Publications of Roxanne P. Springer    :chronological  alphabetical  combined listing:

%% Books   
@book{fds52849,
   Author = {R. Springer and T.B. Bunton and T. Mehen},
   Title = {Heavy Hadron Chiral Perturbation Theory Applied to the
             Charmed Meson Parity Partners},
   Booktitle = {proceedings of Chiral Dynamics, Theory and
             Experiment},
   Publisher = {World Scientific, Singapore},
   Year = {2006},
   Key = {fds52849}
}

@book{fds4091,
   Author = {R. P. Springer},
   Title = {An Effective Theory of QCD for Hyperons and
             Hypernuclei},
   Booktitle = {Proceedings of the Japanese Hadron Facility 1998
             Conference},
   Year = {1998},
   Month = {Spring},
   Key = {fds4091}
}


%% Papers Published   
@article{fds323249,
   Author = {Margaryan, A and Springer, RP and Vanasse, J},
   Title = {scattering and the puzzle to next-to-next-to-next-to-leading
             order},
   Journal = {Physical Review C},
   Volume = {93},
   Number = {5},
   Year = {2016},
   Month = {May},
   url = {http://dx.doi.org/10.1103/PhysRevC.93.054001},
   Doi = {10.1103/PhysRevC.93.054001},
   Key = {fds323249}
}

@article{fds323250,
   Author = {Schindler, MR and Springer, RP and Vanasse, J},
   Title = {Large- limit reduces the number of independent few-body
             parity-violating low-energy constants in pionless effective
             field theory},
   Journal = {Physical Review C},
   Volume = {93},
   Number = {2},
   Year = {2016},
   Month = {February},
   url = {http://dx.doi.org/10.1103/PhysRevC.93.025502},
   Doi = {10.1103/PhysRevC.93.025502},
   Key = {fds323250}
}

@article{fds323251,
   Author = {Margaryan, A and Vanasse, J and Springer, RP},
   Title = {Non-relativistic Neutron Deuteron Scattering},
   Journal = {EPJ Web of Conferences},
   Volume = {113},
   Pages = {08012-08012},
   Editor = {Elster, C and Phillips, DR and Roberts, CD},
   Year = {2016},
   url = {http://dx.doi.org/10.1051/epjconf/201611308012},
   Doi = {10.1051/epjconf/201611308012},
   Key = {fds323251}
}

@article{fds248391,
   Author = {Vanasse, J and Egolf, DA and Kerin, J and König, S and Springer,
             RP},
   Title = {and scattering to next-to-leading order in pionless
             effective field theory},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {89},
   Number = {6},
   Pages = {064003},
   Year = {2014},
   Month = {June},
   ISSN = {0556-2813},
   url = {http://dx.doi.org/10.1103/PhysRevC.89.064003},
   Doi = {10.1103/PhysRevC.89.064003},
   Key = {fds248391}
}

@article{fds248393,
   Author = {Schindler, MR and Springer, RP},
   Title = {The theory of parity violation in few-nucleon
             systems},
   Journal = {Progress in Particle and Nuclear Physics},
   Volume = {72},
   Pages = {1-43},
   Editor = {A. Faessler},
   Year = {2013},
   Month = {September},
   ISSN = {0146-6410},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000322931000001&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Doi = {10.1016/j.ppnp.2013.05.002},
   Key = {fds248393}
}

@article{fds248394,
   Author = {Margaryan, A and Springer, RP},
   Title = {Using the decay psi (4160) -> X(3872) gamma to probe the
             molecular content of the X(3872)},
   Journal = {Physical Review D},
   Volume = {88},
   Number = {1},
   Year = {2013},
   Month = {July},
   ISSN = {1550-7998},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000321839500002&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Doi = {10.1103/PhysRevD.88.014017},
   Key = {fds248394}
}

@article{fds248408,
   Author = {Griesshammer, HW and Schindler, MR and Springer,
             RP},
   Title = {Parity-violating neutron spin rotation in hydrogen and
             deuterium},
   Journal = {The European Physical Journal A - Hadrons and
             Nuclei},
   Volume = {48},
   Number = {1},
   Pages = {7},
   Year = {2012},
   Month = {January},
   ISSN = {1434-6001},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000300285400004&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Doi = {10.1140/epja/i2012-12007-8},
   Key = {fds248408}
}

@article{fds248409,
   Author = {Mehen, T and Springer, R},
   Title = {Radiative Decays X(3872)->psi(2S) gamma and psi(4040)
             ->X(3872) gamma},
   Journal = {Phys. Rev. D},
   Volume = {83},
   Pages = {094009},
   Year = {2011},
   Month = {January},
   Key = {fds248409}
}

