] and [Formula: see text] mesons in their dimuon decay
             modes are measured using 2.1 and 11.4 fb[Formula: see text]
             of data collected with the ATLAS experiment at the Large
             Hadron Collider, in proton-proton collisions at [Formula:
             see text] and 8 respectively. Production cross-sections for
             prompt as well as non-prompt sources, ratios of [Formula:
             see text] to [Formula: see text] production, and the
             fractions of non-prompt production for [Formula: see text]
             and [Formula: see text] are measured as a function of meson
             transverse momentum and rapidity. The measurements are
             compared to theoretical predictions.},
   Doi = {10.1140/epjc/s10052-016-4050-8},
   Key = {fds323677}
}

@article{fds321615,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
   Title = {Measurement of the charged-particle multiplicity inside jets
             from [Formula: see text][Formula: see text] pp
             collisions with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {6},
   Pages = {322},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4126-5},
   Abstract = {The number of charged particles inside jets is a widely used
             discriminant for identifying the quark or gluon nature of
             the initiating parton and is sensitive to both the
             perturbative and non-perturbative components of
             fragmentation. This paper presents a measurement of the
             average number of charged particles with [Formula: see text]
             [Formula: see text] inside high-momentum jets in dijet
             events using 20.3 fb[Formula: see text] of data recorded
             with the ATLAS detector in <i>pp</i> collisions at [Formula:
             see text] [Formula: see text] collisions at the LHC. The
             jets considered have transverse momenta from 50 [Formula:
             see text] up to and beyond 1.5 [Formula: see text]. The
             reconstructed charged-particle track multiplicity
             distribution is unfolded to remove distortions from detector
             effects and the resulting charged-particle multiplicity is
             compared to several models. Furthermore, quark and gluon jet
             fractions are used to extract the average charged-particle
             multiplicity for quark and gluon jets separately.},
   Doi = {10.1140/epjc/s10052-016-4126-5},
   Key = {fds321615}
}

@article{fds316873,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus,
             M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {Reconstruction of hadronic decay products of tau leptons
             with the ATLAS experiment.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {295},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4110-0},
   Abstract = {This paper presents a new method of reconstructing the
             individual charged and neutral hadrons in tau decays with
             the ATLAS detector. The reconstructed hadrons are used to
             classify the decay mode and to calculate the visible
             four-momentum of reconstructed tau candidates, significantly
             improving the resolution with respect to the calibration in
             the existing tau reconstruction. The performance of the
             reconstruction algorithm is optimised and evaluated using
             simulation and validated using samples of [Formula: see
             text] and [Formula: see text]+jets events selected from
             proton-proton collisions at a centre-of-mass energy
             [Formula: see text], corresponding to an integrated
             luminosity of 5 [Formula: see text].},
   Doi = {10.1140/epjc/s10052-016-4110-0},
   Key = {fds316873}
}

@article{fds321439,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
             M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
             C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
             NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
             D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
             I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
             J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
             CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
             A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
             A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
             JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
             S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
             G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
             K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Probing lepton flavour violation via neutrinoless [Formula:
             see text] decays with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {232},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4041-9},
   Abstract = {This article presents the sensitivity of the ATLAS
             experiment to the lepton-flavour-violating decays of
             [Formula: see text]. A method utilising the production of
             [Formula: see text] leptons via [Formula: see text] decays
             is used. This method is applied to the sample of
             20.3 fb[Formula: see text] of <i>pp</i> collision data at a
             centre-of-mass energy of 8 TeV collected by the ATLAS
             experiment at the LHC in 2012. No event is observed passing
             the selection criteria, and the observed (expected) upper
             limit on the [Formula: see text] lepton branching fraction
             into three muons, [Formula: see text], is [Formula: see
             text] ([Formula: see text]) at 90 % confidence
             level.},
   Doi = {10.1140/epjc/s10052-016-4041-9},
   Key = {fds321439}
}

@article{fds316874,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
   Title = {Measurement of the transverse momentum and [Formula: see
             text] distributions of Drell-Yan lepton pairs in
             proton-proton collisions at [Formula: see text] TeV with
             the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {291},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4070-4},
   Abstract = {Distributions of transverse momentum [Formula: see text] and
             the related angular variable [Formula: see text] of
             DrellΓÇôYan lepton pairs are measured in
             20.3 fb[Formula: see text] of proton–proton
             collisions at [Formula: see text] TeV with the ATLAS
             detector at the LHC. Measurements in electron-pair and
             muon-pair final states are corrected for detector effects
             and combined. Compared to previous measurements in
             protonΓÇôproton collisions at [Formula: see
             text] TeV, these new measurements benefit from a larger
             data sample and improved control of systematic
             uncertainties. Measurements are performed in bins of
             lepton-pair mass above, around and below the <i>Z</i>-boson
             mass peak. The data are compared to predictions from
             perturbative and resummed QCD calculations. For values of
             [Formula: see text] the predictions from the Monte Carlo
             generator ResBos are generally consistent with the data
             within the theoretical uncertainties. However, at larger
             values of [Formula: see text] this is not the case. Monte
             Carlo generators based on the parton-shower approach are
             unable to describe the data over the full range of [Formula:
             see text] while the fixed-order prediction of Dynnlo falls
             below the data at high values of [Formula: see text]. ResBos
             and the parton-shower Monte Carlo generators provide a much
             better description of the evolution of the [Formula: see
             text] and [Formula: see text] distributions as a function of
             lepton-pair mass and rapidity than the basic shape of the
             data.},
   Doi = {10.1140/epjc/s10052-016-4070-4},
   Key = {fds316874}
}

@article{fds316875,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
             Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
             M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
             MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
             I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
             JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
             I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
             E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
             Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
             S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
   Title = {Muon reconstruction performance of the ATLAS detector in
             proton-proton collision data at [Formula: see
             text]=13 TeV.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {292},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4120-y},
   Abstract = {This article documents the performance of the ATLAS muon
             identification and reconstruction using the LHC dataset
             recorded at [Formula: see text] TeV in 2015. Using a large
             sample of [Formula: see text] and [Formula: see text] decays
             from 3.2 fb[Formula: see text] of <i>pp</i> collision data,
             measurements of the reconstruction efficiency, as well as of
             the momentum scale and resolution, are presented and
             compared to Monte Carlo simulations. The reconstruction
             efficiency is measured to be close to [Formula: see text]
             over most of the covered phase space ([Formula: see text]
             and [Formula: see text] GeV). The isolation efficiency
             varies between 93 and [Formula: see text] depending on the
             selection applied and on the momentum of the muon. Both
             efficiencies are well reproduced in simulation. In the
             central region of the detector, the momentum resolution is
             measured to be [Formula: see text] ([Formula: see text]) for
             muons from [Formula: see text] ([Formula: see text]) decays,
             and the momentum scale is known with an uncertainty of
             [Formula: see text]. In the region [Formula: see text], the
             [Formula: see text] resolution for muons from [Formula: see
             text] decays is [Formula: see text] while the precision of
             the momentum scale for low-[Formula: see text] muons from
             [Formula: see text] decays is about [Formula: see
             text].},
   Doi = {10.1140/epjc/s10052-016-4120-y},
   Key = {fds316875}
}

@article{fds325770,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
             B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
             YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
             S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
             M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
             EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
             C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
             NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
             I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
             S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
             C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
             JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
             Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
             G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
             R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
             X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
             JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
   Title = {Search for new phenomena in different-flavour high-mass
             dilepton final states in pp collisions at [Formula:
             see text] Tev with the ATLAS detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {10},
   Pages = {541},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4385-1},
   Abstract = {A search is performed for a heavy particle decaying into
             different flavour dilepton pairs ([Formula: see text],
             [Formula: see text] or [Formula: see text]), using
             3.2 fb[Formula: see text] of proton-proton collision data
             at [Formula: see text] TeV collected in 2015 by the ATLAS
             detector at the Large Hadron Collider. No excess over the
             Standard Model prediction is observed. Limits at the 95 %
             credibility level are set on the mass of a [Formula: see
             text] boson with lepton-flavour-violating couplings at 3.0,
             2.7 and 2.6 TeV, and on the mass of a supersymmetric
             [Formula: see text] sneutrino with <i>R</i>-parity-violating
             couplings at 2.3, 2.2 and 1.9 TeV, for [Formula: see text],
             [Formula: see text] and [Formula: see text] final states,
             respectively. The results are also interpreted as limits on
             the threshold mass for quantum black hole
             production.},
   Doi = {10.1140/epjc/s10052-016-4385-1},
   Key = {fds325770}
}

@article{fds315798,
   Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
             F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos,
             S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
             G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
             Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
             P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
             N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
             AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
             R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
             Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
             FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
             MI and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
             L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
             H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
             JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
             N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
             HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
             D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
             F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
             H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
             P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho
             Toro, R and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa,
             A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
             V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
             B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavez
             Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
             E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
             IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Coggeshall, J and Cole, B and Cole, S and Colijn, AP and Collins-Tooth, C and Collot, J and Colombo,
             T},
   Title = {Measurement of the centrality dependence of the
             charged-particle pseudorapidity distribution in proton-lead
             collisions at [Formula: see text] TeV with the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {4},
   Pages = {199},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4002-3},
   Abstract = {The centrality dependence of the mean charged-particle
             multiplicity as a function of pseudorapidity is measured in
             approximately 1 [Formula: see text]b[Formula: see text] of
             proton-lead collisions at a nucleon-nucleon centre-of-mass
             energy of [Formula: see text] [Formula: see text] using the
             ATLAS detector at the Large Hadron Collider. Charged
             particles with absolute pseudorapidity less than 2.7 are
             reconstructed using the ATLAS pixel detector. The [Formula:
             see text] collision centrality is characterised by the total
             transverse energy measured in the Pb-going direction of the
             forward calorimeter. The charged-particle pseudorapidity
             distributions are found to vary strongly with centrality,
             with an increasing asymmetry between the proton-going and
             Pb-going directions as the collisions become more central.
             Three different estimations of the number of nucleons
             participating in the [Formula: see text] collision have been
             carried out using the Glauber model as well as two
             Glauber-Gribov inspired extensions to the Glauber model.
             Charged-particle multiplicities per participant pair are
             found to vary differently for these three models,
             highlighting the importance of including colour fluctuations
             in nucleon-nucleon collisions in the modelling of the
             initial state of [Formula: see text] collisions.},
   Doi = {10.1140/epjc/s10052-016-4002-3},
   Key = {fds315798}
}

@article{fds315800,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
             SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
             Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
             LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
             KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
             C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
             D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
             J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
             AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
             G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
             M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
             CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
             J},
   Title = {A new method to distinguish hadronically decaying boosted
             Z bosons from W bosons using the ATLAS
             detector.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {5},
   Pages = {238},
   Year = {2016},
   Month = {January},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4065-1},
   Abstract = {The distribution of particles inside hadronic jets produced
             in the decay of boosted <i>W</i> and <i>Z</i> bosons can be
             used to discriminate such jets from the continuum
             background. Given that a jet has been identified as likely
             resulting from the hadronic decay of a boosted <i>W</i> or
             <i>Z</i> boson, this paper presents a technique for further
             differentiating <i>Z</i> bosons from <i>W</i> bosons. The
             variables used are jet mass, jet charge, and a
             <i>b</i>-tagging discriminant. A likelihood tagger is
             constructed from these variables and tested in the
             simulation of [Formula: see text] for bosons in the
             transverse momentum range 200 GeV [Formula: see
             text] 400 GeV in [Formula: see text] TeV <i>pp</i>
             collisions with the ATLAS detector at the LHC. For
             <i>Z</i>-boson tagging efficiencies of [Formula: see text],
             50, and [Formula: see text], one can achieve [Formula: see
             text]-boson tagging rejection factors ([Formula: see text])
             of 1.7, 8.3 and 1000, respectively. It is not possible to
             measure these efficiencies in the data due to the lack of a
             pure sample of high [Formula: see text], hadronically
             decaying <i>Z</i> bosons. However, the modelling of the
             tagger inputs for boosted <i>W</i> bosons is studied in data
             using a [Formula: see text]-enriched sample of events in
             20.3 fb[Formula: see text] of data at [Formula: see text]
             TeV. The inputs are well modelled within uncertainties,
             which builds confidence in the expected tagger
             performance.},
   Doi = {10.1140/epjc/s10052-016-4065-1},
   Key = {fds315800}
}

@article{fds321425,
   Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
             MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
             EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
             Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
             Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
             NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
             De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
             JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
             L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
             IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
             TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
             M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
             L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
             DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
             J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
             M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
   Title = {Measurement of event-shape observables in [Formula: see
             text] events in pp collisions at [Formula: see
             text] [Formula: see text] with the ATLAS detector at the
             LHC.},
   Journal = {The European physical journal. C, Particles and
             fields},
   Volume = {76},
   Number = {7},
   Pages = {375},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-4176-8},
   Abstract = {Event-shape observables measured using charged particles in
             inclusive <i>Z</i>-boson events are presented, using the
             electron and muon decay modes of the <i>Z</i> bosons. The
             measurements are based on an integrated luminosity of
             [Formula: see text] of proton-proton collisions recorded by
             the ATLAS detector at the LHC at a centre-of-mass energy
             [Formula: see text] [Formula: see text]. Charged-particle
             distributions, excluding the lepton-antilepton pair from the
             <i>Z</i>-boson decay, are measured in different ranges of
             transverse momentum of the <i>Z</i> boson. Distributions
             include multiplicity, scalar sum of transverse momenta, beam
             thrust, transverse thrust, spherocity, and [Formula: see
             text]-parameter, which are in particular sensitive to
             properties of the underlying event at small values of the
             <i>Z</i>-boson transverse momentum. The measured observables
             are compared with predictions from Pythia 8, Sherpa, and
             Herwig 7. Typically, all three Monte Carlo generators
             provide predictions that are in better agreement with the
             data at high <i>Z</i>-boson transverse momenta than at low
             <i>Z</i>-boson transverse momenta, and for the observables
             that are less sensitive to the number of charged particles
             in the event.},
   Doi = {10.1140/epjc/s10052-016-4176-8},
   Key = {fds321425}
}

@article{fds321633,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of the correlation between the polar angles of
             leptons from top quark decays in the helicity basis at s =7
             T e V using the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {1},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.012002},
   Abstract = {A measurement of the correlations between the polar angles
             of leptons from the decay of pair-produced t and t¯ quarks
             in the helicity basis is reported, using proton-proton
             collision data collected by the ATLAS detector at the LHC.
             The dataset corresponds to an integrated luminosity of 4.6
             fb-1 at a center-of-mass energy of s=7 TeV collected during
             2011. Candidate events are selected in the dilepton topology
             with large missing transverse momentum and at least two
             jets. The angles θ1 and θ2 between the charged leptons and
             the direction of motion of the parent quarks in the tt¯
             rest frame are sensitive to the spin information, and the
             distribution of cosθ1·cosθ2 is sensitive to the spin
             correlation between the t and t¯ quarks. The distribution
             is unfolded to parton level and compared to the
             next-to-leading order prediction. A good agreement is
             observed.},
   Doi = {10.1103/PhysRevD.93.012002},
   Key = {fds321633}
}

@article{fds321634,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Search for invisible decays of a Higgs boson using
             vector-boson fusion in pp collisions at √s=8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {1},
   Pages = {1-44},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {January},
   url = {http://dx.doi.org/10.1007/JHEP01(2016)172},
   Abstract = {A search for a Higgs boson produced via vector-boson fusion
             and decaying into invisible particles is presented, using
             20.3 fb−1of proton-proton collision data at a
             centre-of-mass energy of 8 TeV recorded by the ATLAS
             detector at the LHC. For a Higgs boson with a mass of 125
             GeV, assuming the Standard Model production cross section,
             an upper bound of 0.28 is set on the branching fraction of H
             → invisible at 95% confidence level, where the expected
             upper limit is 0.31. The results are interpreted in models
             of Higgs-portal dark matter where the branching fraction
             limit is converted into upper bounds on the
             dark-matter-nucleon scattering cross section as a function
             of the dark-matter particle mass, and compared to results
             from the direct dark-matter detection experiments.},
   Doi = {10.1007/JHEP01(2016)172},
   Key = {fds321634}
}

@article{fds321626,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the production of single vector-like and excited
             quarks in the Wt final state in pp collisions at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {2},
   Pages = {1-46},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2016)110},
   Abstract = {A search for vector-like quarks and excited quarks in events
             containing a top quark and a W boson in the final state is
             reported here. The search is based on 20.3 fb−1 of
             proton-proton collision data taken at the LHC at a
             centre-of-mass energy of 8 TeV recorded by the ATLAS
             detector. Events with one or two leptons, and one, two or
             three jets are selected with the additional requirement that
             at least one jet contains a b-quark. Single-lepton events
             are also required to contain at least one large-radius jet
             from the hadronic decay of a high-pTW boson or a top quark.
             No significant excess over the expected background is
             observed and upper limits on the cross-section times
             branching ratio for different vector-like quark and
             excited-quark model masses are derived. For the
             excited-quark production and decay to Wt with unit
             couplings, quarks with masses below 1500 GeV are excluded
             and coupling-dependent limits are set.},
   Doi = {10.1007/JHEP02(2016)110},
   Key = {fds321626}
}

@article{fds321627,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {A search for prompt lepton-jets in pp collisions at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {2},
   Pages = {1-51},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1007/JHEP02(2016)062},
   Abstract = {Abstract: A search is presented for a new, light boson with
             a mass of about 1 GeV and decaying promptly to jets of
             collimated electrons and/or muons (lepton-jets). The
             analysis is performed with 20.3 fb−1 of data collected by
             the ATLAS detector at the Large Hadron Collider in
             proton-proton collisions at a centre-of-mass energy of 8
             TeV. Events are required to contain at least two
             lepton-jets. This study finds no statistically significant
             deviation from predictions of the Standard Model and places
             95% confidence-level upper limits on the contribution of new
             phenomena beyond the SM, incuding SUSY-portal and
             Higgs-portal models, on the number of events with
             lepton-jets.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP02(2016)062},
   Key = {fds321627}
}

