%% Papers Published
@article{fds376733,
Author = {Zhao, L and Arnault, EG and Larson, TFQ and Watanabe, K and Taniguchi,
T and Amet, F and Finkelstein, G},
Title = {Nonlocal transport measurements in hybrid quantum
Hall-superconducting devices},
Journal = {Physical Review B},
Volume = {109},
Number = {11},
Year = {2024},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevB.109.115416},
Abstract = {There has been a growing interest in hybrid quantum
Hall-superconductor devices, driven by the prospect to
realize exotic ground states and excitations with
non-Abelian exchange statistics. While the existing
experiments clearly demonstrate Andreev coupling between the
edge states and the superconductors, the question remains
whether the quantum coherence could propagate between
several superconducting contacts via chiral channels. To
answer this question, we have first extended the
Landauer-Büttiker (LB) formalism to samples with one
superconducting contact and found a remarkable agreement
within a series of measurements related to each other via
LB-type formulas. We have then switched to the case of
multiple superconducting contacts, and found that we can
describe the measurements self-consistently if we neglect
the superconducting phase coherence between multiple
contacts. We interpret this result as a negative answer to
the question posed above: the phase correlations between
multiple superconducting contacts are not established via
μm-long quantum Hall edge states. Looking forward, our
approach may find applications in the broader field of
topological superconductivity and proximal structures.
Possible violations of the self-consistency tests presented
here may be used as an indication that superconducting phase
coherence is induced in the quantum Hall
edges.},
Doi = {10.1103/PhysRevB.109.115416},
Key = {fds376733}
}
@article{fds374915,
Author = {Zhao, L and Iftikhar, Z and Larson, TFQ and Arnault, EG and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein, G},
Title = {Loss and Decoherence at the Quantum Hall-Superconductor
Interface.},
Journal = {Physical review letters},
Volume = {131},
Number = {17},
Pages = {176604},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.176604},
Abstract = {We perform a systematic study of Andreev conversion at the
interface between a superconductor and graphene in the
quantum Hall (QH) regime. We find that the probability of
Andreev conversion from electrons to holes follows an
unexpected but clear trend: the dependencies on temperature
and magnetic field are nearly decoupled. We discuss these
trends and the role of the superconducting vortices, whose
normal cores could both absorb and dephase the individual
electrons in a QH edge. Our Letter may pave the road to
engineering a future generation of hybrid devices for
exploiting superconductivity proximity in chiral
channels.},
Doi = {10.1103/physrevlett.131.176604},
Key = {fds374915}
}
@article{fds371253,
Author = {Chiles, J and Arnault, EG and Chen, C-C and Larson, TFQ and Zhao, L and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein,
G},
Title = {Nonreciprocal Supercurrents in a Field-Free Graphene
Josephson Triode.},
Journal = {Nano letters},
Volume = {23},
Number = {11},
Pages = {5257-5263},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1021/acs.nanolett.3c01276},
Abstract = {Superconducting diodes are proposed nonreciprocal circuit
elements that should exhibit nondissipative transport in one
direction while being resistive in the opposite direction.
Multiple examples of such devices have emerged in the past
couple of years; however, their efficiency is typically
limited, and most of them require a magnetic field to
function. Here we present a device that achieves
efficiencies approaching 100% while operating at zero field.