@article{fds248406,
   Author = {Mehen, T and Springer, R},
   Title = {Radiative decays X(3872)→ψ(2S)γ and ψ(4040)→X(3872)
             γ in effective field theory},
   Journal = {Physical Review D - Particles, Fields, Gravitation, and
             Cosmology},
   Volume = {83},
   Number = {9},
   Year = {2011},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.83.094009},
   Abstract = {Heavy hadron chiral perturbation theory (HHχPT) and XEFT
             are applied to the decays X(3872)→ψ(2S)γ and
             ψ(4040)→X(3872)γ under the assumption that the X(3872)
             is a molecular bound state of neutral charm mesons. In these
             decays the emitted photon energies are 181MeV and 165MeV,
             respectively, so HHχPT can be used to calculate the
             underlying D0D ̄0*+D̄0D0 *→ψ(2S)γ or ψ(4040)→(D0D
             ̄0*+D̄0D0*) γ transition. These amplitudes are matched
             onto XEFT to obtain decay rates. The decays receive
             contributions from both long-distance and short-distance
             processes. We study the polarization of the ψ(2S) in the
             decay X(3872)→ψ(2S)γ and the angular distribution of
             X(3872) in the decay ψ(4040)→X(3872)γ and find they can
             be used to differentiate between different decay mechanisms
             as well as discriminate between 2-+ and 1++ quantum number
             assignments of the X(3872). © 2011 American Physical
             Society.},
   Doi = {10.1103/PhysRevD.83.094009},
   Key = {fds248406}
}

@article{fds248407,
   Author = {Mehen, T and Springer, R},
   Title = {X(3872) -> psi(2S) gamma and psi(4040) -> X(3872)
             gamma},
   Journal = {Phys Rev D83 094009},
   Year = {2011},
   Key = {fds248407}
}

@article{fds184764,
   Author = {R. Springer},
   Title = {Parity violation in the NN interaction},
   Volume = {3},
   Booktitle = {EPJ Web of Conferences, 19th International IUPAP Conference
             on Few- Body Problems in Physics, University of Bonn,
             Germany, 31 Aug – 5 Sep 2009},
   Editor = {E. Epelbaum and H.-W. Hammer and U.-G. Meissner},
   Year = {2010},
   url = {http://dx.doi.org/10.1051/epjconf/20100307001},
   Doi = {10.1051/epjconf/20100307001},
   Key = {fds184764}
}

@article{fds248410,
   Author = {Schindler, MR and Springer, RP},
   Title = {Two parity-violating asymmetries from np → dγ in pionless
             effective field theories},
   Journal = {Nuclear Physics A},
   Volume = {846},
   Number = {1-4},
   Pages = {51-62},
   Year = {2010},
   ISSN = {0375-9474},
   url = {http://dx.doi.org/10.1016/j.nuclphysa.2010.06.002},
   Abstract = {We consider parity-violating observables from the processes
             n→p→dγ and np → dγ. We perform calculations using
             pionless effective field theory both with and without
             explicit dibaryon fields. After combining these results with
             ones we have already obtained on parity-violating
             asymmetries in N → N scattering, experimental input would
             in principle allow the extraction of all five parameters
             occurring at leading order in the parity-violating
             Lagrangian. © 2010 Elsevier B.V.},
   Doi = {10.1016/j.nuclphysa.2010.06.002},
   Key = {fds248410}
}

@article{fds248395,
   Author = {Springer, RP and Phillips, DR and Schindler, MJ},
   Title = {Parity Violation in the NN System},
   Journal = {EPJ Web of Conferences},
   Volume = {3},
   Year = {2009},
   ISSN = {2100-014X},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000290401000120&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Doi = {10.1051/epjconf/20100307001},
   Key = {fds248395}
}

@article{fds248403,
   Author = {Canham, DL and Hammer, H-W and Springer, RP},
   Title = {Scattering of D and D* mesons off the X(3872)},
   Journal = {Physical Review D - Particles, Fields, Gravitation, and
             Cosmology},
   Volume = {80},
   Number = {1},
   Year = {2009},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.80.014009},
   Abstract = {Both the mass (just below the D*0D̄0 threshold) and the
             likely quantum numbers (JPC=1++) of the X(3872) suggest that
             it is either a weakly bound hadronic "molecule"
             (X(3872)∼1/2[D*0D̄0+D̄*0D0]) or a virtual state of
             charmed mesons. Assuming the X(3872) is a weakly bound
             molecule, the scattering of neutral D and D* mesons off the
             X(3872) can be predicted from the X(3872) binding energy. We
             calculate the phase shifts and cross section for scattering
             of D0 and D*0 mesons and their antiparticles off the X(3872)
             in an effective field theory for short-range interactions.
             This provides another example of a three-body process, along
             with those in nuclear and atomic systems, that displays
             universal properties. It may be possible to extract the
             scattering within the final state interactions of Bc decays
             and/or other LHC events. © 2009 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.80.014009},
   Key = {fds248403}
}

@article{fds248411,
   Author = {Phillips, DR and Schindler, MR and Springer, RP},
   Title = {An effective-field-theory analysis of low-energy
             parity-violation in nucleon-nucleon scattering},
   Journal = {Nuclear Physics A},
   Volume = {822},
   Number = {1-4},
   Pages = {14-32},
   Year = {2009},
   ISSN = {0375-9474},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000265621600001&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We analyze parity-violating nucleon-nucleon scattering at
             energies E < mπ2 / M using the effective field theory
             appropriate for this regime. The minimal Lagrangian for
             short-range parity-violating NN interactions is written in
             an operator basis that encodes the five partial-wave
             transitions that dominate at these energies. We calculate
             the leading-order relationships between parity-violating NN
             asymmetries and the coefficients in the Lagrangian and also
             discuss the size of sub-leading corrections. We conclude
             with a discussion of further observables needed to
             completely determine the leading-order Lagrangian. © 2009
             Elsevier B.V. All rights reserved.},
   Doi = {10.1016/j.nuclphysa.2009.02.011},
   Key = {fds248411}
}