@article{fds321625,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurements of four-lepton production in pp collisions at
             √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {753},
   Pages = {552-572},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1016/j.physletb.2015.12.048},
   Abstract = {The four-lepton (4ℓ, ℓ=e,μ) production cross section is
             measured in the mass range from 80 to 1000 GeV using 20.3
             fb−1 of data in pp collisions at s=8 TeV collected with
             the ATLAS detector at the LHC. The 4ℓ events are produced
             in the decays of resonant Z and Higgs bosons and the
             non-resonant ZZ continuum originating from qq¯, gg, and qg
             initial states. A total of 476 signal candidate events are
             observed with a background expectation of 26.2±3.6 events,
             enabling the measurement of the integrated cross section and
             the differential cross section as a function of the
             invariant mass and transverse momentum of the four-lepton
             system. In the mass range above 180 GeV, assuming the
             theoretical constraint on the qq¯ production cross section
             calculated with perturbative NNLO QCD and NLO electroweak
             corrections, the signal strength of the gluon-fusion
             component relative to its leading-order prediction is
             determined to be μgg=2.4±1.0 (stat.)±0.5 (syst.)±0.8
             (theory).},
   Doi = {10.1016/j.physletb.2015.12.048},
   Key = {fds321625}
}

@article{fds321628,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of the differential cross-section of highly
             boosted top quarks as a function of their transverse
             momentum in s =8 TeV proton-proton collisions using the
             ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.032009},
   Abstract = {The differential cross-section for pair production of top
             quarks with high transverse momentum is measured in 20.3
             fb-1 of proton-proton collisions at a center-of-mass energy
             of 8 TeV. The measurement is performed for tt¯ events in
             the lepton+jets channel. The cross-section is reported as a
             function of the hadronically decaying top quark transverse
             momentum for values above 300 GeV. The hadronically decaying
             top quark is reconstructed as an anti-kt jet with radius
             parameter R=1.0 and identified with jet substructure
             techniques. The observed yield is corrected for detector
             effects to obtain a cross-section at particle level in a
             fiducial region close to the event selection. A parton-level
             cross-section extrapolated to the full phase space is also
             reported for top quarks with transverse momentum above 300
             GeV. The predictions of a majority of next-to-leading-order
             and leading-order matrix-element Monte Carlo generators are
             found to agree with the measured cross-sections.},
   Doi = {10.1103/PhysRevD.93.032009},
   Key = {fds321628}
}

@article{fds315122,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Erratum to ATLAS Run 1 searches for direct pair production
             of third-generation squarks at the Large Hadron
             Collider},
   Journal = {European Physical Journal C},
   Volume = {76},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {March},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3935-x},
   Doi = {10.1140/epjc/s10052-016-3935-x},
   Key = {fds315122}
}

@article{fds315123,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Erratum to: Study of the spin and parity of the Higgs boson
             in diboson decays with the ATLAS detector},
   Journal = {European Physical Journal C},
   Volume = {76},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {March},
   ISSN = {1434-6044},
   url = {http://dx.doi.org/10.1140/epjc/s10052-016-3934-y},
   Doi = {10.1140/epjc/s10052-016-3934-y},
   Key = {fds315123}
}

@article{fds321624,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of jet charge in dijet events from s =8 TeV pp
             collisions with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052003},
   Abstract = {The momentum-weighted sum of the charges of tracks
             associated to a jet is sensitive to the charge of the
             initiating quark or gluon. This paper presents a measurement
             of the distribution of momentum-weighted sums, called jet
             charge, in dijet events using 20.3 fb-1 of data recorded
             with the ATLAS detector at s=8 TeV in pp collisions at the
             LHC. The jet charge distribution is unfolded to remove
             distortions from detector effects and the resulting
             particle-level distribution is compared with several models.
             The pT dependence of the jet charge distribution average and
             standard deviation are compared to predictions obtained with
             several leading-order and next-to-leading-order parton
             distribution functions. The data are also compared to
             different Monte Carlo simulations of QCD dijet production
             using various settings of the free parameters within these
             models. The chosen value of the strong coupling constant
             used to calculate gluon radiation is found to have a
             significant impact on the predicted jet charge. There is
             evidence for a pT dependence of the jet charge distribution
             for a given jet flavor. In agreement with perturbative QCD
             predictions, the data show that the average jet charge of
             quark-initiated jets decreases in magnitude as the energy of
             the jet increases.},
   Doi = {10.1103/PhysRevD.93.052003},
   Key = {fds321624}
}

@article{fds321622,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the electroweak production of supersymmetric
             particles in √s = 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052002},
   Abstract = {The ATLAS experiment has performed extensive searches for
             the electroweak production of charginos, neutralinos, and
             staus. This article summarizes and extends the search for
             electroweak supersymmetry with new analyses targeting
             scenarios not covered by previously published searches. New
             searches use vector-boson fusion production, initial-state
             radiation jets, and low-momentum lepton final states, as
             well as multivariate analysis techniques to improve the
             sensitivity to scenarios with small mass splittings and
             low-production cross sections. Results are based on 20 fb-1
             of proton-proton collision data at √s = 8 TeV recorded
             with the ATLAS experiment at the Large Hadron Collider. No
             significant excess beyond Standard Model expectations is
             observed. The new and existing searches are combined and
             interpreted in terms of 95% confidence-level exclusion
             limits in simplified models, where a single production
             process and decay mode is assumed, as well as within
             phenomenological supersymmetric models.},
   Doi = {10.1103/PhysRevD.93.052002},
   Key = {fds321622}
}

@article{fds321623,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Search for strong gravity in multijet final states produced
             in pp collisions at √s = 13 TeV using the ATLAS detector
             at the LHC},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2016)026},
   Abstract = {Abstract: A search is conducted for new physics in multijet
             final states using 3.6 inverse femtobarns of data from
             proton-proton collisions at (Formula presented.) TeV taken
             at the CERN Large Hadron Collider with the ATLAS detector.
             Events are selected containing at least three jets with
             scalar sum of jet transverse momenta (HT) greater than 1
             TeV. No excess is seen at large HTand limits are presented
             on new physics: models which produce final states containing
             at least three jets and having cross sections larger than
             1.6 fb with HT> 5.8 TeV are excluded. Limits are also given
             in terms of new physics models of strong gravity that
             hypothesize additional space-time dimensions.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP03(2016)026},
   Key = {fds321623}
}

@article{fds321621,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Search for new phenomena with photon+jet events in
             proton-proton collisions at √s = 13 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {3},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1007/JHEP03(2016)041},
   Abstract = {Abstract: A search is performed for the production of
             high-mass resonances decaying into a photon and a jet in 3.2
             fb−1of proton-proton collisions at a centre-of-mass energy
             of (Formula presented.) TeV collected by the ATLAS detector
             at the Large Hadron Collider. Selected events have an
             isolated photon and a jet, each with transverse momentum
             above 150 GeV. No significant deviation of the γ+jet
             invariant mass distribution from the background-only
             hypothesis is found. Limits are set at 95% confidence level
             on the cross sections of generic Gaussian-shaped signals and
             of a few benchmark phenomena beyond the Standard Model:
             excited quarks with vector-like couplings to the Standard
             Model particles, and non-thermal quantum black holes in two
             models of extra spatial dimensions. The minimum excluded
             visible cross sections for Gaussian-shaped resonances with
             width-to-mass ratios of 2% decrease from about 6 fb for a
             mass of 1.5 TeV to about 0.8 fb for a mass of 5 TeV. The
             minimum excluded visible cross sections for Gaussian-shaped
             resonances with width-to-mass ratios of 15% decrease from
             about 50 fb for a mass of 1.5 TeV to about 1.0 fb for a mass
             of 5 TeV. Excited quarks are excluded below masses of 4.4
             TeV, and non-thermal quantum black holes are excluded below
             masses of 3.8 (6.2) TeV for Randall-Sundrum
             (Arkani-Hamed-Dimopoulous-Dvali) models with one (six) extra
             dimensions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP03(2016)041},
   Key = {fds321621}
}

@article{fds320778,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O},
   Title = {Search for new phenomena in dijet mass and angular
             distributions from pp collisions at √s=13 TeV with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {754},
   Pages = {302-322},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.01.032},
   Abstract = {This Letter describes a model-agnostic search for pairs of
             jets (dijets) produced by resonant and non-resonant
             phenomena beyond the Standard Model in 3.6 fb−1 of
             proton–proton collisions with a centre-of-mass energy of
             s=13 TeV recorded by the ATLAS detector at the Large Hadron
             Collider. The distribution of the invariant mass of the two
             leading jets is examined for local excesses above a
             data-derived estimate of the smoothly falling prediction of
             the Standard Model. The data are also compared to a Monte
             Carlo simulation of Standard Model angular distributions
             derived from the rapidity of the two jets. No evidence of
             anomalous phenomena is observed in the data, which are used
             to exclude, at 95% CL, quantum black holes with threshold
             masses below 8.3 TeV, 8.1 TeV, or 5.1 TeV in three different
             benchmark scenarios; resonance masses below 5.2 TeV for
             excited quarks, 2.6 TeV in a W′ model, a range of masses
             starting from mZ′=1.5 TeV and couplings from gq=0.2 in a
             Z′ model; and contact interactions with a compositeness
             scale below 12.0 TeV and 17.5 TeV respectively for
             destructive and constructive interference between the new
             interaction and QCD processes. These results significantly
             extend the ATLAS limits obtained from 8 TeV data.
             Gaussian-shaped contributions to the mass distribution are
             also excluded if the effective cross-section exceeds values
             ranging from approximately 50–300 fb for masses below 2
             TeV to 2–20 fb for masses above 4 TeV.},
   Doi = {10.1016/j.physletb.2016.01.032},
   Key = {fds320778}
}

@article{fds321620,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Dijet production in √s=7 TeV pp collisions with large
             rapidity gaps at the ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {754},
   Pages = {214-234},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {March},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.01.028},
   Abstract = {A 6.8 nb−1 sample of pp collision data collected under
             low-luminosity conditions at s=7TeV by the ATLAS detector at
             the Large Hadron Collider is used to study diffractive dijet
             production. Events containing at least two jets with
             pT>20GeV are selected and analysed in terms of variables
             which discriminate between diffractive and non-diffractive
             processes. Cross sections are measured differentially in
             ΔηF, the size of the observable forward region of
             pseudorapidity which is devoid of hadronic activity, and in
             an estimator, ξ˜ of the fractional momentum loss of the
             proton assuming single diffractive dissociation (pp→pX).
             Model comparisons indicate a dominant non-diffractive
             contribution up to moderately large ΔηF and small ξ˜
             with a diffractive contribution which is significant at the
             highest ΔηF and the lowest ξ˜. The rapidity-gap survival
             probability is estimated from comparisons of the data in
             this latter region with predictions based on diffractive
             parton distribution functions.},
   Doi = {10.1016/j.physletb.2016.01.028},
   Key = {fds321620}
}

@article{fds315128,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for magnetic monopoles and stable particles with high
             electric charges in 8 TeV pp collisions with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {March},
   ISSN = {2470-0010},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.052009},
   Abstract = {A search for highly ionizing particles produced in
             proton-proton collisions at 8 TeV center-of-mass energy is
             performed by the ATLAS Collaboration at the CERN Large
             Hadron Collider. The data set used corresponds to an
             integrated luminosity of 7.0 fb-1. A customized trigger
             significantly increases the sensitivity, permitting a search
             for such particles with charges and energies beyond what was
             previously accessible. No events were found in the signal
             region, leading to production cross section upper limits in
             the mass range 200-2500 GeV for magnetic monopoles with
             magnetic charge in the range 0.5gD<|g|<2.0gD, where gD is
             the Dirac charge, and for stable particles with electric
             charge in the range 10<|z|<60. Model-dependent limits are
             presented in given pair-production scenarios, and
             model-independent limits are presented in fiducial regions
             of particle energy and pseudorapidity.},
   Doi = {10.1103/PhysRevD.93.052009},
   Key = {fds315128}
}

@article{fds316163,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
             IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
             A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
             J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
             V},
   Title = {Centrality, rapidity, and transverse momentum dependence of
             isolated prompt photon production in lead-lead collisions at
             sNN =2.76 TeV measured with the ATLAS detector},
   Journal = {Physical Review C},
   Volume = {93},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {March},
   ISSN = {2469-9985},
   url = {http://dx.doi.org/10.1103/PhysRevC.93.034914},
   Abstract = {Prompt photon production in sNN=2.76-TeV Pb+Pb collisions
             has been measured by the ATLAS experiment at the Large
             Hadron Collider using data collected in 2011 with an
             integrated luminosity of 0.14 nb-1. Inclusive photon yields,
             scaled by the mean nuclear thickness function, are presented
             as a function of collision centrality and transverse
             momentum in two pseudorapidity intervals, |η|<1.37 and
             1.52≤|η|<2.37. The scaled yields in the two
             pseudorapidity intervals, as well as the ratios of the
             forward yields to those at midrapidity, are compared to the
             expectations from next-to-leading-order perturbative QCD
             (pQCD) calculations. The measured cross sections agree well
             with the predictions for proton-proton collisions within
             statistical and systematic uncertainties. Both the yields
             and the ratios are also compared to two other pQCD
             calculations, one which uses the isospin content appropriate
             to colliding lead nuclei and another which includes nuclear
             modifications to the nucleon parton distribution
             functions.},
   Doi = {10.1103/PhysRevC.93.034914},
   Key = {fds316163}
}

@article{fds315124,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Amako and K and Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for anomalous couplings in the W tb vertex from the
             measurement of double differential angular decay rates of
             single top quarks produced in the t-channel with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {4},
   Pages = {1-46},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.1007/JHEP04(2016)023},
   Abstract = {Abstract: The electroweak production and subsequent decay of
             single top quarks is determined by the properties of the Wtb
             vertex. This vertex can be described by the complex
             parameters of an effective Lagrangian. An analysis of
             angular distributions of the decay products of single top
             quarks produced in the t -channel constrains these
             parameters simultaneously. The analysis described in this
             paper uses 4.6 fb−1 of proton-proton collision data at
             (Formula presented.) TeV collected with the ATLAS detector
             at the LHC. Two parameters are measured simultaneously in
             this analysis. The fraction f1 of decays containing
             transversely polarised W bosons is measured to be 0.37 ±
             0.07 (stat.⊕syst.). The phase δ− between amplitudes for
             transversely and longitudinally polarised W bosons recoiling
             against left-handed b-quarks is measured to be −0.014π ±
             0.036π (stat.⊕syst.). The correlation in the measurement
             of these parameters is 0.15. These values result in
             two-dimensional limits at the 95% confidence level on the
             ratio of the complex coupling parameters gR and VL, yielding
             Re[gR/VL] ∈ [−0.36, 0.10] and Im[gR/VL] ∈ [−0.17,
             0.23] with a correlation of 0.11. The results are in good
             agreement with the predictions of the Standard Model.[Figure
             not available: see fulltext.]},
   Doi = {10.1007/JHEP04(2016)023},
   Key = {fds315124}
}

@article{fds316865,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
             R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
             AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
             BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
             A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
             M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
             TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
             Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
             JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
             T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
             M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
             J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
             D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
             G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
             E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
             AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
             Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
             DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
             A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
             Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
             L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
             J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
             T},
   Title = {Observation of Long-Range Elliptic Azimuthal Anisotropies in
             sqrt[s]=13 and 2.76 TeV pp Collisions with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {116},
   Number = {17},
   Pages = {172301},
   Year = {2016},
   Month = {April},
   ISSN = {0031-9007},
   url = {http://dx.doi.org/10.1103/physrevlett.116.172301},
   Abstract = {ATLAS has measured two-particle correlations as a function
             of the relative azimuthal angle, Δϕ, and pseudorapidity,
             Δη, in sqrt[s]=13 and 2.76 TeV pp collisions at the LHC
             using charged particles measured in the pseudorapidity
             interval |η|<2.5. The correlation functions evaluated in
             different intervals of measured charged-particle
             multiplicity show a multiplicity-dependent enhancement at
             Δϕ∼0 that extends over a wide range of Δη, which has
             been referred to as the "ridge." Per-trigger-particle
             yields, Y(Δϕ), are measured over 2<|Δη|<5. For both
             collision energies, the Y(Δϕ) distribution in all
             multiplicity intervals is found to be consistent with a
             linear combination of the per-trigger-particle yields
             measured in collisions with less than 20 reconstructed
             tracks, and a constant combinatoric contribution modulated
             by cos(2Δϕ). The fitted Fourier coefficient, v_{2,2},
             exhibits factorization, suggesting that the ridge results
             from per-event cos(2ϕ) modulation of the single-particle
             distribution with Fourier coefficients v_{2}. The v_{2}
             values are presented as a function of multiplicity and
             transverse momentum. They are found to be approximately
             constant as a function of multiplicity and to have a p_{T}
             dependence similar to that measured in p+Pb and Pb+Pb
             collisions. The v_{2} values in the 13 and 2.76 TeV data
             are consistent within uncertainties. These results suggest
             that the ridge in pp collisions arises from the same or
             similar underlying physics as observed in p+Pb collisions,
             and that the dynamics responsible for the ridge has no
             strong sqrt[s] dependence.},
   Doi = {10.1103/physrevlett.116.172301},
   Key = {fds316865}
}