Our samples consist of a network of three graphene Josephson
junctions linked by a common superconducting island, to
which we refer as a Josephson triode. The three-terminal
nature of the device inherently breaks the inversion
symmetry, and the control current applied to one of the
contacts breaks the time-reversal symmetry. The triode's
utility is demonstrated by rectifying a small (nA scale
amplitude) applied square wave. We speculate that devices of
this type could be realistically employed in the modern
quantum circuits.},
Doi = {10.1021/acs.nanolett.3c01276},
Key = {fds371253}
}
@article{fds369660,
Author = {Arnault, EG and Al-Tawhid, AH and Salmani-Rezaie, S and Muller, DA and Kumah, DP and Bahramy, MS and Finkelstein, G and Ahadi,
K},
Title = {Anisotropic superconductivity at KTaO3(111)
interfaces.},
Journal = {Science advances},
Volume = {9},
Number = {7},
Pages = {eadf1414},
Year = {2023},
Month = {February},
url = {http://dx.doi.org/10.1126/sciadv.adf1414},
Abstract = {A two-dimensional, anisotropic superconductivity was
recently found at the KTaO<sub>3</sub>(111) interfaces. The
nature of the anisotropic superconducting transition remains
a subject of debate. To investigate the origins of the
observed behavior, we grew epitaxial KTaO<sub>3</sub>(111)-based
heterostructures. We show that the superconductivity is
robust against the in-plane magnetic field and violates the
Pauli limit. We also show that the Cooper pairs are more
resilient when the bias is along [11[Formula: see text]] (I
∥ [11[Formula: see text]]) and the magnetic field is along
[1[Formula: see text]0] (<i>B</i> ∥ [1[Formula: see
text]0]). We discuss the anisotropic nature of
superconductivity in the context of electronic structure,
orbital character, and spin texture at the
KTaO<sub>3</sub>(111) interfaces. The results point to
future opportunities to enhance superconducting transition
temperatures and critical fields in crystalline,
two-dimensional superconductors with strong spin-orbit
coupling.},
Doi = {10.1126/sciadv.adf1414},
Key = {fds369660}
}
@article{fds368118,
Author = {Zhao, L and Arnault, EG and Larson, TFQ and Iftikhar, Z and Seredinski,
A and Fleming, T and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein, G},
Title = {Graphene-Based Quantum Hall Interferometer with Self-Aligned
Side Gates.},
Journal = {Nano letters},
Volume = {22},
Number = {23},
Pages = {9645-9651},
Year = {2022},
Month = {December},
url = {http://dx.doi.org/10.1021/acs.nanolett.2c03805},
Abstract = {The vanishing band gap of graphene has long presented
challenges for making high-quality quantum point contacts
(QPCs)─the partially transparent p-n interfaces introduced
by conventional split gates tend to short circuit the QPCs.
This complication has hindered the fabrication of graphene
quantum Hall Fabry-Pérot interferometers, until recent
advances have allowed split-gate QPCs to operate utilizing
the highly resistive ν = 0 state. Here, we present a simple
recipe to fabricate QPCs by etching a narrow trench in the
graphene sheet to separate the conducting channel from
self-aligned graphene side gates. We demonstrate operation
of the individual QPCs in the quantum Hall regime and
further utilize these QPCs to create and study a quantum
Hall interferometer.},
Doi = {10.1021/acs.nanolett.2c03805},
Key = {fds368118}
}
@article{fds366140,
Author = {Arnault, EG and Idris, S and McConnell, A and Zhao, L and Larson, TFQ and Watanabe, K and Taniguchi, T and Finkelstein, G and Amet,
F},
Title = {Dynamical Stabilization of Multiplet Supercurrents in
Multiterminal Josephson Junctions.},
Journal = {Nano letters},
Volume = {22},
Number = {17},
Pages = {7073-7079},
Year = {2022},
Month = {September},
url = {http://dx.doi.org/10.1021/acs.nanolett.2c01999},
Abstract = {The dynamical properties of multiterminal Josephson
junctions (MT-JJs) have attracted interest, driven by the
promise of new insights into synthetic topological phases of
matter and Floquet states. This effort has culminated in the
discovery of Cooper multiplets in which the splitting of a
Cooper pair is enabled via a series of Andreev reflections
that entangle four (or more) electrons. Here, we show that
multiplet resonances can also emerge as a consequence of the
three-terminal circuit model. The supercurrent appears due
to correlated phase dynamics at values that correspond to
the multiplet condition <i>nV</i><sub>1</sub> =
-<i>mV</i><sub>2</sub> of applied bias. Multiplet resonances
are seen in nanofabricated three-terminal graphene JJs,
analog three-terminal JJ circuits, and circuit simulations.
The stabilization of the supercurrent is purely dynamical,
and a close analog to Kapitza's inverted pendulum problem.