@article{fds248412,
   Author = {Bedaque, PF and Buchoff, MI and Cherman, A and Springer,
             RP},
   Title = {Can fermions save large N dimensional reduction?},
   Journal = {Journal of High Energy Physics},
   Volume = {2009},
   Number = {10},
   Pages = {070},
   Year = {2009},
   ISSN = {1126-6708},
   url = {http://dx.doi.org/10.1088/1126-6708/2009/10/070},
   Abstract = {This paper explores whether Eguchi-Kawai reduction for gauge
             theories with adjoint fermions is valid. The Eguchi-Kawai
             reduction relates gauge theories in different numbers of
             dimensions in the large N limit provided that certain
             conditions are met. In principle, this relation opens up the
             possibility of learning about the dynamics of 4D gauge
             theories through techniques only available in lower
             dimensions. Dimensional reduction can be understood as a
             special case of large N equivalence between theories related
             by an orbifold projection. In this work, we focus on the
             simplest case of dimensional reduction, relating a 4D gauge
             theory to a 3D gauge theory via an orbifold projection. A
             necessary condition for the large N equivalence between the
             4D and 3D theories to hold is that certain discrete
             symmetries in the two theories must not be broken
             spontaneously. In pure 4D Yang-Mills theory, these
             symmetries break spontaneously as the size of one of the
             spacetime dimensions shrinks. An analysis of the effect of
             adjoint fermions on the relevant symmetries of the 4D theory
             shows that the fermions help stabilize the symmetries. We
             consider the same problem from the point of view of the
             lower dimensional 3D theory and find that, surprisingly,
             adjoint fermions are not generally enough to stabilize the
             necessary symmetries of the 3D theory. In fact, a rich phase
             diagram arises, with a complicated pattern of symmetry
             breaking. We discuss the possible causes and consequences of
             this finding. © 2009 SISSA.},
   Doi = {10.1088/1126-6708/2009/10/070},
   Key = {fds248412}
}

@article{fds248413,
   Author = {Canham, D and Hammer, HW and Springer, R},
   Title = {On the scattering of D and D* mesons off the
             X(3872)},
   Journal = {Phys Rev D},
   Volume = {D80},
   Pages = {014009},
   Year = {2009},
   Key = {fds248413}
}

@article{fds248392,
   Author = {Springer, RP},
   Title = {HHChPT applied to the charmed-strange parity
             partners},
   Journal = {Chiral Dynamics 2006 - Proceedings of the 5th International
             Workshop on Chiral Dynamics, Theory and Experiment, CD
             2006},
   Pages = {302-303},
   Year = {2007},
   Month = {December},
   Abstract = {We apply heavy hadron chiral perturbation theory (HHChPT) to
             study the properties of the even- and odd-parity
             charmed-strange mesons. We find that the experimental masses
             and electromagnetic decay rates are consistent with
             HHChPT.We consider the hypothesis that the even-parity
             states are molecules. An RG analysis shows that once the
             HHChPT parameter set overlaps with the parity doubling
             model, the parameters remain at those values. Finally, the
             implications for the bottom-strange system are
             described.},
   Key = {fds248392}
}

@article{fds248414,
   Author = {Mehen, T and Springer, RP},
   Title = {Even- and Odd-Parity Charmed Meson Masses in Heavy Hadron
             Chiral Perturbation Theory},
   Journal = {Phys Rev D},
   Volume = {72},
   Number = {034006},
   Pages = {1-12},
   Year = {2005},
   Month = {Spring},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.034006},
   Abstract = {We derive mass formulas for the ground state, JP=0- and 1-,
             and first excited even-parity, JP=0+ and 1+, charmed mesons
             including one-loop chiral corrections and O(1/mc)
             counterterms in heavy hadron chiral perturbation theory. We
             show that including these counterterms is critical for
             fitting the current data. We find that certain parameter
             relations in the parity doubling model are not renormalized
             at one-loop, providing a natural explanation for the
             observed equality of the hyperfine splittings of ground
             state and excited doublets. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.72.034006},
   Key = {fds248414}
}

@article{fds304618,
   Author = {Mehen, T and Springer, RP},
   Title = {Even- and odd-parity charmed meson masses in heavy hadron
             chiral perturbation theory},
   Journal = {Physical Review D - Particles, Fields, Gravitation, and
             Cosmology},
   Volume = {72},
   Number = {3},
   Pages = {1-12},
   Year = {2005},
   ISSN = {1550-7998},
   url = {http://dx.doi.org/10.1103/PhysRevD.72.034006},
   Abstract = {We derive mass formulas for the ground state, JP=0- and 1-,
             and first excited even-parity, JP=0+ and 1+, charmed mesons
             including one-loop chiral corrections and O(1/mc)
             counterterms in heavy hadron chiral perturbation theory. We
             show that including these counterterms is critical for
             fitting the current data. We find that certain parameter
             relations in the parity doubling model are not renormalized
             at one-loop, providing a natural explanation for the
             observed equality of the hyperfine splittings of ground
             state and excited doublets. © 2005 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.72.034006},
   Key = {fds304618}
}