@article{fds316160,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Performance of b-jet identification in the ATLAS
             experiment},
   Journal = {Journal of Instrumentation},
   Volume = {11},
   Number = {4},
   Pages = {P04008-P04008},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1748-0221/11/04/P04008},
   Abstract = {The identification of jets containing b hadrons is important
             for the physics programme of the ATLAS experiment at the
             Large Hadron Collider. Several algorithms to identify jets
             containing b hadrons are described, ranging from those based
             on the reconstruction of an inclusive secondary vertex or
             the presence of tracks with large impact parameters to
             combined tagging algorithms making use of multi-variate
             discriminants. An independent b-tagging algorithm based on
             the reconstruction of muons inside jets as well as the
             b-tagging algorithm used in the online trigger are also
             presented. The b-jet tagging efficiency, the c-jet tagging
             efficiency and the mistag rate for light flavour jets in
             data have been measured with a number of complementary
             methods. The calibration results are presented as scale
             factors defined as the ratio of the efficiency (or mistag
             rate) in data to that in simulation. In the case of b jets,
             where more than one calibration method exists, the results
             from the various analyses have been combined taking into
             account the statistical correlation as well as the
             correlation of the sources of systematic
             uncertainty.},
   Doi = {10.1088/1748-0221/11/04/P04008},
   Key = {fds316160}
}

@article{fds321619,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Combination of searches for WW, WZ, and ZZ resonances in pp
             collisions at √s=8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {755},
   Pages = {285-305},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.02.015},
   Abstract = {The ATLAS experiment at the CERN Large Hadron Collider has
             performed searches for new, heavy bosons decaying to WW, WZ
             and ZZ final states in multiple decay channels using 20.3
             fb−1 of pp collision data at s=8 TeV. In the current
             study, the results of these searches are combined to provide
             a more stringent test of models predicting heavy resonances
             with couplings to vector bosons. Direct searches for a
             charged diboson resonance decaying to WZ in the
             ℓνℓ′ℓ′ (ℓ=μ,e), ℓℓqq¯ ℓνqq¯ and fully
             hadronic final states are combined and upper limits on the
             rate of production times branching ratio to the WZ bosons
             are compared with predictions of an extended gauge model
             with a heavy W′ boson. In addition, direct searches for a
             neutral diboson resonance decaying to WW and ZZ in the
             ℓℓqq¯ ℓνqq¯ and fully hadronic final states are
             combined and upper limits on the rate of production times
             branching ratio to the WW and ZZ bosons are compared with
             predictions for a heavy, spin-2 graviton in an extended
             Randall–Sundrum model where the Standard Model fields are
             allowed to propagate in the bulk of the extra
             dimension.},
   Doi = {10.1016/j.physletb.2016.02.015},
   Key = {fds321619}
}

@article{fds315799,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Search for dark matter produced in association with a Higgs
             boson decaying to two bottom quarks in pp collisions at s =8
             TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {7},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {April},
   ISSN = {2470-0010},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.072007},
   Abstract = {This article reports on a search for dark matter pair
             production in association with a Higgs boson decaying to a
             pair of bottom quarks, using data from 20.3 fb-1 of pp
             collisions at a center-of-mass energy of 8 TeV collected by
             the ATLAS detector at the LHC. The decay of the Higgs boson
             is reconstructed as a high-momentum bb system with either a
             pair of small-radius jets, or a single large-radius jet with
             substructure. The observed data are found to be consistent
             with the expected Standard Model backgrounds.
             Model-independent upper limits are placed on the visible
             cross sections for events with a Higgs boson decaying into
             bb and large missing transverse momentum with thresholds
             ranging from 150 to 400 GeV. Results are interpreted using a
             simplified model with a Z′ gauge boson decaying into
             different Higgs bosons predicted in a two-Higgs-doublet
             model, of which the heavy pseudoscalar Higgs decays into a
             pair of dark matter particles. Exclusion limits are also
             presented for the mass scales of various effective field
             theory operators that describe the interaction between dark
             matter particles and the Higgs boson.},
   Doi = {10.1103/PhysRevD.93.072007},
   Key = {fds315799}
}

@article{fds327376,
   Author = {Mindur, B and Åkesson, TPA and Anghinolfi, F and Antonov, A and Arslan,
             O and Baker, OK and Banas, E and Bault, C and Beddall, AJ and Bendotti, J and Benjamin, DP and Bertelsen, H and Bingul, A and Bocci, A and Boldyrev,
             AS and Brock, I and Capeáns Garrido and M and Catinaccio, A and Celebi, E and Cetin, SA and Choi, K and Dam, M and Danielsson, H and Davis, D and Degeorge, C and Derendarz, D and Desch, K and Di Girolamo and B and Dittus,
             F and Dixon, N and Dressnandt, N and Dubinin, FA and Evans, H and Farthouat, P and Fedin, OL and Froidevaux, D and Gavrilenko, IL and Gay,
             C and Gecse, Z and Godlewski, J and Grefe, C and Gurbuz, S and Hajduk, Z and Hance, M and Haney, B and Hansen, JB and Hansen, PH and Hawkins, AD and Heim, S and Holway, K and Kantserov, VA and Katounine, S and Kayumov, F and Keener, PT and Kisielewski, B and Klopov, NV and Konovalov, SP and Koperny, S and Korotkova, NA and Kowalski, TZ and Kramarenko, V and Krasnopevtsev, D and Kruse, M and Kudin, LG and Lichard, P and Loginov,
             A and Lorenzo Martinez and N and Lucotte, A and Luehring, F and Lytken, E and Maleev, VP and Maevskiy, AS and Manjarres Ramos and J and Mashinistov,
             RY and Meyer, C and Mialkovski, V and Mistry, K and Mitsou, VA and Nadtochi, AV and Newcomer, FM and Novodvorski, EG and Ogren, H and Oh,
             SH and Oleshko, SB and Olszowska, J and Ostrowicz, W and Palacino, G and Patrichev, S and Penwell, J and Perez-Gomez, F and Peshekhonov, VD and Røhne, O and Reilly, MB and Rembser, C and Ricken, O and Romaniouk, A and Rousseau, D and Ryjov, V and Sasmaz, U and Schaepe,
             S},
   Title = {Gas gain stabilisation in the ATLAS TRT detector},
   Journal = {Journal of Instrumentation},
   Volume = {11},
   Number = {4},
   Year = {2016},
   Month = {April},
   url = {http://dx.doi.org/10.1088/1748-0221/11/04/P04027},
   Abstract = {The ATLAS (one of two general purpose detectors at the LHC)
             Transition Radiation Tracker (TRT) is the outermost of the
             three tracking subsystems of the ATLAS Inner Detector. It is
             a large straw-based detector and contains about 350,000
             electronics channels. The performance of the TRT as tracking
             and particularly particle identification detector strongly
             depends on stability of the operation parameters with most
             important parameter being the gas gain which must be kept
             constant across the detector volume. The gas gain in the
             straws can vary significantly with atmospheric pressure,
             temperature, and gas mixture composition changes. This paper
             presents a concept of the gas gain stabilisation in the TRT
             and describes in detail the Gas Gain Stabilisation System
             (GGSS) integrated into the Detector Control System (DCS).
             Operation stability of the GGSS during Run-1 is
             demonstrated.},
   Doi = {10.1088/1748-0221/11/04/P04027},
   Key = {fds327376}
}

@article{fds329531,
   Author = {Adam, J and Adamová, D and Aggarwal, MM and Aglieri Rinella and G and Agnello, M and Agrawal, N and Ahammed, Z and Ahmad, S and Ahn, SU and Aiola, S and Akindinov, A and Alam, SN and Albuquerque, DSD and Aleksandrov, D and Alessandro, B and Alexandre, D and Alfaro Molina,
             R and Alici, A and Alkin, A and Almaraz, JRM and Alme, J and Alt, T and Altinpinar, S and Altsybeev, I and Alves Garcia Prado and C and Andrei,
             C and Andronic, A and Anguelov, V and Antičić, T and Antinori, F and Antonioli, P and Aphecetche, L and Appelshäuser, H and Arcelli, S and Arnaldi, R and Arnold, OW and Arsene, IC and Arslandok, M and Audurier,
             B and Augustinus, A and Averbeck, R and Azmi, MD and Badalà, A and Baek,
             YW and Bagnasco, S and Bailhache, R and Bala, R and Balasubramanian, S and Baldisseri, A and Baral, RC and Barbano, AM and Barbera, R and Barile,
             F and Barnaföldi, GG and Barnby, LS and Barret, V and Bartalini, P and Barth, K and Bartke, J and Bartsch, E and Basile, M and Bastid, N and Basu,
             S and Bathen, B and Batigne, G and Batista Camejo and A and Batyunya, B and Batzing, PC and Bearden, IG and Beck, H and Bedda, C and Behera, NK and Belikov, I and Bellini, F and Bello Martinez and H and Bellwied, R and Belmont, R and Belmont-Moreno, E and Belyaev, V and Benacek, P and Bencedi, G and Beole, S and Berceanu, I and Bercuci, A and Berdnikov, Y and Berenyi, D and Bertens, RA and Berzano, D and Betev, L and Bhasin, A and Bhat, IR and Bhati, AK and Bhattacharjee, B and Bhom, J and Bianchi, L and Bianchi, N and Bianchin, C and Bielčík, J and Bielčíková, J and Bilandzic, A},
   Title = {Particle identification in ALICE: a Bayesian
             approach},
   Journal = {European Physical Journal Plus},
   Volume = {131},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1140/epjp/i2016-16168-5},
   Abstract = {We present a Bayesian approach to particle identification
             (PID) within the ALICE experiment. The aim is to more
             effectively combine the particle identification capabilities
             of its various detectors. After a brief explanation of the
             adopted methodology and formalism, the performance of the
             Bayesian PID approach for charged pions, kaons and protons
             in the central barrel of ALICE is studied. PID is performed
             via measurements of specific energy loss (dE/dx) and time of
             flight. PID efficiencies and misidentification probabilities
             are extracted and compared with Monte Carlo simulations
             using high-purity samples of identified particles in the
             decay channels K0S→ π-π+}, ɸ → K-K+, and Λ → p π-
             in p-Pb collisions at √sNN=5.02 TeV. In order to
             thoroughly assess the validity of the Bayesian approach,
             this methodology was used to obtain corrected pT spectra of
             pions, kaons, protons, and D0 mesons in pp collisions at
             √s=7 TeV. In all cases, the results using Bayesian PID
             were found to be consistent with previous measurements
             performed by ALICE using a standard PID approach. For the
             measurement of D0 → K-π+, it was found that a Bayesian
             PID approach gave a higher signal-to-background ratio and a
             similar or larger statistical significance when compared
             with standard PID selections, despite a reduced
             identification efficiency. Finally, we present an
             exploratory study of the measurement of Λc+ → p K-π+ in
             pp collisions at √s=7 TeV, using the Bayesian approach for
             the identification of its decay products.},
   Doi = {10.1140/epjp/i2016-16168-5},
   Key = {fds329531}
}

@article{fds321438,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for the Standard Model Higgs boson decaying into bb¯
             produced in association with top quarks decaying
             hadronically in pp collisions at √s = 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {5},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1007/JHEP05(2016)160},
   Abstract = {A search for Higgs boson production in association with a
             pair of top quarks (tt¯ H) is performed, where the Higgs
             boson decays to bb¯, and both top quarks decay
             hadronically. The data used correspond to an integrated
             luminosity of 20.3 fb−1 of pp collisions at √s = 8 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider. The search selects events with at least six
             energetic jets and uses a boosted decision tree algorithm to
             discriminate between signal and Standard Model background.
             The dominant multijet background is estimated using a
             dedicated data-driven technique. For a Higgs boson mass of
             125 GeV, an upper limit of 6.4 (5.4) times the Standard
             Model cross section is observed (expected) at 95% confidence
             level. The best-fit value for the signal strength is μ =
             1.6 ± 2.6 times the Standard Model expectation for mH = 125
             GeV. Combining all tt¯ H searches carried out by ATLAS at
             √s = 8 and 7 TeV, an observed (expected) upper limit of
             3.1 (1.4) times the Standard Model expectation is obtained
             at 95% confidence level, with a signal strength μ = 1.7 ±
             0.8.},
   Doi = {10.1007/JHEP05(2016)160},
   Key = {fds321438}
}

@article{fds321617,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Measurement of the charge asymmetry in highly boosted
             top-quark pair production in √s=8 TeV pp collision data
             collected by the ATLAS experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {756},
   Pages = {52-71},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.02.055},
   Abstract = {In the pp→tt¯ process the angular distributions of top
             and anti-top quarks are expected to present a subtle
             difference, which could be enhanced by processes not
             included in the Standard Model. This Letter presents a
             measurement of the charge asymmetry in events where the
             top-quark pair is produced with a large invariant mass. The
             analysis is performed on 20.3 fb−1 of pp collision data at
             s=8TeV collected by the ATLAS experiment at the LHC, using
             reconstruction techniques specifically designed for the
             decay topology of highly boosted top quarks. The charge
             asymmetry in a fiducial region with large invariant mass of
             the top-quark pair (mtt¯>0.75 TeV) and an absolute rapidity
             difference of the top and anti-top quark candidates within
             −2<|yt|−|yt¯|<2 is measured to be 4.2±3.2%, in
             agreement with the Standard Model prediction at
             next-to-leading order. A differential measurement in three
             tt¯ mass bins is also presented.},
   Doi = {10.1016/j.physletb.2016.02.055},
   Key = {fds321617}
}

@article{fds321618,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of the dependence of transverse energy
             production at large pseudorapidity on the hard-scattering
             kinematics of proton–proton collisions at √s=2.76 TeV
             with ATLAS},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {756},
   Pages = {10-28},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.02.056},
   Abstract = {The relationship between jet production in the central
             region and the underlying-event activity in a
             pseudorapidity-separated region is studied in 4.0 pb−1 of
             s=2.76 TeV pp collision data recorded with the ATLAS
             detector at the LHC. The underlying event is characterised
             through measurements of the average value of the sum of the
             transverse energy at large pseudorapidity downstream of one
             of the protons, which are reported here as a function of
             hard-scattering kinematic variables. The hard scattering is
             characterised by the average transverse momentum and
             pseudorapidity of the two highest transverse momentum jets
             in the event. The dijet kinematics are used to estimate, on
             an event-by-event basis, the scaled longitudinal momenta of
             the hard-scattered partons in the target and projectile
             beam-protons moving toward and away from the region
             measuring transverse energy, respectively. Transverse energy
             production at large pseudorapidity is observed to decrease
             with a linear dependence on the longitudinal momentum
             fraction in the target proton and to depend only weakly on
             that in the projectile proton. The results are compared to
             the predictions of various Monte Carlo event generators,
             which qualitatively reproduce the trends observed in data
             but generally underpredict the overall level of transverse
             energy at forward pseudorapidity.},
   Doi = {10.1016/j.physletb.2016.02.056},
   Key = {fds321618}
}

@article{fds321616,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Evidence for single top-quark production in the s-channel in
             proton–proton collisions at √s=8 TeV with the ATLAS
             detector using the Matrix Element Method},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {756},
   Pages = {228-246},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.03.017},
   Abstract = {This Letter presents evidence for single top-quark
             production in the s-channel using proton–proton collisions
             at a centre-of-mass energy of 8 TeV with the ATLAS detector
             at the CERN Large Hadron Collider. The analysis is performed
             on events containing one isolated electron or muon, large
             missing transverse momentum and exactly two b-tagged jets in
             the final state. The analysed data set corresponds to an
             integrated luminosity of 20.3 fb−1. The signal is
             extracted using a maximum-likelihood fit of a discriminant
             which is based on the matrix element method and optimized in
             order to separate single-top-quark s-channel events from the
             main background contributions, which are top-quark pair
             production and W boson production in association with
             heavy-flavour jets. The measurement leads to an observed
             signal significance of 3.2 standard deviations and a
             measured cross-section of σs=4.8±0.8(stat.)−1.3+1.6(syst.)
             pb, which is consistent with the Standard Model expectation.
             The expected significance for the analysis is 3.9 standard
             deviations.},
   Doi = {10.1016/j.physletb.2016.03.017},
   Key = {fds321616}
}

@article{fds316872,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Measurements of W±Z production cross sections in pp
             collisions at s =8 TeV with the ATLAS detector and limits on
             anomalous gauge boson self-couplings},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {93},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {May},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.092004},
   Abstract = {This paper presents measurements of W±Z production in pp
             collisions at a center-of-mass energy of 8 TeV. The gauge
             bosons are reconstructed using their leptonic decay modes
             into electrons and muons. The data were collected in 2012 by
             the ATLAS experiment at the Large Hadron Collider and
             correspond to an integrated luminosity of 20.3 fb-1. The
             measured inclusive cross section in the detector fiducial
             region is σW±Z→ ′ν=35.1±0.9(stat)±0.8(sys)±0.8(lumi)
             fb, for one leptonic decay channel. In comparison, the
             next-to-leading-order Standard Model expectation is
             30.0±2.1 fb. Cross sections for W+Z and W-Z production and
             their ratio are presented as well as differential cross
             sections for several kinematic observables. Limits on
             anomalous triple gauge boson couplings are derived from the
             transverse mass spectrum of the W±Z system. From the
             analysis of events with a W and a Z boson associated with
             two or more forward jets an upper limit at 95% confidence
             level on the W±Z scattering cross section of 0.63 fb, for
             each leptonic decay channel, is established, while the
             Standard Model prediction at next-to-leading order is
             0.13±0.01 fb. Limits on anomalous quartic gauge boson
             couplings are also extracted.},
   Doi = {10.1103/PhysRevD.93.092004},
   Key = {fds316872}
}