@article{fds248425,
   Author = {Mehen, T and Springer, RP},
   Title = {Heavy-quark symmetry and the electromagnetic decays of
             excited charmed strange mesons},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {70},
   Number = {7},
   Pages = {074014-1-074014-12},
   Year = {2004},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.70.074014},
   Abstract = {Heavy-hadron chiral perturbation theory (HHχPT) is applied
             to the decays of the even-parity charmed strange mesons,
             Ds0(2317) and Ds1(2460). Heavy-quark spin-symmetry predicts
             the branching fractions for the three electromagnetic decays
             of these states to the ground states Ds and Ds* in terms of
             a single parameter. The resulting predictions for two of the
             branching fractions are significantly higher than current
             upper limits from the CLEO experiment. Leading corrections
             to the branching ratios from chiral loop diagrams and
             spin-symmetry violating operators in the HHχPT Lagrangian
             can naturally account for this discrepancy. Finally the
             proposal that the Ds0(2317) (D s1(2460)) is a hadronic bound
             state of a D(D*) meson and a kaon is considered. Leading
             order predictions for electromagnetic branching ratios in
             this molecular scenario are in very poor agreement with
             existing data.},
   Doi = {10.1103/PhysRevD.70.074014},
   Key = {fds248425}
}

@article{fds248426,
   Author = {Egolf, DA and Springer, RP and Urban, J},
   Title = {SU(3) predictions for weak decays of doubly heavy baryons,
             including SU(3) breaking terms},
   Journal = {Physical Review D: Particles, Fields, Gravitation and
             Cosmology},
   Volume = {68},
   Number = {1},
   Pages = {013003},
   Year = {2003},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.68.013003},
   Abstract = {We find expressions for the weak decay amplitudes of baryons
             containing two b quarks (or one b and one c quark - many
             relationships are the same) in terms of unknown reduced
             matrix elements. This project was originally motivated by
             the request of the Fermilab run II b Physics Workshop
             organizers for a guide to experimentalists in their search
             for as yet unobserved hadrons. We include an analysis of
             linear SU(3) breaking terms in addition to relationships
             generated by unbroken SU(3) symmetry, and relate these to
             expressions in terms of the complete set of possible reduced
             matrix elements. © 2003 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.68.013003},
   Key = {fds248426}
}

@article{fds248428,
   Author = {Savage, MJ and Springer, RP},
   Title = {The anapole form factor of the deuteron},
   Journal = {Nuclear Physics A},
   Volume = {686},
   Number = {1-4},
   Pages = {413-428},
   Year = {2001},
   Month = {Summer},
   url = {http://dx.doi.org/10.1016/S0375-9474(00)00568-6},
   Abstract = {We find the leading-order result for the anapole form factor
             of the deuteron using effective field theory. The momentum
             dependence of the anapole form factor is different from that
             of the matrix element of the strange currents in the
             deuteron, which may provide a way for disentangling these
             two competing effects when analyzing parity-violating
             electron-deuteron scattering experiments. We give closed
             form expressions for both the form factor and integrals
             often encountered in the NN effective field theory. © 2001
             Elsevier Science B.V. All rights reserved.},
   Doi = {10.1016/S0375-9474(00)00568-6},
   Key = {fds248428}
}

@article{fds248402,
   Author = {Egolf, DA and Melnikov, IV and Springer, RP},
   Title = {Weak nonleptonic Ω- decay in chiral perturbation
             theory},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {451},
   Number = {3-4},
   Pages = {267-274},
   Year = {1999},
   Abstract = {We calculate the weak nonleptonic decay of the Ω- baryon to
             octet final states in heavy baryon chiral perturbation
             theory (HBChPT). We include the one-loop leading logarithmic
             effects and show that this improves the universality of the
             HBChPT constants. © 1999 Published by Elsevier Science B.V.
             All rights reserved.},
   Key = {fds248402}
}

@article{fds248427,
   Author = {Springer, RP},
   Title = {Heavy baryon chiral perturbation theory and the weak
             nonleptonic p-wave decays of the baryon octet},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {461},
   Number = {3},
   Pages = {167-174},
   Year = {1999},
   Month = {Spring},
   Abstract = {Considerable confusion in the literature about heavy baryon
             chiral perturbation theory, its convergence properties, and
             appropriate calculational techniques, make it timely to
             discuss the nonleptonic p-wave decays of the octet of
             baryons. We present model independent results. © 1999
             Published by Elsevier Science B.V. All rights
             reserved.},
   Key = {fds248427}
}

@article{fds248431,
   Author = {Kaplan, DB and Savage, MJ and Springer, RP and Wise,
             MB},
   Title = {An effective field theory calculation of the parity
             violating asymmetry in n + p > d +
             γ},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {449},
   Number = {1-2},
   Pages = {1-5},
   Year = {1999},
   Month = {Fall},
   Abstract = {Weak interactions are expected to induce a parity violating
             pion-nucleon coupling, hπNN(1). This coupling should be
             measurable in a proposed experiment to study the parity
             violating asymmetry Aγ in the process n→ + p → d + γ.
             We compute the leading dependence of Aγ on the coupling
             hπNN(1) using recently developed effective field theory
             techniques and find an asymmetry of Aγ = + 0.17 hπNN(1) at
             leading order. This asymmetry has the opposite sign to that
             given by Desplanques and Missimer. © 1999 Published by
             Elsevier Science B.V. All rights reserved.},
   Key = {fds248431}
}

@article{fds248429,
   Author = {Chen, J-W and Griesshammer, HW and Savage, MJ and Springer,
             RP},
   Title = {Gamma-Deuteron Compton Scattering in Effective Field
             Theory},
   Journal = {Nuclear Physics},
   Volume = {A 644},
   Number = {3},
   Pages = {245},
   Year = {1998},
   Month = {Fall},
   Abstract = {The differential cross section for γ-deuteron Compton
             scattering is computed to next-to-leading order (NLO) in an
             effective field theory that describes nucleon-nucleon
             interactions below the pion production threshold.
             Contributions at NLO include the nucleon isoscalar electric
             polarizability from its 1/mπ behavior in the chiral
             limit. The parameter-free prediction of the γ-deuteron
             differential cross section at NLO is in good agreement with
             data. © 1998 Elsevier Science B.V.},
   Key = {fds248429}
}

@article{fds248430,
   Author = {Egolf, DA and Melnikov, IV and Springer, RP},
   Title = {Weak Nonleptonic Omega Decay in Chiral Perturbation
             Theory},
   Journal = {Physics Letters},
   Volume = {B451},
   Number = {267},
   Year = {1998},
   Month = {Fall},
   Key = {fds248430}
}

@article{fds248401,
   Author = {Savage, MJ and Springer, RP},
   Title = {NNK and ΛΛK amplitudes in chiral perturbation
             theory},
   Journal = {Nuclear Physics A},
   Volume = {639},
   Number = {1-2},
   Pages = {325c-328c},
   Year = {1998},
   Abstract = {We explore the S-wave and P-wave amplitudes for NNK and
             ΛΛK interactions using chiral perturbation theory to
             script O sign(ms log ms). In contrast to the large
             corrections found in P-wave amplitudes in the nonleptonic
             decay of octet baryons, the NNK amplitudes receive only
             small corrections to their tree-level values. The
             uncertainty in the ΛΛK amplitudes is found to be
             large.},
   Key = {fds248401}
}

@article{fds248432,
   Author = {Savage, MJ and Springer, RP},
   Title = {Parity violation in effective field theory and the deuteron
             anapole moment},
   Journal = {Nuclear Physics A},
   Volume = {644},
   Number = {3},
   Pages = {235-244},
   Year = {1998},
   Month = {Summer},
   Abstract = {Effective field theory, including pions, provides a
             consistent and systematic description of nucleon-nucleon
             strong interactions up to center-of-mass momentum p ∼ 300
             MeV per nucleon. We describe the inclusion of hadronic
             parity violation into this effective field theory and find
             an analytic form for the deuteron anapole moment at leading
             order in the expansion. © 1998 Elsevier Science
             B.V.},
   Key = {fds248432}
}

@article{fds248433,
   Author = {Chen, J-W and Grießhammer, HW and Savage, MJ and Springer,
             RP},
   Title = {The polarizability of the deuteron},
   Journal = {Nuclear Physics A},
   Volume = {644},
   Number = {3},
   Pages = {221-234},
   Year = {1998},
   Month = {Summer},
   Abstract = {The scalar and tensor polarizabilities of the deuteron are
             calculated using the recently developed effective field
             theory that describes nucleon-nucleon interactions. Leading
             and next-to-leading order contributions in the perturbative
             expansion predict a scalar electric polarizability of αE0 =
             0.595 fm3. The tensor electric polarizability receives
             contributions starting at next-to-leading order from the
             exchange of a single potential pion and is found to be αE2
             = -0.062 fm3. We compute the leading contributions to the
             scalar and tensor magnetic polarizabilities, finding βM0 =
             0.067 fm3 and βM2 = 0.195 fm3. © 1998 Elsevier Science
             B.V.},
   Key = {fds248433}
}

@article{fds248434,
   Author = {Savage, MJ and Springer, RP},
   Title = {Weak ΛΛK0 interaction},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {57},
   Number = {3},
   Pages = {1478-1484},
   Year = {1998},
   Month = {Spring},
   ISSN = {0556-2813},
   url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000072596600056&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
   Abstract = {We calculate the leading contribution to the weak ΛΛK
             coupling in heavy baryon chiral perturbation theory,
             including the SU(3) breaking terms arising at one loop. This
             coupling gives the leading one-boson exchange amplitude for
             the process ΛΛ → Λn and is an important component in
             understanding the decay of ΛΛ hypernuclei. We predict the
             S-wave and P-wave amplitudes to be found in the ranges
             -0.5≲A(S)≲1.1 and -8.9≲A(P)≲-0.7,
             respectively.},
   Doi = {10.1103/PhysRevC.57.1478},
   Key = {fds248434}
}