@article{fds316871,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Search for the standard model Higgs boson produced in
             association with a vector boson and decaying into a tau pair
             in pp collisions at s =8 TeV with the ATLAS
             detector},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {93},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {May},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.092005},
   Abstract = {A search for the standard model Higgs boson produced in
             association with a vector boson with the decay H→ττ is
             presented. The data correspond to 20.3 fb-1 of integrated
             luminosity from proton-proton collisions at s=8 TeV recorded
             by the ATLAS experiment at the LHC during 2012. The data
             agree with the background expectation, and 95%
             confidence-level upper limits are placed on the cross
             section of this process. The observed (expected) limit,
             expressed in terms of the signal strength μ=σ/σSM for
             mH=125 GeV, is μ<5.6 (3.7). The measured value of the
             signal strength is μ=2.3±1.6.},
   Doi = {10.1103/PhysRevD.93.092005},
   Key = {fds316871}
}

@article{fds323676,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arduini, G and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Beam-induced and cosmic-ray backgrounds observed in the
             ATLAS detector during the LHC 2012 proton-proton running
             period},
   Journal = {Journal of Instrumentation},
   Volume = {11},
   Number = {5},
   Pages = {P05013-P05013},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1088/1748-0221/11/05/P05013},
   Abstract = {This paper discusses various observations on beam-induced
             and cosmic-ray backgrounds in the ATLAS detector during the
             LHC 2012 proton-proton run. Building on published results
             based on 2011 data, the correlations between background and
             residual pressure of the beam vacuum are revisited. Ghost
             charge evolution over 2012 and its role for backgrounds are
             evaluated. New methods to monitor ghost charge with beam-gas
             rates are presented and observations of LHC abort gap
             population by ghost charge are discussed in detail. Fake
             jets from colliding bunches and from ghost charge are
             analysed with improved methods, showing that ghost charge in
             individual radio-frequency buckets of the LHC can be
             resolved. Some results of two short periods of dedicated
             cosmic-ray background data-taking are shown; in particular
             cosmic-ray muon induced fake jet rates are compared to Monte
             Carlo simulations and to the fake jet rates from beam
             background. A thorough analysis of a particular LHC fill,
             where abnormally high background was observed, is presented.
             Correlations between backgrounds and beam intensity losses
             in special fills with very high β∗ are
             studied.},
   Doi = {10.1088/1748-0221/11/05/P05013},
   Key = {fds323676}
}

@article{fds321435,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Search for new phenomena in events with a photon and missing
             transverse momentum in pp collisions at √s = 13 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Pages = {1-41},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)059},
   Abstract = {Results of a search for new phenomena in events with an
             energetic photon and large missing transverse momentum with
             the ATLAS experiment at the Large Hadron Collider are
             reported. The data were collected in proton-proton
             collisions at a centre-of-mass energy of 13 TeV and
             correspond to an integrated luminosity of 3.2 fb−1. The
             observed data are in agreement with the Standard Model
             expectations. Exclusion limits are presented in models of
             new phenomena including pair production of dark matter
             candidates or large extra spatial dimensions. In a
             simplified model of dark matter and an axial-vector
             mediator, the search excludes mediator masses below 710 GeV
             for dark matter candidate masses below 150 GeV. In an
             effective theory of dark matter production, values of the
             suppression scale M∗ up to 570 GeV are excluded and the
             effect of truncation for various coupling values is
             reported. For the ADD large extra spatial dimension model
             the search places more stringent limits than earlier
             searches in the same event topology, excluding MD up to
             about 2.3 (2.8) TeV for two (six) additional spatial
             dimensions; the limits are reduced by 20-40% depending on
             the number of additional spatial dimensions when applying a
             truncation procedure.},
   Doi = {10.1007/JHEP06(2016)059},
   Key = {fds321435}
}

@article{fds321437,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Measurement of the relative width difference of the
             B0‐ B¯ 0 system with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)081},
   Abstract = {Abstract: This paper presents the measurement of the
             relative width difference ΔΓd/Γd of the B0‐ B¯ 0
             system using the data collected by the ATLAS experiment at
             the LHC in pp collisions at s=7 TeV and s=8 TeV and
             corresponding to an integrated luminosity of 25.2 fb−1.
             The value of ΔΓd/Γd is obtained by comparing the
             decay-time distributions of B0 → J/ψKS and B0 →
             J/ψK*0(892) decays. The result is ΔΓd/Γd = (−0.1±1.1
             (stat.)± 0.9 (syst.)) × 10−2. Currently, this is the
             most precise single measurement of ΔΓd/Γd. It agrees with
             the Standard Model prediction and the measurements by other
             experiments.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP06(2016)081},
   Key = {fds321437}
}

@article{fds321433,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {A search for top squarks with R-parity-violating decays to
             all-hadronic final states with the ATLAS detector in √s =
             8 TeV proton-proton collisions},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Pages = {1-49},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)067},
   Abstract = {A search for the pair production of top squarks, each with
             R-parity-violating decays into two Standard Model quarks, is
             performed using 17.4 fb−1 of √s = 8 TeV proton-proton
             collision data recorded by the ATLAS experiment at the LHC.
             Each top squark is assumed to decay to a b- and an s-quark,
             leading to four quarks in the final state. Background
             discrimination is achieved with the use of b-tagging and
             selections on the mass and substructure of large-radius
             jets, providing sensitivity to top squark masses as low as
             100 GeV. No evidence of an excess beyond the Standard Model
             background prediction is observed and top squarks decaying
             to b¯ s¯ are excluded for top squark masses in the range
             100 ≤ mt≤ 315 GeV at 95% confidence level.},
   Doi = {10.1007/JHEP06(2016)067},
   Key = {fds321433}
}

@article{fds316162,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
             J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
             B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Measurement of D⁎±, D± and
             Ds± meson production cross sections
             in pp collisions at √s=7 TeV with the ATLAS
             detector},
   Journal = {Nuclear Physics B},
   Volume = {907},
   Pages = {717-763},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {June},
   ISSN = {0550-3213},
   url = {http://dx.doi.org/10.1016/j.nuclphysb.2016.04.032},
   Abstract = {The production of D⁎±, D± and Ds± charmed mesons has
             been measured with the ATLAS detector in pp collisions at
             s=7 TeV at the LHC, using data corresponding to an
             integrated luminosity of 280 nb−1. The charmed mesons have
             been reconstructed in the range of transverse momentum
             3.5<pT(D)<100 GeV and pseudorapidity |η(D)|<2.1. The
             differential cross sections as a function of transverse
             momentum and pseudorapidity were measured for D⁎± and D±
             production. The next-to-leading-order QCD predictions are
             consistent with the data in the visible kinematic region
             within the large theoretical uncertainties. Using the
             visible D cross sections and an extrapolation to the full
             kinematic phase space, the strangeness-suppression factor in
             charm fragmentation, the fraction of charged non-strange D
             mesons produced in a vector state, and the total cross
             section of charm production at s=7 TeV were
             derived.},
   Doi = {10.1016/j.nuclphysb.2016.04.032},
   Key = {fds316162}
}

@article{fds329530,
   Author = {Adam, J and Adamová, D and Aggarwal, MM and Aglieri Rinella and G and Agnello, M and Agrawal, N and Ahammed, Z and Ahmad, S and Ahn, SU and Aiola, S and Akindinov, A and Alam, SN and Albuquerque, DSD and Aleksandrov, D and Alessandro, B and Alexandre, D and Alfaro Molina,
             R and Alici, A and Alkin, A and Almaraz, JRM and Alme, J and Alt, T and Altinpinar, S and Altsybeev, I and Alves Garcia Prado and C and Andrei,
             C and Andronic, A and Anguelov, V and Antičić, T and Antinori, F and Antonioli, P and Aphecetche, L and Appelshäuser, H and Arcelli, S and Arnaldi, R and Arnold, OW and Arsene, IC and Arslandok, M and Audurier,
             B and Augustinus, A and Averbeck, R and Azmi, MD and Badalà, A and Baek,
             YW and Bagnasco, S and Bailhache, R and Bala, R and Balasubramanian, S and Baldisseri, A and Baral, RC and Barbano, AM and Barbera, R and Barile,
             F and Barnaföldi, GG and Barnby, LS and Barret, V and Bartalini, P and Barth, K and Bartke, J and Bartsch, E and Basile, M and Bastid, N and Basu,
             S and Bathen, B and Batigne, G and Batista Camejo and A and Batyunya, B and Batzing, PC and Bearden, IG and Beck, H and Bedda, C and Behera, NK and Belikov, I and Bellini, F and Bello Martinez and H and Bellwied, R and Belmont, R and Belmont-Moreno, E and Belyaev, V and Bencedi, G and Beole, S and Berceanu, I and Bercuci, A and Berdnikov, Y and Berenyi, D and Bertens, RA and Berzano, D and Betev, L and Bhasin, A and Bhat, IR and Bhati, AK and Bhattacharjee, B and Bhom, J and Bianchi, L and Bianchi,
             N and Bianchin, C and Bielčík, J and Bielčíková, J and Bilandzic,
             A and Biro, G},
   Title = {Centrality dependence of ψ(2S) suppression in p-Pb
             collisions at √sNN= 5.02 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Pages = {1-23},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)050},
   Abstract = {The inclusive production of the ψ(2S) charmonium state was
             studied as a function of centrality in p-Pb collisions at
             the nucleon-nucleon center of mass energy √sNN = 5.02 TeV
             at the CERN LHC. The measurement was performed with the
             ALICE detector in the center of mass rapidity ranges −4.46
             < ycms< −2.96 and 2.03 < ycms< 3.53, down to zero
             transverse momentum, by reconstructing the ψ(2S) decay to a
             muon pair. The ψ(2S) production cross section σψ(2S) is
             presented as a function of the collision centrality, which
             is estimated through the energy deposited in forward
             rapidity calorimeters. The relative strength of nuclear
             effects on the ψ(2S) and on the corresponding 1S charmonium
             state J/ψ is then studied by means of the double ratio of
             cross sections [σψ(2S)/σJ/ψ]pPb/[σψ(2S)/σJ/ψ]pp
             between p-Pb and pp collisions, and by the values of the
             nuclear modification factors for the two charmonium states.
             The results show a large suppression of ψ(2S) production
             relative to the J/ψ at backward (negative) rapidity,
             corresponding to the flight direction of the Pb-nucleus,
             while at forward (positive) rapidity the suppressions of the
             two states are comparable. Finally, comparisons to results
             from lower energy experiments and to available theoretical
             models are presented.},
   Doi = {10.1007/JHEP06(2016)050},
   Key = {fds329530}
}

@article{fds321436,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {Identification of high transverse momentum top quarks in pp
             collisions at √s= 8 TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {6},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1007/JHEP06(2016)093},
   Abstract = {This paper presents studies of the performance of several
             jet-substructure techniques, which are used to identify
             hadronically decaying top quarks with high transverse
             momentum contained in large-radius jets. The efficiency of
             identifying top quarks is measured using a sample of
             top-quark pairs and the rate of wrongly identifying jets
             from other quarks or gluons as top quarks is measured using
             multijet events collected with the ATLAS experiment in 20.3
             fb−1of 8 TeV proton-proton collisions at the Large Hadron
             Collider. Predictions from Monte Carlo simulations are found
             to provide an accurate description of the performance. The
             techniques are compared in terms of signal efficiency and
             background rejection using simulations, covering a larger
             range in jet transverse momenta than accessible in the
             dataset. Additionally, a novel technique is developed that
             is optimized to reconstruct top quarks in events with many
             jets.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP06(2016)093},
   Key = {fds321436}
}

@article{fds321432,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Measurements of Zγ and Zγγ production in pp collisions at
             s =8 TeV with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112002},
   Abstract = {The production of Z bosons with one or two isolated
             high-energy photons is studied using pp collisions at s=8
             TeV. The analyses use a data sample with an integrated
             luminosity of 20.3 fb-1 collected by the ATLAS detector
             during the 2012 LHC data taking. The Zγ and Zγγ
             production cross sections are measured with leptonic (e+e-,
             μ+μ-, νν) decays of the Z boson, in extended fiducial
             regions defined in terms of the lepton and photon
             acceptance. They are then compared to cross-section
             predictions from the Standard Model, where the sources of
             the photons are radiation off initial-state quarks and
             radiative Z-boson decay to charged leptons, and from
             fragmentation of final-state quarks and gluons into photons.
             The yields of events with photon transverse energy ET>250
             GeV from +-γ events and with ET>400 GeV from ννγ events
             are used to search for anomalous triple gauge-boson
             couplings ZZγ and Zγγ. The yields of events with diphoton
             invariant mass mγγ>200 GeV from +-γγ events and with
             mγγ>300 GeV from ννγγ events are used to search for
             anomalous quartic gauge-boson couplings ZZγγ and Zγγγ.
             No deviations from Standard Model predictions are observed
             and limits are placed on parameters used to describe
             anomalous triple and quartic gauge-boson
             couplings.},
   Doi = {10.1103/PhysRevD.93.112002},
   Key = {fds321432}
}

@article{fds321429,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Measurement of the forward-backward asymmetry in low-mass
             bottom-quark pairs produced in proton-antiproton
             collisions},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112003},
   Abstract = {We report a measurement of the forward-backward asymmetry,
             AFB, in bb pairs produced in proton-antiproton collisions
             and identified by muons from semileptonic b-hadron decays.
             The event sample is collected at a center-of-mass energy of
             s=1.96 TeV with the CDF II detector and corresponds to 6.9
             fb-1 of integrated luminosity. We obtain an integrated
             asymmetry of AFB(bb)=(1.2±0.7)% at the particle level for
             b-quark pairs with invariant mass, mbb, down to 40 GeV/c2
             and measure the dependence of AFB(bb) on mbb. The results
             are compatible with expectations from the standard
             model.},
   Doi = {10.1103/PhysRevD.93.112003},
   Key = {fds321429}
}

@article{fds321430,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Measurement of the forward-backward asymmetry of top-quark
             and antiquark pairs using the full CDF Run II data
             set},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112005},
   Abstract = {We measure the forward-backward asymmetry of the production
             of top-quark and antiquark pairs in proton-antiproton
             collisions at center-of-mass energy s=1.96 TeV using the
             full data set collected by the Collider Detector at Fermilab
             (CDF) in Tevatron Run II corresponding to an integrated
             luminosity of 9.1 fb-1. The asymmetry is characterized by
             the rapidity difference between top quarks and antiquarks
             (Δy) and measured in the final state with two charged
             leptons (electrons and muons). The inclusive asymmetry,
             corrected to the entire phase space at parton level, is
             measured to be AFBtt=0.12±0.13, consistent with the
             expectations from the standard model (SM) and previous CDF
             results in the final state with a single charged lepton. The
             combination of the CDF measurements of the inclusive AFBtt
             in both final states yields AFBtt=0.160±0.045, which is
             consistent with the SM predictions. We also measure the
             differential asymmetry as a function of Δy. A linear fit to
             AFBtt(|Δy|), assuming zero asymmetry at Δy=0, yields a
             slope of α=0.14±0.15, consistent with the SM prediction
             and the previous CDF determination in the final state with a
             single charged lepton. The combined slope of AFBtt(|Δy|) in
             the two final states is α=0.227±0.057, which is 2.0σ
             larger than the SM prediction.},
   Doi = {10.1103/PhysRevD.93.112005},
   Key = {fds321430}
}

@article{fds315125,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
             PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O and Artamonov, A},
   Title = {Search for new phenomena in final states with large jet
             multiplicities and missing transverse momentum with ATLAS
             using √s=13 TeV proton–proton collisions},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {757},
   Pages = {334-355},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {June},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.04.005},
   Abstract = {Results are reported of a search for new phenomena, such as
             supersymmetric particle production, that could be observed
             in high-energy proton–proton collisions. Events with large
             numbers of jets, together with missing transverse momentum
             from unobserved particles, are selected. The data analysed
             were recorded by the ATLAS experiment during 2015 using the
             13 TeV centre-of-mass proton–proton collisions at the
             Large Hadron Collider, and correspond to an integrated
             luminosity of 3.2 fb−1. The search selected events with
             various jet multiplicities from ≥7 to ≥10 jets, and with
             various b-jet multiplicity requirements to enhance
             sensitivity. No excess above Standard Model expectations is
             observed. The results are interpreted within two
             supersymmetry models, where gluino masses up to 1400 GeV are
             excluded at 95% confidence level, significantly extending
             previous limits.},
   Doi = {10.1016/j.physletb.2016.04.005},
   Key = {fds315125}
}

@article{fds321428,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Search for a low-mass neutral Higgs boson with suppressed
             couplings to fermions using events with multiphoton final
             states},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112010},
   Abstract = {A search for a Higgs boson with suppressed couplings to
             fermions, hf, assumed to be the neutral, lower-mass partner
             of the Higgs boson discovered at the Large Hadron Collider,
             is reported. Such a Higgs boson could exist in extensions of
             the standard model with two Higgs doublets, and could be
             produced via pp→H±hf→W∗hfhf→4γ+X, where H± is a
             charged Higgs boson. This analysis uses all events with at
             least three photons in the final state from
             proton-antiproton collisions at a center-of-mass energy of
             1.96 TeV collected by the Collider Detector at Fermilab,
             corresponding to an integrated luminosity of 9.2 fb-1. No
             evidence of a signal is observed in the data. Values of
             Higgs-boson masses between 10 and 100 GeV/c2 are excluded at
             95% Bayesian credibility.},
   Doi = {10.1103/PhysRevD.93.112010},
   Key = {fds321428}
}