@article{fds304617,
   Author = {Chen, J-W and Grießhammer, HW and Savage, MJ and Springer,
             RP},
   Title = {γ-deuteron Compton scattering in effective field
             theory},
   Journal = {Nuclear Physics A},
   Volume = {644},
   Number = {3},
   Pages = {245-259},
   Year = {1998},
   Abstract = {The differential cross section for γ-deuteron Compton
             scattering is computed to next-to-leading order (NLO) in an
             effective field theory that describes nucleon-nucleon
             interactions below the pion production threshold.
             Contributions at NLO include the nucleon isoscalar electric
             polarizability from its 1/mπ behavior in the chiral limit.
             The parameter-free prediction of the γ-deuteron
             differential cross section at NLO is in good agreement with
             data. © 1998 Elsevier Science B.V.},
   Key = {fds304617}
}

@booklet{Savage96,
   Author = {Savage, MJ and Springer, RP},
   Title = {Kaon-nucleon couplings for weak decays of hypernuclei (vol
             C53, pg 441, 1996)},
   Journal = {Physical Review C},
   Volume = {54},
   Number = {5},
   Pages = {2786-2786},
   Year = {1996},
   Month = {November},
   Key = {Savage96}
}

@booklet{Engel96,
   Author = {Engel, J and Frampton, PH and Springer, RP},
   Title = {Effective Lagrangians and parity-conserving time-reversal
             violation at low energies},
   Journal = {Physical Review D - Particles, Fields, Gravitation and
             Cosmology},
   Volume = {53},
   Number = {9},
   Pages = {5112-5114},
   Year = {1996},
   Abstract = {Using effective Lagrangians, we argue that any
             time-reversal-violating but parity-conserving effects are
             too small to be observed in flavor-conserving nuclear
             processes without dramatic improvement in experimental
             accuracy. In the process we discuss other arguments that
             have appeared in the literature.},
   Key = {Engel96}
}

@booklet{Savage96a,
   Author = {Savage, MJ and Springer, RP},
   Title = {Kaon-nucleon couplings for weak decays of
             hypernuclei},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {53},
   Number = {1},
   Pages = {441-447},
   Year = {1996},
   url = {http://dx.doi.org/10.1103/PhysRevC.53.441},
   Abstract = {We investigate the weak kaon-nucleon (NNK) S-wave and P-wave
             interactions using heavy baryon chiral perturbation theory.
             The leading one-loop SU(3) breaking contributions to the
             ppK, pnK, and nnK couplings are computed. We find that they
             suppress all NNK amplitudes by 30% to 50%. The ratio of
             neutron-induced to proton-induced hypernuclear decay widths
             is sensitive to such reductions. It has been argued that the
             discrepancy between the predicted and observed P-wave
             amplitudes in Δs = 1 hyperon decay results from an
             accidental cancellation between tree-level amplitudes, and
             is not a fundamental problem for chiral perturbation theory.
             Agreement between experimentally determined NNK P-wave
             amplitudes and our estimates would support this
             explanation.},
   Doi = {10.1103/PhysRevC.53.441},
   Key = {Savage96a}
}

@booklet{Butler94,
   Author = {Butler, MN and Savage, MJ and Springer, RP},
   Title = {Electromagnetic moments of the baryon decuplet},
   Journal = {Physical Review D: Particles, Fields, Gravitation and
             Cosmology},
   Volume = {49},
   Number = {7},
   Pages = {3459-3465},
   Year = {1994},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.49.3459},
   Abstract = {We compute the leading contributions to the magnetic dipole
             and electric quadrupole moments of the baryon decuplet in
             chiral perturbation theory. The measured value for the
             magnetic moment of the Ω- is used to determine the local
             counterterm for the magnetic moments. We compare the chiral
             perturbation theory predictions for the magnetic moments of
             the decuplet with those of the baryon octet and find
             reasonable agreement with the predictions of the large-Nc
             limit of QCD. The leading contribution to the quadrupole
             moment of the Δ and other members of the decuplet comes
             from one-loop graphs. The pionic contribution is shown to be
             proportional to Iz (and so will not contribute to the
             quadrupole moment of I=0 nuclei), while the contribution
             from kaons has both isovector and isoscalar components. The
             chiral logarithmic enhancement of both pion and kaon loops
             has a coefficient that vanishes in the SU(6) limit. The
             third allowed moment, the magnetic octupole, is shown to be
             dominated by a local counterterm with corrections arising at
             two loops. We briefly mention the strange counterparts of
             these moments. © 1994 The American Physical
             Society.},
   Doi = {10.1103/PhysRevD.49.3459},
   Key = {Butler94}
}

@booklet{Butler93,
   Author = {Butler, MN and Savage, MJ and Springer, RP},
   Title = {Erratum and addendum to E2/M1 mixing ratio of Δ→Nγ and
             hyperon resonance radiative decay},
   Journal = {Physics Letters B},
   Volume = {314},
   Number = {1},
   Pages = {122-124},
   Year = {1993},
   ISSN = {0370-2693},
   Abstract = {We correct an error in the definition of our amplitudes, and
             then discuss using γ-γ correlations to find the ratio of
             electric quadrupole to magnetic dipole transitions in the
             electromagnetic production and decay of the Δ. ©
             1993.},
   Key = {Butler93}
}

@booklet{Butler93b,
   Author = {Butler, MN and Savage, MJ and Springer, RP},
   Title = {Strong and electromagnetic decays of the baryon
             decuplet},
   Journal = {Nuclear Physics B},
   Volume = {399},
   Number = {1},
   Pages = {69-85},
   Year = {1993},
   Abstract = {To explore further the role that QCD symmetries play on
             hadron dynamics, we discuss the radiative decay of the
             baryon decuplet to the baryon octet and compute the leading
             non-analytic SU(3) violating corrections induced at the
             one-loop level. In the limit of exact flavour SU(3) symmetry
             two of the possible decay modes are forbidden and the rates
             for these two decays are dominated by loop corrections.
             There is only one SU(3) conserving contact term at leading
             order in chiral perturbation theory for the radiative
             decays. We determine its coefficient from the observed
             branching ratio for Δ → Nγ and from the present upper
             limit on Ξ*0 → Ξ0γ. We then predict the branching
             fractions for Σ*- → Σ-γ, Σ*0 → Λγ, Σ*0 → Σ0γ,
             Σ*+ → Σ+γ, Ξ*0γ → Ξ0γ and Ξ*- → Ξ-γ. Some of
             the decay modes are predicted to have branching fractions
             near the current experimental upper limit and could possibly
             be observed in the near future. The leading corrections to
             the octet-decuplet-meson strong coupling constant, script c
             sign, are computed at one-loop and the strong decay rates of
             the Δ, Σ* and Ξ* allow us to determine |script c sign| =
             1.2±0.1 and script K = -2.2±0.6, in remarkable agreement
             with predictions based on spin-flavour symmetry. We
             calculate the Δ pole graph contribution to the
             polarisability of the nucleon to order 1/Λχ2 in chiral
             perturbation theory.},
   Key = {Butler93b}
}

@booklet{Butler93a,
   Author = {Butler, MN and Savage, MJ and Springer, RP},
   Title = {Probing hadronic structure with the decay
             Nl+l-},
   Journal = {Physical Review C - Nuclear Physics},
   Volume = {48},
   Number = {2},
   Pages = {917-919},
   Year = {1993},
   ISSN = {0556-2813},
   url = {http://dx.doi.org/10.1103/PhysRevC.48.917},
   Abstract = {We compute the branching ratio for Ne+e- and N+- in chiral
             perturbation theory and find that both decays should be
             observable at the Continuous Electron Beam Accelerator
             Facility. With sufficiently low thresholds on the e+e-
             invariant mass a branching ratio of 10-5 may be observed for
             Ne+e-. For the N+- decay mode we predict a branching ratio
             of 3×10-7. The dependence of the M1 and E2 amplitudes on
             the momentum transfer will provide a useful test of chiral
             perturbation theory which predicts 20% variation over the
             allowed kinematic range. © 1993 The American Physical
             Society.},
   Doi = {10.1103/PhysRevC.48.917},
   Key = {Butler93a}
}

@booklet{Butler93c,
   Author = {Butler, MN and Savage, MJ and Springer, RP},
   Title = {E2/M1 mixing ratio of Δ→Nγ and hyperon resonance
             radiative decay},
   Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
             High-Energy Physics},
   Volume = {304},
   Number = {3-4},
   Pages = {353-358},
   Year = {1993},
   Abstract = {We complete the leading contribution to the E2/M1 mixing
             ratio of the decay Δ→Nγ in heavy baryon chiral
             perturbation theory. We find the mixing ratio to be
             4%≲|δE2/M1|≲11%, much larger than estimates based on
             the quark model and other hadronic models. We also compute
             the mixing ratio for the radiative decay of the hyperon
             resonances. The decays Σ*+→Σ+γ and Ξ*-→Ξ-γ provide
             a particularly sensitive probe of deviations from heavy
             baryon spin-flavour SU(6).},
   Key = {Butler93c}
}

@booklet{Savage91,
   Author = {Savage, MJ and Springer, RP},
   Title = {Very charming baryons},
   Journal = {International Journal Of Modern Physics A},
   Volume = {6},
   Number = {10},
   Pages = {1701-1712},
   Year = {1991},
   Month = {April},
   Key = {Savage91}
}

@article{fds248397,
   Author = {Dai, J and Savage, MJ and Liu, J and Springer, R},
   Title = {Low energy effective hamiltonian for ΔI = 1 nuclear parity
             violation and nucleonic strangeness},
   Journal = {Physics Letters B},
   Volume = {271},
   Number = {3-4},
   Pages = {403-409},
   Year = {1991},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/0370-2693(91)90108-3},
   Abstract = {We calculate the low energy effective hamiltonian for
             isovector (ΔI = 1) nuclear parity violation, including the
             effects of heavy quarks s, c and b. At the hadronic scale,
             the hamiltonian contains four-quark operators of the u, d,
             and s quarks whose coefficients contain leading logarithmic
             QCD corrections from running between the weak scale and the
             hadronic scale. The coefficients of the operators involving
             the s quark are substantially larger than those of the
             operators involving only the u and d quarks. Recent EMC
             measurements of the spin-dependent proton structure
             functions g1p (x) and measurements of the low-Q2 axial
             nucleon-Z0 coupling from neutrino scattering indicate that
             the nucleon matrix element of the strange vector axial
             current is substantial. Assumming that the weak amplitude
             factorizes, this matrix element gives rise to an enhancement
             in the weak isovector parity violating NNρ{variant}
             coupling, and consequently an enhancement of hρ{variant}1.
             © 1991.},
   Doi = {10.1016/0370-2693(91)90108-3},
   Key = {fds248397}
}