@article{fds321431,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
             G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
             N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
             JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
             K and Edgar, R and Erbacher, R and Errede, S and Esham,
             B},
   Title = {Measurement of sin2 θefflept
             using e+e- pairs from γ/Z bosons produced in
             pp collisions at a center-of-momentum energy of 1.96
             TeV},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112016},
   Abstract = {At the Fermilab Tevatron proton-antiproton (pp) collider,
             Drell-Yan lepton pairs are produced in the process
             pp→e+e-+X through an intermediate γ∗/Z boson. The
             forward-backward asymmetry in the polar-angle distribution
             of the e- as a function of the e+e - pair mass is used to
             obtain sin2θefflept, the effective leptonic determination
             of the electroweak-mixing parameter sin2θW. The measurement
             sample, recorded by the Collider Detector at Fermilab (CDF),
             corresponds to 9.4 fb-1 of integrated luminosity from pp
             collisions at a center-of-momentum energy of 1.96 TeV, and
             is the full CDF Run II data set. The value of sin2θefflept
             is found to be 0.23248±0.00053. The combination with the
             previous CDF measurement based on μ+μ- pairs yields
             sin2θefflept=0.23221±0.00046. This result, when
             interpreted within the specified context of the standard
             model assuming sin2θW=1-MW2/MZ2 and that the W- and Z-boson
             masses are on-shell, yields sin2θW=0.22400±0.00045, or
             equivalently a W-boson mass of 80.328±0.024
             GeV/c2.},
   Doi = {10.1103/PhysRevD.93.112016},
   Key = {fds321431}
}

@article{fds321434,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for metastable heavy charged particles with large
             ionization energy loss in pp collisions at s =13 TeV using
             the ATLAS experiment},
   Journal = {Physical Review D},
   Volume = {93},
   Number = {11},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {June},
   url = {http://dx.doi.org/10.1103/PhysRevD.93.112015},
   Abstract = {This paper presents a search for massive charged long-lived
             particles produced in pp collisions at s=13 TeV at the LHC
             using the ATLAS experiment. The data set used corresponds to
             an integrated luminosity of 3.2 fb-1. Many extensions of the
             Standard Model predict the existence of massive charged
             long-lived particles, such as R-hadrons. These massive
             particles are expected to be produced with a velocity
             significantly below the speed of light, and therefore to
             have a specific ionization higher than any Standard Model
             particle of unit charge at high momenta. The Pixel subsystem
             of the ATLAS detector is used to measure the ionization
             energy loss of reconstructed charged particles and to search
             for such highly ionizing particles. The search presented
             here has much greater sensitivity than a similar search
             performed using the ATLAS detector in the s=8 TeV data set,
             thanks to the increase in expected signal cross section due
             to the higher center-of-mass energy of collisions, to an
             upgraded detector with a new silicon layer close to the
             interaction point, and to analysis improvements. No
             significant deviation from Standard Model background
             expectations is observed, and lifetime-dependent upper
             limits on R-hadron production cross sections and masses are
             set. Gluino R-hadrons with lifetimes above 0.4 ns and
             decaying to qq plus a 100 GeV neutralino are excluded at the
             95% confidence level, with lower mass limit ranging between
             740 and 1590 GeV. In the case of stable R-hadrons the lower
             mass limit at the 95% confidence level is 1570
             GeV.},
   Doi = {10.1103/PhysRevD.93.112015},
   Key = {fds321434}
}

@article{fds321424,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
   Title = {A search for an excited muon decaying to a muon and two jets
             in pp collisions at √ s = 8 TeV with the ATLAS
             detector},
   Journal = {New Journal of Physics},
   Volume = {18},
   Number = {7},
   Pages = {073021-073021},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {July},
   url = {http://dx.doi.org/10.1088/1367-2630/18/7/073021},
   Abstract = {Anew search signature for excited leptons is explored.
             Excited muons are sought in the channel pp → μμ∗→
             μμ jet jet, assuming both the production and decay occur
             via a contact interaction. The analysis is based on 20.3
             fb-1 of pp collision data at a centre-of-mass energy of s =
             8 TeV taken with the ATLAS detector at the large hadron
             collider. No evidence of excited muons is found, and limits
             are set at the 95% confidence level on the cross section
             times branching ratio as a function of the excited-muonmass
             μμ∗. For μμ∗between 1.3 and 3.0 TeV, the upper limit
             on φB (μ∗→ μqq) is between 0.6 and 1 fb. Limits on sB
             are converted to lower bounds on the compositeness scale. In
             the limiting case L = μμ∗, excitedmuonswith amass
             below2.8 TeVare excluded.With the samemodel assumptions,
             these limits at larger μ∗masses improve upon previous
             limits fromtraditional searches based on the gauge-mediated
             decay μ∗→ μγ.},
   Doi = {10.1088/1367-2630/18/7/073021},
   Key = {fds321424}
}

@article{fds316164,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M and Arslan, O},
   Title = {Search for single production of a vector-like quark via a
             heavy gluon in the 4b final state with the ATLAS detector in
             pp collisions at s=8 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {758},
   Pages = {249-268},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {July},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.04.061},
   Abstract = {A search is performed for the process pp→G*→BHb-/B-Hb→Hbb-→bb-bb-,
             predicted in composite Higgs scenarios, where G* is a heavy
             colour octet vector resonance and BH a vector-like quark of
             charge -1/3. The data were obtained from pp collisions at a
             centre-of-mass energy of 8 TeV corresponding to an
             integrated luminosity of 19.5 fb-1, recorded by the ATLAS
             detector at the LHC. The largest background, multijet
             production, is estimated using a data-driven method. No
             significant excess of events with respect to Standard Model
             predictions is observed, and upper limits on the production
             cross section times branching ratio are set. Comparisons to
             the predictions from a specific benchmark model are made,
             resulting in lower mass limits in the two-dimensional mass
             plane of mG* vs. mBH.},
   Doi = {10.1016/j.physletb.2016.04.061},
   Key = {fds316164}
}

@article{fds315801,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Charged-particle distributions in √s=13 TeV pp
             interactions measured with the ATLAS detector at the
             LHC},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {758},
   Pages = {67-88},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {July},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.04.050},
   Abstract = {Charged-particle distributions are measured in
             proton–proton collisions at a centre-of-mass energy of 13
             TeV, using a data sample of nearly 9 million events,
             corresponding to an integrated luminosity of 170 μb−1,
             recorded by the ATLAS detector during a special Large Hadron
             Collider fill. The charged-particle multiplicity, its
             dependence on transverse momentum and pseudorapidity and the
             dependence of the mean transverse momentum on the
             charged-particle multiplicity are presented. The
             measurements are performed with charged particles with
             transverse momentum greater than 500 MeV and absolute
             pseudorapidity less than 2.5, in events with at least one
             charged particle satisfying these kinematic requirements.
             Additional measurements in a reduced phase space with
             absolute pseudorapidity less than 0.8 are also presented, in
             order to compare with other experiments. The results are
             corrected for detector effects, presented as particle-level
             distributions and are compared to the predictions of various
             Monte Carlo event generators.},
   Doi = {10.1016/j.physletb.2016.04.050},
   Key = {fds315801}
}

@article{fds321416,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
             BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
             F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Measurement of fiducial differential cross sections of
             gluon-fusion production of Higgs bosons decaying to WW
             →eνμν with the ATLAS detector at √s=8
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)104},
   Abstract = {This paper describes a measurement of fiducial and
             differential cross sections of gluon-fusion Higgs boson
             production in the H → W W∗→ eνμν channel, using
             20.3 fb−1 of proton-proton collision data. The data were
             produced at a centre-of-mass energy of s=8 TeV at the CERN
             Large Hadron Collider and recorded by the ATLAS detector in
             2012. Cross sections are measured from the observed H→ W
             W∗→ eνμν signal yield in categories distinguished by
             the number of associated jets. The total cross section is
             measured in a fiducial region defined by the kinematic
             properties of the charged leptons and neutrinos.
             Differential cross sections are reported as a function of
             the number of jets, the Higgs boson transverse momentum, the
             dilepton rapidity, and the transverse momentum of the
             leading jet. The jet-veto efficiency, or fraction of events
             with no jets above a given transverse momentum threshold, is
             also reported. All measurements are compared to QCD
             predictions from Monte Carlo generators and fixed-order
             calculations, and are in agreement with the Standard Model
             predictions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)104},
   Key = {fds321416}
}

@article{fds321421,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
             A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
   Title = {Measurement of the CP-violating phase ϕsand the
             Bs0meson decay width difference with
             Bs0→ J/ψϕ decays in
             ATLAS},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)147},
   Abstract = {A measurement of the Bs0decay parameters in the Bs0→
             J/ψϕ channel using an integrated luminosity of 14.3
             fb−1collected by the ATLAS detector from 8 TeV pp
             collisions at the LHC is presented. The measured parameters
             include the CP -violating phase ϕs, the decay width Γs and
             the width difference between the mass eigenstates ΔΓs. The
             values measured for the physical parameters are
             statistically combined with those from 4.9 fb−1of 7 TeV
             data, leading to the following: Φs = -0.090 ± 0.078
             (stat.) ± (syst.) rad Δ Γs = 0.085 ± 0.011 (stat.) ±
             0.007 (syst.) Ps-1 Δ Γs = 0.675 ± 0.003 (stat.) ± 0.03
             (syst.) Ps-1 In the analysis the parameter ΔΓs is
             constrained to be positive. Results for ϕs and ΔΓs are
             also presented as 68% and 95% likelihood contours in the
             ϕs-ΔΓs plane. Also measured in this decay channel are the
             transversity amplitudes and corresponding strong phases. All
             measurements are in agreement with the Standard Model
             predictions.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)147},
   Key = {fds321421}
}

@article{fds321422,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Measurement of the angular coefficients in Z-boson events
             using electron and muon pairs from data taken at √s = 8
             TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)159},
   Abstract = {The angular distributions of Drell-Yan charged lepton pairs
             in the vicinity of the Z-boson mass peak probe the
             underlying QCD dynamics of Z-boson production. This paper
             presents a measurement of the complete set of angular
             coefficients A0−7 describing these distributions in the
             Z-boson Collins-Soper frame. The data analysed correspond to
             20.3 fb−1 of pp collisions at s=8 TeV, collected by the
             ATLAS detector at the CERN LHC. The measurements are
             compared to the most precise fixed-order calculations
             currently available (O(αs2)) and with theoretical
             predictions embedded in Monte Carlo generators. The
             measurements are precise enough to probe QCD corrections
             beyond the formal accuracy of these calculations and to
             provide discrimination between different parton-shower
             models. A significant deviation from the (O(αs2))
             predictions is observed for A0 − A2. Evidence is found for
             non-zero A5,6,7, consistent with expectations.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)159},
   Key = {fds321422}
}

@article{fds321413,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Measurement of the double-differential high-mass Drell-Yan
             cross section in pp collisions at √s = 8 TeV with the
             ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)009},
   Abstract = {This paper presents a measurement of the double-differential
             cross section for the Drell-Yan Z/γ∗ → ℓ+ℓ− and
             photon-induced γγ → ℓ+ℓ− processes where ℓ is an
             electron or muon. The measurement is performed for invariant
             masses of the lepton pairs, mℓℓ, between 116 GeV and
             1500 GeV using a sample of 20.3 fb−1 of pp collisions data
             at centre-of-mass energy of s=8 TeV collected by the ATLAS
             detector at the LHC in 2012. The data are presented double
             differentially in invariant mass and absolute dilepton
             rapidity as well as in invariant mass and absolute
             pseudorapidity separation of the lepton pair. The
             single-differential cross section as a function of mℓℓ
             is also reported. The electron and muon channel measurements
             are combined and a total experimental precision of better
             than 1% is achieved at low mℓℓ. A comparison to
             next-to-next-to-leading order perturbative QCD predictions
             using several recent parton distribution functions and
             including next-to-leading order electroweak effects
             indicates the potential of the data to constrain parton
             distribution functions. In particular, a large impact of the
             data on the photon PDF is demonstrated.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP08(2016)009},
   Key = {fds321413}
}

@article{fds321414,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
             C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
             H},
   Title = {Measurement of the inclusive isolated prompt photon cross
             section in pp collisions at s=8TeV with the ATLAS
             detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)005},
   Abstract = {Abstract: A measurement of the cross section for the
             inclusive production of isolated prompt photons in
             proton-proton collisions at a centre-of-mass energy of s=8
             TeV is presented. The measurement covers the pseudorapidity
             ranges |ηγ | < 1.37 and 1.56 ≤ |ηγ | < 2.37 in the
             transverse energy range 25 < ETγ < 1500 GeV. The results
             are based on an integrated luminosity of 20.2 fb−1,
             recorded by the ATLAS detector at the LHC. Photon candidates
             are identified by combining information from the
             calorimeters and the inner tracker. The background is
             subtracted using a data-driven technique, based on the
             observed calorimeter shower-shape variables and the
             deposition of hadronic energy in a narrow cone around the
             photon candidate. The measured cross sections are compared
             with leading-order and next-to-leading order perturbative
             QCD calculations and are found to be in a good agreement
             over ten orders of magnitude.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP08(2016)005},
   Key = {fds321414}
}

@article{fds321417,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
             A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
             M},
   Title = {Measurements of the Higgs boson production and decay rates
             and constraints on its couplings from a combined ATLAS and
             CMS analysis of the LHC pp collision data at √s = 7 and 8
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)045},
   Abstract = {Combined ATLAS and CMS measurements of the Higgs boson
             production and decay rates, as well as constraints on its
             couplings to vector bosons and fermions, are presented. The
             combination is based on the analysis of five production
             processes, namely gluon fusion, vector boson fusion, and
             associated production with a W or a Z boson or a pair of top
             quarks, and of the six decay modes H → ZZ, W W, γγ,
             ττ, bb, and μμ. All results are reported assuming a
             value of 125.09 GeV for the Higgs boson mass, the result of
             the combined measurement by the ATLAS and CMS experiments.
             The analysis uses the CERN LHC proton-proton collision data
             recorded by the ATLAS and CMS experiments in 2011 and 2012,
             corresponding to integrated luminosities per experiment of
             approximately 5 fb−1 at √s = 7 TeV and 20 fb−1 at √s
             = 8 TeV. The Higgs boson production and decay rates measured
             by the two experiments are combined within the context of
             three generic parameterisations: two based on cross sections
             and branching fractions, and one on ratios of coupling
             modifiers. Several interpretations of the measurements with
             more model-dependent parameterisations are also given. The
             combined signal yield relative to the Standard Model
             prediction is measured to be 1.09 ± 0.11. The combined
             measurements lead to observed significances for the vector
             boson fusion production process and for the H → ττ decay
             of 5.4 and 5.5 standard deviations, respectively. The data
             are consistent with the Standard Model predictions for all
             parameterisations considered.},
   Doi = {10.1007/JHEP08(2016)045},
   Key = {fds321417}
}

@article{fds329529,
   Author = {Adam, J and Adamová, D and Aggarwal, MM and Aglieri Rinella and G and Agnello, M and Agrawal, N and Ahammed, Z and Ahn, SU and Aiola, S and Akindinov, A and Alam, SN and Aleksandrov, D and Alessandro, B and Alexandre, D and Alfaro Molina and R and Alici, A and Alkin, A and Almaraz,
             JRM and Alme, J and Alt, T and Altinpinar, S and Altsybeev, I and Alves
             Garcia Prado and C and Andrei, C and Andronic, A and Anguelov, V and Anielski, J and Antičić, T and Antinori, F and Antonioli, P and Aphecetche, L and Appelshäuser, H and Arcelli, S and Arnaldi, R and Arnold, OW and Arsene, IC and Arslandok, M and Audurier, B and Augustinus, A and Averbeck, R and Azmi, MD and Badalà, A and Baek, YW and Bagnasco, S and Bailhache, R and Bala, R and Balasubramanian, S and Baldisseri, A and Baral, RC and Barbano, AM and Barbera, R and Barile,
             F and Barnaföldi, GG and Barnby, LS and Barret, V and Bartalini, P and Barth, K and Bartke, J and Bartsch, E and Basile, M and Bastid, N and Basu,
             S and Bathen, B and Batigne, G and Batista Camejo and A and Batyunya, B and Batzing, PC and Bearden, IG and Beck, H and Bedda, C and Behera, NK and Belikov, I and Bellini, F and Bello Martinez and H and Bellwied, R and Belmont, R and Belmont-Moreno, E and Belyaev, V and Benacek, P and Bencedi, G and Beole, S and Berceanu, I and Bercuci, A and Berdnikov, Y and Berenyi, D and Bertens, RA and Berzano, D and Betev, L and Bhasin, A and Bhat, IR and Bhati, AK and Bhattacharjee, B and Bhom, J and Bianchi, L and Bianchi, N and Bianchin, C and Bielčík, J and Bielčíková, J and Bilandzic, A and Biro, G},
   Title = {Measurement of D-meson production versus multiplicity in
             p-Pb collisions at √sNN=5.02 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {8},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1007/JHEP08(2016)078},
   Abstract = {The measurement of prompt D-meson production as a function
             of multiplicity in p-Pb collisions at sNN=5.02 TeV with the
             ALICE detector at the LHC is reported. D0, D+ and D∗+
             mesons are reconstructed via their hadronic decay channels
             in the centre-of-mass rapidity range −0.96 < ycms< 0.04
             and transverse momentum interval 1<pT<24 GeV/c. The
             multiplicity dependence of D-meson production is examined by
             either comparing yields in p-Pb collisions in different
             event classes, selected based on the multiplicity of
             produced particles or zero-degree energy, with those in pp
             collisions, scaled by the number of binary nucleon-nucleon
             collisions (nuclear modification factor); as well as by
             evaluating the per-event yields in p-Pb collisions in
             different multiplicity intervals normalised to the
             multiplicity-integrated ones (relative yields). The nuclear
             modification factors for D0, D+ and D∗+ are consistent
             with one another. The D-meson nuclear modification factors
             as a function of the zero-degree energy are consistent with
             unity within uncertainties in the measured pT regions and
             event classes. The relative D-meson yields, calculated in
             various pT intervals, increase as a function of the
             charged-particle multiplicity. The results are compared with
             the equivalent pp measurements at s=7 TeV as well as with
             EPOS 3 calculations.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP08(2016)078},
   Key = {fds329529}
}