@article{fds248398,
   Author = {Grinstein, B and Springer, R and Wise, MB},
   Title = {Strong-interaction effects in weak radiative B̄-meson
             decay},
   Journal = {Nuclear Physics B},
   Volume = {339},
   Number = {2},
   Pages = {269-309},
   Year = {1990},
   Abstract = {Strong-interaction corrections to the effective hamiltonian
             for weak radiative B̄-meson decay (i.e., B̄ → Xs-γ,
             where Xs denotes a strange hadronic final state) are
             calculated using the leading logarithmic approximation. The
             inclusive rate for decays B̄ → Xsγ, where the energy of
             the photon is large, is computed in the standard model with
             minimal particle content and in extensions of the minimal
             standard model with two Higgs doublets.},
   Key = {fds248398}
}

@booklet{Savage90,
   Author = {Savage, MJ and Springer, RP},
   Title = {SU(3) predictions for charmed-baryon decays},
   Journal = {Physical Review D: Particles, Fields, Gravitation and
             Cosmology},
   Volume = {42},
   Number = {5},
   Pages = {1527-1543},
   Year = {1990},
   ISSN = {0556-2821},
   url = {http://dx.doi.org/10.1103/PhysRevD.42.1527},
   Abstract = {The charmed baryons c+, źc1+, źc10 and ©c0 can only
             weakly decay to lower-mass baryons and mesons. We derive
             relations between the decay rates of these particles based
             on flavor SU(3). Two-body and three-body nonleptonic decays
             are explored along with semileptonic decays. © 1990 The
             American Physical Society.},
   Doi = {10.1103/PhysRevD.42.1527},
   Key = {Savage90}
}

@article{fds248396,
   Author = {Grinstein, B and Springer, R and Wise, MB},
   Title = {Effective hamiltonian for weak radiative B-meson
             decay},
   Journal = {Physics Letters B},
   Volume = {202},
   Number = {1},
   Pages = {138-144},
   Year = {1988},
   ISSN = {0370-2693},
   url = {http://dx.doi.org/10.1016/0370-2693(88)90868-4},
   Abstract = {The inclusive rate for decay of a B-meson to a hard photon
             and strange hadronic final states (i.e., B→γXs with
             Xs=K*, etc.), is likely to be dominated by short-distance
             physics which gives rise to an effective hamiltonian that is
             a magnetic-moment-type operator. Strong interaction
             corrections to this hamiltonian are computed in the leading
             logarithmic approximation. © 1988.},
   Doi = {10.1016/0370-2693(88)90868-4},
   Key = {fds248396}
}

@article{fds221147,
   Author = {A. Margaryan and R. Springer},
   Title = {Using the decay Y(4160) -> X(3872) + photon to probe the
             molecular content of the X(3872)},
   Journal = {Phys Rev. D.},
   Volume = {88},
   Pages = {014017},
   url = {http://dx.doi.org/10.1103/PhysRevD.88.014017},
   Doi = {10.1103/PhysRevD.88.014017},
   Key = {fds221147}
}


%% Preprints   
@article{fds17515,
   Author = {D. Egolf and R. Springer},
   Title = {SU(3) predictions for weak decays of doubly heavy
             baryons},
   Journal = {DUKE-TH-00-207},
   Year = {2000},
   Key = {fds17515}
}


%% Other   
@misc{fds221149,
   Author = {M. Ahmed and A. Champagne and B. Holstein and C. Howell and M. Snow and R.
             Springer and Y. Wu},
   Title = {Parity Violation in Photonuclear Reactions at HIGS –
             Submission to Snowmass 2013: Intensity Frontier,
             arXiv:1307.8178},
   Year = {2013},
   Month = {July},
   Key = {fds221149}
}

@misc{fds212338,
   Author = {H. Gao and S.S. Jawalker and M.R. Schindler and W.M. Snow and R.
             Springer and Y. Wu},
   Title = {Parity Violation in Photonuclear Reactions at
             HIGS},
   Year = {2012},
   url = {http://www.phy.ornl.gov/funsym/positions/parityviolationatHIGS.pdf},
   Key = {fds212338}
}

@misc{fds212339,
   Author = {M.W. Ahmed and A.E. Champagne and C.R. Howell and W.M. Snow and R.P.
             Springer and Y. Wu},
   Title = {HIGS2: The Next Generation Compton $\gamma$-ray
             Source},
   Year = {2012},
   url = {http://www.tunl.duke.edu/documents/public/higs2_prospectus_31aug2012.pdf},
   Key = {fds212339}
}

@misc{fds17514,
   Author = {R. Springer},
   Title = {Hyperons and Hypernuclei},
   Booktitle = {Chiral Dynamics, Newport News, VA},
   Year = {2000},
   Key = {fds17514}
}