@article{fds321420,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
             A},
   Title = {Search for pair production of gluinos decaying via stop and
             sbottom in events with b -jets and large missing transverse
             momentum in pp collisions at s =13 TeV with the ATLAS
             detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032003},
   Abstract = {A search for supersymmetry involving the pair production of
             gluinos decaying via third-generation squarks to the
             lightest neutralino (χ10) is reported. It uses an LHC
             proton-proton data set at a center-of-mass energy s=13 TeV
             with an integrated luminosity of 3.2 fb-1 collected with the
             ATLAS detector in 2015. The signal is searched for in events
             containing several energetic jets, of which at least three
             must be identified as b jets, large missing transverse
             momentum, and, potentially, isolated electrons or muons.
             Large-radius jets with a high mass are also used to identify
             highly boosted top quarks. No excess is found above the
             predicted background. For χ10 masses below approximately
             700 GeV, gluino masses of less than 1.78 TeV and 1.76 TeV
             are excluded at the 95% C.L. in simplified models of the
             pair production of gluinos decaying via sbottom and stop,
             respectively. These results significantly extend the
             exclusion limits obtained with the s=8 TeV data
             set.},
   Doi = {10.1103/PhysRevD.94.032003},
   Key = {fds321420}
}

@article{fds321411,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Measurement of W± and Z-boson production cross
             sections in pp collisions at √s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {759},
   Pages = {601-621},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.06.023},
   Abstract = {Measurements of the W±→ℓ±ν and Z→ℓ+ℓ−
             production cross sections (where ℓ±=e±,μ±) in
             proton–proton collisions at s=13 TeV are presented using
             data recorded by the ATLAS experiment at the Large Hadron
             Collider, corresponding to a total integrated luminosity of
             81 pb−1. The total inclusive W±-boson production cross
             sections times the single-lepton-flavour branching ratios
             are σW+tot=11.83±0.02 (stat)±0.32 (sys)±0.25 (lumi) nb
             and σW−tot=8.79±0.02 (stat)±0.24 (sys)±0.18 (lumi) nb
             for W+ and W−, respectively. The total inclusive Z-boson
             production cross section times leptonic branching ratio,
             within the invariant mass window 66<mℓℓ<116 GeV, is
             σZtot=1.981±0.007 (stat)±0.038 (sys)±0.042 (lumi) nb.
             The W+, W−, and Z-boson production cross sections and
             cross-section ratios within a fiducial region defined by the
             detector acceptance are also measured. The cross-section
             ratios benefit from significant cancellation of experimental
             uncertainties, resulting in σW+fid/σW−fid=1.295±0.003
             (stat)±0.010 (sys) and σW±fid/σZfid=10.31±0.04
             (stat)±0.20 (sys). Theoretical predictions, based on
             calculations accurate to next-to-next-to-leading order for
             quantum chromodynamics and to next-to-leading order for
             electroweak processes and which employ different parton
             distribution function sets, are compared to these
             measurements.},
   Doi = {10.1016/j.physletb.2016.06.023},
   Key = {fds321411}
}

@article{fds321442,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for resonances in the mass distribution of jet pairs
             with one or two jets identified as b-jets in proton–proton
             collisions at s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {759},
   Pages = {229-246},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.05.064},
   Abstract = {Searches for high-mass resonances in the dijet invariant
             mass spectrum with one or two jets identified as b-jets are
             performed using an integrated luminosity of 3.2 fb−1 of
             proton–proton collisions with a centre-of-mass energy of
             s=13 TeV recorded by the ATLAS detector at the Large Hadron
             Collider. No evidence of anomalous phenomena is observed in
             the data, which are used to exclude, at 95% credibility
             level, excited b⁎ quarks with masses from 1.1 TeV to 2.1
             TeV and leptophobic Z′ bosons with masses from 1.1 TeV to
             1.5 TeV. Contributions of a Gaussian signal shape with
             effective cross sections ranging from approximately 0.4 to
             0.001 pb are also excluded in the mass range 1.5–5.0
             TeV.},
   Doi = {10.1016/j.physletb.2016.05.064},
   Key = {fds321442}
}

@article{fds321614,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for charged Higgs bosons produced in association with
             a top quark and decaying via H± → τν using
             pp collision data recorded at √s=13 TeV by the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {759},
   Pages = {555-574},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.06.017},
   Abstract = {Charged Higgs bosons produced in association with a single
             top quark and decaying via H±→τν are searched for with
             the ATLAS experiment at the LHC, using proton–proton
             collision data at s=13 TeV corresponding to an integrated
             luminosity of 3.2 fb−1. The final state is characterised
             by the presence of a hadronic τ decay and missing
             transverse momentum, as well as a hadronically decaying top
             quark, resulting in the absence of high-transverse-momentum
             electrons and muons. The data are found to be consistent
             with the expected background from Standard Model processes.
             A statistical analysis leads to 95% confidence-level upper
             limits on the production cross section times branching
             fraction, σ(pp→[b]tH±)×BR(H±→τν), between 1.9 pb
             and 15 fb, for charged Higgs boson masses ranging from 200
             to 2000 GeV. The exclusion limits for this search surpass
             those obtained with the proton–proton collision data
             recorded at s=8 TeV.},
   Doi = {10.1016/j.physletb.2016.06.017},
   Key = {fds321614}
}

@article{fds321419,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for new phenomena in final states with an energetic
             jet and large missing transverse momentum in pp collisions
             at s =13 TeV using the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032005},
   Abstract = {Results of a search for new phenomena in final states with
             an energetic jet and large missing transverse momentum are
             reported. The search uses proton-proton collision data
             corresponding to an integrated luminosity of 3.2 fb-1 at
             s=13 TeV collected in 2015 with the ATLAS detector at the
             Large Hadron Collider. Events are required to have at least
             one jet with a transverse momentum above 250 GeV and no
             leptons. Several signal regions are considered with
             increasing missing-transverse-momentum requirements between
             ETmiss>250 GeV and ETmiss>700 GeV. Good agreement is
             observed between the number of events in data and Standard
             Model predictions. The results are translated into exclusion
             limits in models with large extra spatial dimensions, pair
             production of weakly interacting dark-matter candidates, and
             the production of supersymmetric particles in several
             compressed scenarios.},
   Doi = {10.1103/PhysRevD.94.032005},
   Key = {fds321419}
}

@article{fds321418,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Measurements of the charge asymmetry in top-quark pair
             production in the dilepton final state at s =8 TeV with the
             ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032006},
   Abstract = {Measurements of the top-antitop quark pair production charge
             asymmetry in the dilepton channel, characterized by two
             high-pT leptons (electrons or muons), are presented using
             data corresponding to an integrated luminosity of 20.3 fb-1
             from pp collisions at a center-of-mass energy s=8 TeV
             collected with the ATLAS detector at the Large Hadron
             Collider at CERN. Inclusive and differential measurements as
             a function of the invariant mass, transverse momentum, and
             longitudinal boost of the tt system are performed both in
             the full phase space and in a fiducial phase space closely
             matching the detector acceptance. Two observables are
             studied: ACℓℓ based on the selected leptons and ACtt
             based on the reconstructed tt final state. The inclusive
             asymmetries are measured in the full phase space to be
             ACℓℓ=0.008±0.006 and ACtt=0.021±0.016, which are in
             agreement with the Standard Model predictions of
             ACℓℓ=0.0064±0.0003 and ACtt=0.0111±0.0004.},
   Doi = {10.1103/PhysRevD.94.032006},
   Key = {fds321418}
}

@article{fds321412,
   Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
             F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
             HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
             M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
             A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
             A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
   Title = {Measurement of the WW and WZ production cross section using
             final states with a charged lepton and heavy-flavor jets in
             the full CDF Run II data set},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032008},
   Abstract = {We present a measurement of the total WW and WZ production
             cross sections in pp collision at s=1.96 TeV, in a final
             state consistent with leptonic W boson decay and jets
             originating from heavy-flavor quarks from either a W or a Z
             boson decay. This analysis uses the full data set collected
             with the CDF II detector during Run II of the Tevatron
             collider, corresponding to an integrated luminosity of 9.4
             fb-1. An analysis of the dijet mass spectrum provides 3.7σ
             evidence of the summed production processes of either WW or
             WZ bosons with a measured total cross section of
             σWW+WZ=13.7±3.9 pb. Independent measurements of the WW and
             WZ production cross sections are allowed by the different
             heavy-flavor decay patterns of the W and Z bosons and by the
             analysis of secondary-decay vertices reconstructed within
             heavy-flavor jets. The productions of WW and of WZ dibosons
             are independently seen with significances of 2.9σ and
             2.1σ, respectively, with total cross sections of
             σWW=9.4±4.2 pb and σWZ=3.7-2.2+2.5 pb. The measurements
             are consistent with standard-model predictions.},
   Doi = {10.1103/PhysRevD.94.032008},
   Key = {fds321412}
}

@article{fds321423,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of exclusive γγ →w+W- production and search
             for exclusive Higgs boson production in pp collisions at s
             =8 TeV using the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {3},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {August},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.032011},
   Abstract = {Searches for exclusively produced W boson pairs in the
             process pp(γγ)→pW+W-p and an exclusively produced Higgs
             boson in the process pp(gg)→pHp have been performed using
             e±μ final states. These measurements use 20.2 fb-1 of pp
             collisions collected by the ATLAS experiment at a
             center-of-mass energy s=8 TeV at the LHC. Exclusive
             production of W+W- consistent with the Standard Model
             prediction is found with 3.0σ significance. The exclusive
             W+W- production cross section is determined to be
             σ(γγ→W+W-→e±μX)=6.9±2.2(stat)±1.4(sys) fb, in
             agreement with the Standard Model prediction. Limits on
             anomalous quartic gauge couplings are set at 95% confidence
             level as -1.7×10-6<a0W/Λ2<1.7×10-6 GeV-2 and
             -6.4×10-6<aCW/Λ2<6.3×10-6 GeV-2. A 95% confidence-level
             upper limit on the total production cross section for an
             exclusive Higgs boson is set to 1.2 pb.},
   Doi = {10.1103/PhysRevD.94.032011},
   Key = {fds321423}
}

@article{fds321405,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Measurement of jet activity in top quark events using the
             eμ final state with two b-tagged jets in pp collisions at
             √s=8 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)074},
   Abstract = {Measurements of the jet activity in tt¯ events produced in
             proton-proton collisions at s=8 TeV are presented, using
             20.3 fb−1 of data collected by the ATLAS experiment at the
             Large Hadron Collider. The events were selected in the
             dilepton eμ decay channel with two identified b-jets. The
             numbers of additional jets for various jet transverse
             momentum (pT) thresholds, and the normalised differential
             cross-sections as a function of pT for the five highest-pT
             additional jets, were measured in the jet pseudo-rapidity
             range |η| < 4.5. The gap fraction, the fraction of events
             which do not contain an additional jet in a central rapidity
             region, was measured for several rapidity intervals as a
             function of the minimum pT of a single jet or the scalar sum
             of pT of all additional jets. These fractions were also
             measured in different intervals of the invariant mass of the
             eμbb¯ system. All measurements were corrected for detector
             effects, and found to be mostly well-described by
             predictions from next-to-leading-order and leading-order
             tt¯ event generators with appropriate parameter choices.
             The results can be used to further optimise the parameters
             used in such generators.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP09(2016)074},
   Key = {fds321405}
}

@article{fds321407,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Searches for heavy diboson resonances in pp collisions at
             √s=13 TeV with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)173},
   Abstract = {Searches for new heavy resonances decaying to WW, WZ, and ZZ
             bosons are presented, using a data sample corresponding to
             3.2 fb−1 of pp collisions at s=13 TeV collected with the
             ATLAS detector at the CERN Large Hadron Collider. Analyses
             selecting ννqq, ℓνqq, ℓℓqq and qqqq final states
             are combined, searching for an arrow-width resonance with
             mass between 500 and 3000 GeV. The discriminating variable
             is either an invariant mass or a transverse mass. No
             significant deviations from the Standard Model predictions
             are observed. Three benchmark models are tested: a model
             predicting the existence of a new heavy scalar singlet, a
             simplified model predicting a heavy vector-boson triplet,
             and a bulk Randall-Sundrum model with a heavy spin-2
             graviton. Cross-section limits are set at the 95% confidence
             level and are compared to theoretical cross-section
             predictions for a variety of models. The data exclude a
             scalar singlet with mass below 2650 GeV, a heavy
             vector-boson triplet with mass below 2600 GeV, and a
             graviton with mass below 1100 GeV. These results
             significantly extend the previous limits set using pp
             collisions at s=8 TeV.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP09(2016)173},
   Key = {fds321407}
}

@article{fds321408,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
             A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Dark matter interpretations of ATLAS searches for the
             electroweak production of supersymmetric particles in √s=8
             TeV proton-proton collisions},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)175},
   Abstract = {A selection of searches by the ATLAS experiment at the LHC
             for the electroweak production of SUSY particles are used to
             study their impact on the constraints on dark matter
             candidates. The searches use 20 fb−1 of proton-proton
             collision data at s=8 TeV. A likelihood-driven scan of a
             five-dimensional effective model focusing on the
             gaugino-higgsino and Higgs sector of the phenomenological
             minimal supersymmetric Standard Model is performed. This
             scan uses data from direct dark matter detection
             experiments, the relic dark matter density and precision
             flavour physics results. Further constraints from the ATLAS
             Higgs mass measurement and SUSY searches at LEP are also
             applied. A subset of models selected from this scan are used
             to assess the impact of the selected ATLAS searches in this
             five-dimensional parameter space. These ATLAS searches
             substantially impact those models for which the mass
             m(χ˜10) of the lightest neutralino is less than 65 GeV,
             excluding 86% of such models. The searches have limited
             impact on models with larger m(χ˜10) due to either heavy
             electroweakinos or compressed mass spectra where the mass
             splittings between the produced particles and the lightest
             supersymmetric particle is small.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP09(2016)175},
   Key = {fds321408}
}

@article{fds329528,
   Author = {Adam, J and Adamová, D and Aggarwal, MM and Aglieri Rinella and G and Agnello, M and Agrawal, N and Ahammed, Z and Ahmad, S and Ahn, SU and Aiola, S and Akindinov, A and Alam, SN and Albuquerque, DSD and Aleksandrov, D and Alessandro, B and Alexandre, D and Alfaro Molina,
             R and Alici, A and Alkin, A and Alme, J and Alt, T and Altinpinar, S and Altsybeev, I and Alves Garcia Prado and C and Andrei, C and Andronic, A and Anguelov, V and Antičić, T and Antinori, F and Antonioli, P and Aphecetche, L and Appelshäuser, H and Arcelli, S and Arnaldi, R and Arnold, OW and Arsene, IC and Arslandok, M and Audurier, B and Augustinus, A and Averbeck, R and Azmi, MD and Badalà, A and Baek, YW and Bagnasco, S and Bailhache, R and Bala, R and Balasubramanian, S and Baldisseri, A and Baral, RC and Barbano, AM and Barbera, R and Barile,
             F and Barnaföldi, GG and Barnby, LS and Barret, V and Bartalini, P and Barth, K and Bartke, J and Bartsch, E and Basile, M and Bastid, N and Basu,
             S and Bathen, B and Batigne, G and Batista Camejo and A and Batyunya, B and Batzing, PC and Bearden, IG and Beck, H and Bedda, C and Behera, NK and Belikov, I and Bellini, F and Bello Martinez and H and Bellwied, R and Belmont, R and Belmont-Moreno, E and Beltran, LGE and Belyaev, V and Bencedi, G and Beole, S and Berceanu, I and Bercuci, A and Berdnikov, Y and Berenyi, D and Bertens, RA and Berzano, D and Betev, L and Bhasin, A and Bhat, IR and Bhati, AK and Bhattacharjee, B and Bhom, J and Bianchi, L and Bianchi, N and Bianchin, C and Bielčík, J and Bielčíková, J and Bilandzic, A and Biro, G},
   Title = {Elliptic flow of electrons from heavy-flavour hadron decays
             at mid-rapidity in Pb-Pb collisions at √sNN=2.76
             TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)028},
   Abstract = {The elliptic flow of electrons from heavy-flavour hadron
             decays at mid-rapidity (|y| < 0.7) is measured in Pb-Pb
             collisions at sNN=2.76 TeV with ALICE at the LHC. The
             particle azimuthal distribution with respect to the reaction
             plane can be parametrized with a Fourier expansion, where
             the second coefficient (v2) represents the elliptic flow.
             The v2 coefficient of inclusive electrons is measured in
             three centrality classes (0–10%, 10–20% and 20–40%)
             with the event plane and the scalar product methods in the
             transverse momentum (pT) intervals 0.5–13 GeV/c and
             0.5–8 GeV/c, respectively. After subtracting the
             background, mainly from photon conversions and Dalitz decays
             of neutral mesons, a positive v2 of electrons from
             heavy-flavour hadron decays is observed in all centrality
             classes, with a maximum significance of 5.9σ in the
             interval 2 < pT < 2.5 GeV/c in semi-central collisions
             (20–40%). The value of v2 decreases towards more central
             collisions at low and intermediate pT (0.5 < pT < 3 GeV/c).
             The v2 of electrons from heavy-flavour hadron decays at
             mid-rapidity is found to be similar to the one of muons from
             heavy-flavour hadron decays at forward rapidity (2.5 < y <
             4). The results are described within uncertainties by model
             calculations including substantial elastic interactions of
             heavy quarks with an expanding strongly-interacting
             medium.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP09(2016)028},
   Key = {fds329528}
}

@article{fds321401,
   Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for resonances in diphoton events at √s=13 TeV with
             the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)001},
   Abstract = {Searches for new resonances decaying into two photons in the
             ATLAS experiment at the CERN Large Hadron Collider are
             described. The analysis is based on proton-proton collision
             data corresponding to an integrated luminosity of 3.2 fb−1
             at s=13 TeV recorded in 2015. Two searches are performed,
             one targeted at a spin-2 particle of mass larger than 500
             GeV, using Randall-Sundrum graviton states as a benchmark
             model, and one optimized for a spin-0 particle of mass
             larger than 200 GeV. Varying both the mass and the decay
             width, the most significant deviation from the
             background-only hypothesis is observed at a diphoton
             invariant mass around 750 GeV with local significances of
             3.8 and 3.9 standard deviations in the searches optimized
             for a spin-2 and spin-0 particle, respectively. The global
             significances are estimated to be 2.1 standard deviations
             for both analyses. The consistency between the data
             collected at 13 TeV and 8 TeV is also evaluated. Limits on
             the production cross section times branching ratio to two
             photons for the two resonance types are reported.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP09(2016)001},
   Key = {fds321401}
}

@article{fds321402,
   Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
             L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
             G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
             CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
             A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
             ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
   Title = {Measurement of total and differential W + W
              production cross sections in proton-proton
             collisions at √s=8 TeV with the ATLAS detector and limits
             on anomalous triple-gauge-boson couplings},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)029},
   Abstract = {The production of W boson pairs in proton-proton collisions
             at s=8 TeV is studied using data corresponding to 20.3
             fb−1 of integrated luminosity collected by the ATLAS
             detector during 2012 at the CERN Large Hadron Collider. The
             W bosons are reconstructed using their leptonic decays into
             electrons or muons and neutrinos. Events with reconstructed
             jets are not included in the candidate event sample. A total
             of 6636 WW candidate events are observed. Measurements are
             performed in fiducial regions closely approximating the
             detector acceptance. The integrated measurement is corrected
             for all acceptance effects and for the W branching fractions
             to leptons in order to obtain the total WW production cross
             section, which is found to be 71.1 ± 1.1(stat) − 5.0+
             5.7(syst) ± 1.4(lumi) pb. This agrees with the
             next-to-next-to-leading-order Standard Model prediction of
             63. 2− 1.4+ 1.6(scale) ± 1.2(PDF) pb. Fiducial
             differential cross sections are measured as a function of
             each of six kinematic variables. The distribution of the
             transverse momentum of the leading lepton is used to set
             limits on anomalous triple-gauge-boson couplings.[Figure not
             available: see fulltext.]},
   Doi = {10.1007/JHEP09(2016)029},
   Key = {fds321402}
}

@article{fds321399,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
             J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Search for Higgs and Z Boson Decays to ϕγ with the ATLAS
             Detector.},
   Journal = {Physical review letters},
   Volume = {117},
   Number = {11},
   Pages = {111802},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1103/physrevlett.117.111802},
   Abstract = {A search for the decays of the Higgs and Z bosons to a ϕ
             meson and a photon is performed with a pp collision data
             sample corresponding to an integrated luminosity of
             2.7  fb^{-1} collected at sqrt[s]=13  TeV with the
             ATLAS detector at the LHC. No significant excess of events
             is observed above the background, and 95% confidence level
             upper limits on the branching fractions of the Higgs and Z
             boson decays to ϕγ of 1.4×10^{-3} and 8.3×10^{-6},
             respectively, are obtained.},
   Doi = {10.1103/physrevlett.117.111802},
   Key = {fds321399}
}

@article{fds329527,
   Author = {Adam, J and Adamová, D and Aggarwal, MM and Aglieri Rinella and G and Agnello, M and Agrawal, N and Ahammed, Z and Ahmad, S and Ahn, SU and Aiola, S and Akindinov, A and Alam, SN and Albuquerque, DSD and Aleksandrov, D and Alessandro, B and Alexandre, D and Alfaro Molina,
             R and Alici, A and Alkin, A and Alme, J and Alt, T and Altinpinar, S and Altsybeev, I and Alves Garcia Prado and C and An, M and Andrei, C and Andrews, HA and Andronic, A and Anguelov, V and Antičić, T and Antinori, F and Antonioli, P and Aphecetche, L and Appelshäuser, H and Arcelli, S and Arnaldi, R and Arnold, OW and Arsene, IC and Arslandok,
             M and Audurier, B and Augustinus, A and Averbeck, R and Azmi, MD and Badalà, A and Baek, YW and Bagnasco, S and Bailhache, R and Bala, R and Balasubramanian, S and Baldisseri, A and Baral, RC and Barbano, AM and Barbera, R and Barile, F and Barnaföldi, GG and Barnby, LS and Barret,
             V and Bartalini, P and Barth, K and Bartke, J and Bartsch, E and Basile, M and Bastid, N and Basu, S and Bathen, B and Batigne, G and Batista Camejo,
             A and Batyunya, B and Batzing, PC and Bearden, IG and Beck, H and Bedda, C and Behera, NK and Belikov, I and Bellini, F and Bello Martinez and H and Bellwied, R and Belmont, R and Belmont-Moreno, E and Beltran, LGE and Belyaev, V and Bencedi, G and Beole, S and Berceanu, I and Bercuci, A and Berdnikov, Y and Berenyi, D and Bertens, RA and Berzano, D and Betev, L and Bhasin, A and Bhat, IR and Bhati, AK and Bhattacharjee, B and Bhom, J and Bianchi, L and Bianchi, N and Bianchin, C and Bielčík, J and Bielčíková, J},
   Title = {Higher harmonic flow coefficients of identified hadrons in
             Pb-Pb collisions at √sNN=2.76 TeV},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {9},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1007/JHEP09(2016)164},
   Abstract = {The elliptic, triangular, quadrangular and pentagonal
             anisotropic flow coefficients for π±, K± and p + p ¯ in
             Pb-Pb collisions at sNN=2.76 TeV were measured with the
             ALICE detector at the Large Hadron Collider. The results
             were obtained with the Scalar Product method, correlating
             the identified hadrons with reference particles from a
             different pseudorapidity region. Effects not related to the
             common event symmetry planes (non-flow) were estimated using
             correlations in pp collisions and were subtracted from the
             measurement. The obtained flow coefficients exhibit a clear
             mass ordering for transverse momentum (pT) values below ≈
             3 GeV/c. In the intermediate pT region (3 < pT< 6 GeV/c),
             particles group at an approximate level according to the
             number of constituent quarks, suggesting that coalescence
             might be the relevant particle production mechanism in this
             region. The results for pT< 3 GeV/c are described fairly
             well by a hydrodynamical model (iEBE-VISHNU) that uses
             initial conditions generated by A Multi-Phase Transport
             model (AMPT) and describes the expansion of the fireball
             using a value of 0.08 for the ratio of shear viscosity to
             entropy density (η/s), coupled to a hadronic cascade model
             (UrQMD). Finally, expectations from AMPT alone fail to
             quantitatively describe the measurements for all harmonics
             throughout the measured transverse momentum region. However,
             the comparison to the AMPT model highlights the importance
             of the late hadronic rescattering stage to the development
             of the observed mass ordering at low values of pT and of
             coalescence as a particle production mechanism for the
             particle type grouping at intermediate values of pT for all
             harmonics.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP09(2016)164},
   Key = {fds329527}
}

@article{fds321410,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
             O},
   Title = {Search for pair production of Higgs bosons in the bbbb final
             state using proton-proton collisions at √s =13 TeV with
             the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.052002},
   Abstract = {A search for Higgs-boson pair production in the bbbb final
             state is carried out with 3.2 fb-1 of proton-proton
             collision data collected at s=13 TeV with the ATLAS
             detector. The data are consistent with the estimated
             background and are used to set upper limits on the
             production cross section of Higgs-boson pairs times
             branching ratio to bbbb for both nonresonant and resonant
             production. In the case of resonant production of
             Kaluza-Klein gravitons within the Randall-Sundrum model,
             upper limits in the 24 to 91 fb range are obtained for
             masses between 600 and 3000 GeV, at the 95% confidence
             level. The production cross section times branching ratio
             for nonresonant Higgs-boson pairs is also constrained to be
             less than 1.22 pb, at the 95% confidence
             level.},
   Doi = {10.1103/PhysRevD.94.052002},
   Key = {fds321410}
}

@article{fds321397,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for TeV-scale gravity signatures in high-mass final
             states with leptons and jets with the ATLAS detector at
             √s=13 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {760},
   Pages = {520-537},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.07.030},
   Abstract = {A search for physics beyond the Standard Model, in final
             states with at least one high transverse momentum charged
             lepton (electron or muon) and two additional high transverse
             momentum leptons or jets, is performed using 3.2 fb−1 of
             proton–proton collision data recorded by the ATLAS
             detector at the Large Hadron Collider in 2015 at s=13 TeV.
             The upper end of the distribution of the scalar sum of the
             transverse momenta of leptons and jets is sensitive to the
             production of high-mass objects. No excess of events beyond
             Standard Model predictions is observed. Exclusion limits are
             set for models of microscopic black holes with two to six
             extra dimensions.},
   Doi = {10.1016/j.physletb.2016.07.030},
   Key = {fds321397}
}

@article{fds321398,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adersberger, M and Adomeit, S and Adye,
             T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
             Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
             Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
             V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
             L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Search for heavy long-lived charged R-hadrons with the ATLAS
             detector in 3.2 fb−1 of proton–proton
             collision data at √s=13 TeV},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {760},
   Pages = {647-665},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.07.042},
   Abstract = {A search for heavy long-lived charged R-hadrons is reported
             using a data sample corresponding to 3.2 fb−1 of
             proton–proton collisions at s=13 TeV collected by the
             ATLAS experiment at the Large Hadron Collider at CERN. The
             search is based on observables related to large ionisation
             losses and slow propagation velocities, which are signatures
             of heavy charged particles travelling significantly slower
             than the speed of light. No significant deviations from the
             expected background are observed. Upper limits at 95%
             confidence level are provided on the production cross
             section of long-lived R-hadrons in the mass range from 600
             GeV to 2000 GeV and gluino, bottom and top squark masses are
             excluded up to 1580 GeV, 805 GeV and 890 GeV,
             respectively.},
   Doi = {10.1016/j.physletb.2016.07.042},
   Key = {fds321398}
}

@article{fds321409,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for top squarks in final states with one isolated
             lepton, jets, and missing transverse momentum in s =13 TeV
             pp collisions with the ATLAS detector},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {5},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {September},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.052009},
   Abstract = {The results of a search for the top squark, the
             supersymmetric partner of the top quark, in final states
             with one isolated electron or muon, jets, and missing
             transverse momentum are reported. The search uses the 2015
             LHC pp collision data at a center-of-mass energy of s=13 TeV
             recorded by the ATLAS detector and corresponding to an
             integrated luminosity of 3.2 fb-1. The analysis targets two
             types of signal models: gluino-mediated pair production of
             top squarks with a nearly mass-degenerate top squark and
             neutralino and direct pair production of top squarks,
             decaying to the top quark and the lightest neutralino. The
             experimental signature in both signal scenarios is similar
             to that of a top quark pair produced in association with
             large missing transverse momentum. No significant excess
             over the Standard Model background prediction is observed,
             and exclusion limits on gluino and top squark masses are set
             at 95% confidence level. The results extend the LHC run-1
             exclusion limit on the gluino mass up to 1460 GeV in the
             gluino-mediated scenario in the high gluino and low top
             squark mass region and add an excluded top squark mass
             region from 745 to 780 GeV for the direct top squark model
             with a massless lightest neutralino. The results are also
             reinterpreted to set exclusion limits in a model of
             vectorlike top quarks.},
   Doi = {10.1103/PhysRevD.94.052009},
   Key = {fds321409}
}

@article{fds321391,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for high-mass new phenomena in the dilepton final
             state using proton–proton collisions at s=13TeV with the
             ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {372-392},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.055},
   Abstract = {A search is conducted for both resonant and non-resonant
             high-mass new phenomena in dielectron and dimuon final
             states. The search uses 3.2fb−1 of proton–proton
             collision data, collected at s=13TeV by the ATLAS experiment
             at the LHC in 2015. The dilepton invariant mass is used as
             the discriminating variable. No significant deviation from
             the Standard Model prediction is observed; therefore limits
             are set on the signal model parameters of interest at 95%
             credibility level. Upper limits are set on the cross-section
             times branching ratio for resonances decaying to dileptons,
             and the limits are converted into lower limits on the
             resonance mass, ranging between 2.74 TeV and 3.36 TeV,
             depending on the model. Lower limits on the ℓℓqq contact
             interaction scale are set between 16.7 TeV and 25.2 TeV,
             also depending on the model.},
   Doi = {10.1016/j.physletb.2016.08.055},
   Key = {fds321391}
}

@article{fds321443,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of the tt¯ production cross-section using eμ
             events with b-tagged jets in pp collisions at √s=13TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {136-157},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.019},
   Abstract = {This paper describes a measurement of the inclusive top
             quark pair production cross-section (σtt¯) with a data
             sample of 3.2fb−1 of proton–proton collisions at a
             centre-of-mass energy of s=13TeV, collected in 2015 by the
             ATLAS detector at the LHC. This measurement uses events with
             an opposite-charge electron–muon pair in the final state.
             Jets containing b-quarks are tagged using an algorithm based
             on track impact parameters and reconstructed secondary
             vertices. The numbers of events with exactly one and exactly
             two b-tagged jets are counted and used to determine
             simultaneously σtt¯ and the efficiency to reconstruct and
             b-tag a jet from a top quark decay, thereby minimising the
             associated systematic uncertainties. The cross-section is
             measured to be: σtt¯=818±8(stat)±27(syst)±19(lumi)±12(beam)
             pb, where the four uncertainties arise from data statistics,
             experimental and theoretical systematic effects, the
             integrated luminosity and the LHC beam energy, giving a
             total relative uncertainty of 4.4%. The result is consistent
             with theoretical QCD calculations at next-to-next-to-leading
             order. A fiducial measurement corresponding to the
             experimental acceptance of the leptons is also
             presented.},
   Doi = {10.1016/j.physletb.2016.08.019},
   Key = {fds321443}
}

@article{fds321444,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of the top quark mass in the tt¯→dilepton
             channel from √s=8 TeV ATLAS data},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {761},
   Pages = {350-371},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.042},
   Abstract = {The top quark mass is measured in the tt¯→dilepton
             channel (lepton=e,μ) using ATLAS data recorded in the year
             2012 at the LHC. The data were taken at a proton–proton
             centre-of-mass energy of s=8 TeV and correspond to an
             integrated luminosity of about 20.2 fb−1. Exploiting the
             template method, and using the distribution of invariant
             masses of lepton–b-jet pairs, the top quark mass is
             measured to be mtop=172.99±0.41 (stat)±0.74 (syst) GeV,
             with a total uncertainty of 0.84 GeV. Finally, a combination
             with previous ATLAS mtop measurements from s=7 TeV data in
             the tt¯→dilepton and tt¯→lepton+jets channels results
             in mtop=172.84±0.34 (stat)±0.61 (syst) GeV, with a total
             uncertainty of 0.70 GeV.},
   Doi = {10.1016/j.physletb.2016.08.042},
   Key = {fds321444}
}

@article{fds321390,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
             B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
             NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
             T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
             P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
             CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
             K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
             G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
             RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
             J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
             J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
             U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
             P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
             Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
             J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
             WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
             FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
             WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
             Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
             K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
             D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
             G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
             S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
             C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
             M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
             Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
             A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
             Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
             SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
             MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
             M},
   Title = {Measurement of the Inelastic Proton-Proton Cross Section at
             sqrt[s]=13  TeV with the ATLAS Detector at the
             LHC.},
   Journal = {Phys Rev Lett},
   Volume = {117},
   Number = {18},
   Pages = {182002},
   Year = {2016},
   Month = {October},
   url = {http://dx.doi.org/10.1103/PhysRevLett.117.182002},
   Abstract = {This Letter presents a measurement of the inelastic
             proton-proton cross section using 60  μb^{-1} of pp
             collisions at a center-of-mass energy sqrt[s] of 13 TeV
             with the ATLAS detector at the LHC. Inelastic interactions
             are selected using rings of plastic scintillators in the
             forward region (2.07<|η|<3.86) of the detector. A cross
             section of 68.1±1.4  mb is measured in the fiducial
             region ξ=M_{X}^{2}/s>10^{-6}, where M_{X} is the larger
             invariant mass of the two hadronic systems separated by the
             largest rapidity gap in the event. In this ξ range the
             scintillators are highly efficient. For diffractive events
             this corresponds to cases where at least one proton
             dissociates to a system with M_{X}>13  GeV. The measured
             cross section is compared with a range of theoretical
             predictions. When extrapolated to the full phase space, a
             cross section of 78.1±2.9  mb is measured, consistent
             with the inelastic cross section increasing with
             center-of-mass energy.},
   Doi = {10.1103/PhysRevLett.117.182002},
   Key = {fds321390}
}

@article{fds321389,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
   Title = {Study of hard double-parton scattering in four-jet events in
             pp collisions at √s=7 TeV with the ATLAS
             experiment},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2016)110},
   Abstract = {Inclusive four-jet events produced in proton-proton
             collisions at a centre-of-mass energy of s=7 TeV are
             analysed for the presence of hard double-parton scattering
             using data corresponding to an integrated luminosity of 37.3
             pb−1, collected with the ATLAS detector at the LHC. The
             contribution of hard double-parton scattering to the
             production of four-jet events is extracted using an
             artificial neural network, assuming that hard double-parton
             scattering can be approximated by an uncorrelated overlaying
             of dijet events. For events containing at least four jets
             with transverse momentum pT ≥ 20 GeV and pseudorapidity
             |η| ≤ 4.4, and at least one having pT ≥ 42.5 GeV, the
             contribution of hard double-parton scattering is estimated
             to be fDPS = 0.092− 0.011+ 0.005(stat.)− 0.037+
             0.033(syst.). After combining this measurement with those of
             the inclusive dijet and four-jet cross-sections in the
             appropriate phase space regions, the effective
             cross-section, σeff , was determined to be σeff = 14. 9−
             1.0+ 1.2(stat.)− 3.8+ 5.1(syst.) mb. This result is
             consistent within the quoted uncertainties with previous
             measurements of σeff , performed at centre-of-mass energies
             between 63 GeV and 8 TeV using various final states, and it
             corresponds to 21− 6+ 7 % of the total inelastic
             cross-section measured at s=7 TeV. The distributions of the
             observables sensitive to the contribution of hard
             double-parton scattering, corrected for detector effects,
             are also provided.[Figure not available: see
             fulltext.]},
   Doi = {10.1007/JHEP11(2016)110},
   Key = {fds321389}
}

@article{fds321388,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
   Title = {Search for the Standard Model Higgs boson produced by
             vector-boson fusion and decaying to bottom quarks in √s=8
             TeV pp collisions with the ATLAS detector},
   Journal = {Journal of High Energy Physics},
   Volume = {2016},
   Number = {11},
   Publisher = {Springer Nature},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1007/JHEP11(2016)112},
   Abstract = {A search with the ATLAS detector is presented for the
             Standard Model Higgs boson produced by vector-boson fusion
             and decaying to a pair of bottom quarks, using 20.2 fb−1
             of LHC proton-proton collision data at s=8 TeV. The signal
             is searched for as a resonance in the invariant mass
             distribution of a pair of jets containing b-hadrons in
             vector-boson-fusion candidate events. The yield is measured
             to be −0.8 ± 2.3 times the Standard Model cross-section
             for a Higgs boson mass of 125 GeV. The upper limit on the
             cross-section times the branching ratio is found to be 4.4
             times the Standard Model cross-section at the 95% confidence
             level, consistent with the expected limit value of 5.4 (5.7)
             in the background-only (Standard Model production)
             hypothesis.[Figure not available: see fulltext.]},
   Doi = {10.1007/JHEP11(2016)112},
   Key = {fds321388}
}

@article{fds327146,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {A measurement of material in the ATLAS tracker using
             secondary hadronic interactions in 7TeV pp
             collisions},
   Journal = {Journal of Instrumentation},
   Volume = {11},
   Number = {11},
   Pages = {P11020-P11020},
   Publisher = {IOP Publishing},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1088/1748-0221/11/11/P11020},
   Abstract = {Knowledge of the material in the ATLAS inner tracking
             detector is crucial in understanding the reconstruction of
             charged-particle tracks, the performance of algorithms that
             identify jets containing b-hadrons and is also essential to
             reduce background in searches for exotic particles that can
             decay within the inner detector volume. Interactions of
             primary hadrons produced in pp collisions with the material
             in the inner detector are used to map the location and
             amount of this material. The hadronic interactions of
             primary particles may result in secondary vertices, which in
             this analysis are reconstructed by an inclusive
             vertex-finding algorithm. Data were collected using
             minimum-bias triggers by the ATLAS detector operating at the
             LHC during 2010 at centre-of-mass energy √s = 7TeV, and
             correspond to an integrated luminosity of 19nb-1. Kinematic
             properties of these secondary vertices are used to study the
             validity of the modelling of hadronic interactions in
             simulation. Secondary-vertex yields are compared between
             data and simulation over a volume of about 0.7 m3 around the
             interaction point, and agreement is found within overall
             uncertainties.},
   Doi = {10.1088/1748-0221/11/11/P11020},
   Key = {fds327146}
}

@article{fds321384,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Search for new resonances in events with one lepton and
             missing transverse momentum in pp collisions at √s=13 TeV
             with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {762},
   Pages = {334-352},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.09.040},
   Abstract = {A search for W′ bosons in events with one lepton (electron
             or muon) and missing transverse momentum is presented. The
             search uses 3.2 fb−1 of pp collision data collected at
             s=13 TeV by the ATLAS experiment at the LHC in 2015. The
             transverse mass distribution is examined and no significant
             excess of events above the level expected from Standard
             Model processes is observed. Upper limits on the W′ boson
             cross-section times branching ratio to leptons are set as a
             function of the W′ mass. Within the Sequential Standard
             Model W′ masses below 4.07 TeV are excluded at the 95%
             confidence level. This extends the limit set using LHC data
             at s=8 TeV by around 800 GeV.},
   Doi = {10.1016/j.physletb.2016.09.040},
   Key = {fds321384}
}

@article{fds321445,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of the W±Z boson pair-production
             cross section in pp collisions at s=13 TeV with the ATLAS
             detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {762},
   Pages = {1-22},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.08.052},
   Abstract = {The production of W±Z events in proton–proton collisions
             at a centre-of-mass energy of 13 TeV is measured with the
             ATLAS detector at the LHC. The collected data correspond to
             an integrated luminosity of 3.2 fb−1. The W±Z candidates
             are reconstructed using leptonic decays of the gauge bosons
             into electrons or muons. The measured inclusive cross
             section in the detector fiducial region for leptonic decay
             modes is σW±Z→ℓ′νℓℓfid.=63.2±3.2(stat.)±2.6(sys.)±1.5(lumi.)
             fb. In comparison, the next-to-leading-order Standard Model
             prediction is 53.4−2.8+3.6 fb. The extrapolation of the
             measurement from the fiducial to the total phase space
             yields σW±Ztot.=50.6±2.6(stat.)±2.0(sys.)±0.9(th.)±1.2(lumi.)
             pb, in agreement with a recent next-to-next-to-leading-order
             calculation of 48.2−1.0+1.1 pb. The cross section as a
             function of jet multiplicity is also measured, together with
             the charge-dependent W+Z and W−Z cross sections and their
             ratio.},
   Doi = {10.1016/j.physletb.2016.08.052},
   Key = {fds321445}
}

@article{fds321387,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
             L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of top quark pair differential cross sections in
             the dilepton channel in pp collisions at √s =7 and 8 TeV
             with ATLAS},
   Journal = {Physical Review D},
   Volume = {94},
   Number = {9},
   Publisher = {American Physical Society (APS)},
   Year = {2016},
   Month = {November},
   url = {http://dx.doi.org/10.1103/PhysRevD.94.092003},
   Abstract = {Measurements of normalized differential cross sections of
             top quark pair (tt production are presented as a function of
             the mass, the transverse momentum and the rapidity of the tt
             system in proton-proton collisions at center-of-mass
             energies of s=7 and 8 TeV. The data set corresponds to an
             integrated luminosity of 4.6 fb-1 at 7 TeV and 20.2 fb-1 at
             8 TeV, recorded with the ATLAS detector at the Large Hadron
             Collider. Events with top quark pair signatures are selected
             in the dilepton final state, requiring exactly two charged
             leptons and at least two jets with at least one of the jets
             identified as likely to contain a b hadron. The measured
             distributions are corrected for detector effects and
             selection efficiency to cross sections at the parton level.
             The differential cross sections are compared with different
             Monte Carlo generators and theoretical calculations of tt
             production. The results are consistent with the majority of
             predictions in a wide kinematic range.},
   Doi = {10.1103/PhysRevD.94.092003},
   Key = {fds321387}
}

@article{fds322488,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
             SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
             G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
   Title = {Measurement of W+W-production in
             association with one jet in proton-proton collisions at √s
             = 8 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {763},
   Pages = {114-133},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.10.014},
   Abstract = {The production of Wboson pairs in association with one jet
             in pp collisions at √s = 8 TeV is studied using data
             corresponding to an integrated luminosity of 20.3
             fb-1collected by the ATLAS detector during 2012 at the CERN
             Large Hadron Collider. The cross section is measured in a
             fiducial phase-space region defined by the presence of
             exactly one electron and one muon, missing transverse
             momentum and exactly one jet with a transverse momentum
             above 25 GeV and a pseudorapidity of |η| <4.5. The leptons
             are required to have opposite electric charge and to pass
             transverse momentum and pseudorapidity requirements. The
             fiducial cross section is found to be σWWfid,1-jet= 136 ±
             6 (stat)± 14 (syst)± 3 (lumi) fb. In combination with a
             previous measurement restricted to leptonic final states
             with no associated jets, the fiducial cross section of WW
             production with zero or one jet is measured to be
             σWWfid,≤1-jet= 511 ±9 (stat)±26 (syst)±10 (lumi)fb.
             The ratio of fiducial cross sections in final states with
             one and zero jets is determined to be 0.36 ±0.05. Finally,
             a total cross section extrapolated from the fiducial
             measurement of WW production with zero or one associated jet
             is reported. The measurements are compared to theoretical
             predictions and found in good agreement.},
   Doi = {10.1016/j.physletb.2016.10.014},
   Key = {fds322488}
}

@article{fds321381,
   Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
             H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
             A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
             N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
             KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
             N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
   Title = {Search for dark matter produced in association with a
             hadronically decaying vector boson in pp collisions at
             √s=13 TeV with the ATLAS detector},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {763},
   Pages = {251-268},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.10.042},
   Abstract = {A search is presented for dark matter produced in
             association with a hadronically decaying W or Z boson using
             3.2 fb−1 of pp collisions at s=13 TeV recorded by the
             ATLAS detector at the Large Hadron Collider. Events with a
             hadronic jet compatible with a W or Z boson and with large
             missing transverse momentum are analysed. The data are
             consistent with the Standard Model predictions and are
             interpreted in terms of both an effective field theory and a
             simplified model containing dark matter.},
   Doi = {10.1016/j.physletb.2016.10.042},
   Key = {fds321381}
}

@article{fds321382,
   Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
             TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
             BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
             Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
             Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
             LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
             A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
             Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
             A},
   Title = {Transverse momentum, rapidity, and centrality dependence of
             inclusive charged-particle production in sNN=5.02
             TeV p + Pb collisions measured by the ATLAS
             experiment},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {763},
   Pages = {313-336},
   Publisher = {Elsevier BV},
   Year = {2016},
   Month = {December},
   url = {http://dx.doi.org/10.1016/j.physletb.2016.10.053},
   Abstract = {Measurements of the per-event charged-particle yield as a
             function of the charged-particle transverse momentum and
             rapidity are performed using p+Pb collision data collected
             by the ATLAS experiment at the LHC at a centre-of-mass
             energy of sNN=5.02TeV. Charged particles are reconstructed
             over pseudorapidity |η|<2.3 and transverse momentum between
             0.1 GeV and 22 GeV in a dataset corresponding to an
             integrated luminosity of 1 μb−1. The results are
             presented in the form of charged-particle nuclear
             modification factors, where the p+Pb charged-particle
             multiplicities are compared between central and peripheral
             p+Pb collisions as well as to charged-particle cross
             sections measured in pp collisions. The p+Pb collision
             centrality is characterized by the total transverse energy
             measured in −4.9<η<−3.1, which is in the direction of
             the outgoing lead beam. Three different estimations of the
             number of nucleons participating in the p+Pb collision are
             carried out using the Glauber model and two Glauber–Gribov
             colour-fluctuation extensions to the Glauber model. The
             values of the nuclear modification factors are found to vary
             significantly as a function of rapidity and transverse
             momentum. A broad peak is observed for all centralities and
             rapidities in the nuclear modification factors for
             charged-particle transverse momentum values around 3 GeV.
             The magnitude of the peak increases for more central
             collisions as well as rapidity ranges closer to the
             direction of the outgoing lead nucleus.},
   Doi = {10.1016/j.physletb.2016.10.053},
   Key = {fds321382}
}

@article{fds356859,
   Author = {Oh, SH and Lin, S and Wang, C},
   Title = {Techniques to measure tension in wires or straw
             tubes},
   Journal = {Journal of Instrumentation},
   Volume = {13},
   Number = {1},
   Year = {2018},
   Month = {January},
   url = {http://dx.doi.org/10.1088/1748-0221/13/01/T01001},
   Abstract = {We discuss two different ways of measuring the tension in
             light wires and straws. The first technique uses an
             operational amplifier to subtract out the oscillating
             driving voltage mixed in the output voltage, which also has
             the signal. The isolated signal is amplified and displayed
             in an oscilloscope. In the second technique, an analog
             switch routes the oscillating voltage to a wire for a
             fraction of seconds, and then switches off the voltage. As
             the voltage is turned off, the induced signal from the wire
             is routed to an amplifier-rectifier circuit for a fraction
             of a second to measure the signal size as a function of the
             driving frequency. The first technique fits well to measure
             a single wire, while the second one fits well to measure
             many wires, 16 in our case, at a time.},
   Doi = {10.1088/1748-0221/13/01/T01001},
   Key = {fds356859}
}

@article{fds356858,
   Author = {Oh, SH and Hazineh, D and Wang, C},
   Title = {The effect of electrostatic and gravity force on offset wire
             inside tube},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {888},
   Pages = {79-87},
   Year = {2018},
   Month = {April},
   url = {http://dx.doi.org/10.1016/j.nima.2018.01.017},
   Abstract = {In a straw-tube detector, a wire that is offset with respect
             to the tube axis experiences a Coulomb force when high
             voltage is applied between the anode wire and the tube. This
             force results in a shifting of the wire and straw, in
             addition to the gravitational sag, and is a function of the
             tube and wire radius, initial offset, high voltage, tension
             and length. The presence of such effects is well known, but
             the precise magnitude of the shift for the anode wires under
             conditions of detector operation have not been previously
             documented with measurable confidence. In this work, we
             provide the first systematic measurements for the wire shift
             in straw-tube detectors due to gravity and the electrostatic
             force using an x-ray scanner developed for the Mu2e
             experiment. The data are compared to the solutions of the
             differential equations governing the system, and we find a
             good match between the two. The solutions can predict the
             final wire and straw positions from the initial positions
             measured without the high voltage, and the final wire and
             straw positions can then be used as an input to the track
             reconstruction software to improve the track position
             resolution.},
   Doi = {10.1016/j.nima.2018.01.017},
   Key = {fds356858}
}

@article{fds356854,
   Author = {Bono, JS and Caron, JF and Oh, SH and Wang, C},
   Title = {The stress relaxation (creep) rate of Mu2e straw
             tubes},
   Journal = {Nuclear Instruments and Methods in Physics Research, Section
             A: Accelerators, Spectrometers, Detectors and Associated
             Equipment},
   Volume = {902},
   Pages = {95-102},
   Year = {2018},
   Month = {September},
   url = {http://dx.doi.org/10.1016/j.nima.2018.05.051},
   Abstract = {We report on the material relaxation properties of the Mu2e
             straw tubes measured over a period of about 5 years under
             two conditions. One is a fixed tension condition: two straw
             tubes are under a constant tension, and the lengthening of
             the tubes is measured as a function of time. The other is a
             fixed length condition: the length of four straw tubes with
             different initial tensions is fixed, and the tension in the
             tubes is measured. For the latter case, a scaling behavior
             appears when the ratio of the tension to the initial tension
             of the four straws is plotted as a function of time. In both
             cases, we find that the creep rates can be well
             parameterized with a logarithmic function of time elapsed.
             This implies that, for example, the amount of creep from day
             20 to 200 is the same as between day 200 and
             2000.},
   Doi = {10.1016/j.nima.2018.05.051},
   Key = {fds356854}
}

@article{fds347955,
   Author = {S. Oh (CDF collaboration)},
   Title = {Search for higgs like particle produced with bottom
             quark},
   Journal = {Phys.Rev. D99 (2019) no.5, 052001},
   Year = {2019},
   Key = {fds347955}
}

@article{fds347956,
   Author = {S. Oh (ATLAS collaboration)},
   Title = {Low mass dijet resonances with ISR 2017},
   Journal = {Phys. Lett B (795) (2019) 56},
   Year = {2019},
   Key = {fds347956}
}

@article{fds347957,
   Author = {S. Oh (ATLAS Collaboration)},
   Title = {Observation of VBS WZ production at 13 TeV},
   Journal = {Phys. Lett B (793) (2019) 469},
   Year = {2019},
   Key = {fds347957}
}

@article{fds375134,
   Author = {and S. Oh},
   Title = {Mu2e Run 1 Sensitivity Projections for the Neutrinoless mu-
             --> e- Conversion Search in Aluminum},
   Journal = {Universe 2023, 9(1), 54},
   Year = {2023},
   Key = {fds375134}
}


%% Papers Submitted   
@article{fds368743,
   Author = {Mu2e collaboration},
   Title = {Mu2e Run I Sensitivity Projections for the Neutrinoless
             μ−→e− Conversion Search in Aluminum},
   Journal = {Universe},
   Year = {2022},
   Month = {October},
   Key = {fds368743}
}


%% Preprints   
@article{fds225677,
   Author = {mu2e collaboration},
   Title = {Mu2e Technical Design Report},
   Year = {2014},
   Month = {November},
   Key = {fds225677}
}