We describe parameter considerations that optimize the
detection of the multiplet lines both for design of future
devices.},
Doi = {10.1021/acs.nanolett.2c01999},
Key = {fds366140}
}
@article{fds359996,
Author = {Arnault, EG and Larson, TFQ and Seredinski, A and Zhao, L and Idris, S and McConnell, A and Watanabe, K and Taniguchi, T and Borzenets, I and Amet,
F and Finkelstein, G},
Title = {Multiterminal Inverse AC Josephson Effect.},
Journal = {Nano letters},
Volume = {21},
Number = {22},
Pages = {9668-9674},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1021/acs.nanolett.1c03474},
Abstract = {When a Josephson junction is exposed to microwave radiation,
it undergoes the inverse AC Josephson effect─the phase of
the junction locks to the drive frequency. As a result, the
<i>I</i>-<i>V</i> curves of the junction acquire "Shapiro
steps" of quantized voltage. If the junction has three or
more superconducting contacts, coupling between different
pairs of terminals must be taken into account and the state
of the junction evolves in a phase space of higher
dimensionality. Here, we study the multiterminal inverse AC
Josephson effect in a graphene sample with three
superconducting terminals. We observe robust fractional
Shapiro steps and correlated switching events, which can
only be explained by considering the device as a completely
connected Josephson network. We successfully simulate the
observed behaviors using a modified two-dimensional RCSJ
model. Our results suggest that multiterminal Josephson
junctions are a playground to study highly connected
nonlinear networks with novel topologies.},
Doi = {10.1021/acs.nanolett.1c03474},
Key = {fds359996}
}
@article{fds355985,
Author = {Seredinski, A and Arnault, EG and Costa, VZ and Zhao, L and Larson, TFQ and Watanabe, K and Taniguchi, T and Amet, F and Newaz, AKM and Finkelstein,
G},
Title = {One-dimensional edge contact to encapsulated MoS2
with a superconductor},
Journal = {AIP Advances},
Volume = {11},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1063/5.0045009},
Abstract = {Establishing ohmic contact to van der Waals semiconductors
such as MoS2 is crucial to unlocking their full potential in
next-generation electronic devices. Encapsulation of few
layer MoS2 with hBN preserves the material’s electronic
properties but makes electrical contacts more challenging.
Progress toward high quality edge contact to encapsulated
MoS2 has been recently reported. Here, we evaluate a contact
methodology using sputtered MoRe, a type II superconductor
with a relatively high critical field and temperature
commonly used to induce superconductivity in graphene. We
find that the contact transparency is poor and that the
devices do not support a measurable supercurrent down to
3 K, which has ramifications for future fabrication
recipes.},
Doi = {10.1063/5.0045009},
Key = {fds355985}
}
@article{fds329747,
Author = {Zhang, G and Chung, C-H and Ke, C-T and Lin, C-Y and Mebrahtu, H and Smirnov, AI and Finkelstein, G and Baranger, HU},
Title = {Nonequilibrium quantum critical steady state: Transport
through a dissipative resonant level},
Journal = {Physical Review Research},
Volume = {3},
Number = {1},
Pages = {013136-013136},
Publisher = {American Physical Society (APS)},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevresearch.3.013136},
Abstract = {Nonequilibrium properties of correlated quantum matter are
being intensively investigated because of the rich interplay
between external driving and the many-body correlations. Of
particular interest is the nonequilibrium behavior near a
quantum critical point (QCP), where the system is delicately
balanced between different ground states. We present both an
analytical calculation of the nonequilibrium steady-state
current in a critical system and experimental results to
which the theory is compared. The system is a quantum dot
coupled to resistive leads: a spinless resonant level
interacting with an ohmic dissipative environment. A
two-channel Kondo-like QCP occurs when the level is on
resonance and symmetrically coupled to the leads, conditions
achieved by fine tuning using electrostatic gates. We
calculate and measure the nonlinear current as a function of
bias (I−V curve) at the critical values of the gate
voltages corresponding to the QCP. The quantitative
agreement between the experimental data and the theory, with
no fitting parameter, is excellent. As our system is fully
accessible to both theory and experiment, it provides an
ideal setting for addressing nonequilibrium phenomena in
correlated quantum matter.},
Doi = {10.1103/physrevresearch.3.013136},
Key = {fds329747}
}
@article{fds360649,
Author = {Zhang G and Chung C-H and Ke C-T and Lin C-Y and Mebrahtu H and Smirnov AI and Finkelstein G and Baranger HU},
Title = {Nonequilibrium quantum critical steady state: Transport
through a dissipative resonant level},
Journal = {Physical Review Research},
Volume = {3},
Number = {1},
Year = {2021},
url = {http://dx.doi.org/10.1103/physrevresearch.3.013136},
Doi = {10.1103/physrevresearch.3.013136},
Key = {fds360649}
}
@article{fds353325,
Author = {Larson, TFQ and Zhao, L and Arnault, EG and Wei, M-T and Seredinski, A and Li, H and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein,
G},
Title = {Zero Crossing Steps and Anomalous Shapiro Maps in Graphene
Josephson Junctions.},
Journal = {Nano letters},
Volume = {20},
Number = {10},
Pages = {6998-7003},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1021/acs.nanolett.0c01598},
Abstract = {The AC Josephson effect manifests itself in the form of
"Shapiro steps" of quantized voltage in Josephson junctions
subject to radiofrequency (RF) radiation. This effect
presents an early example of a driven-dissipative quantum
phenomenon and is presently utilized in primary voltage
standards. Shapiro steps have also become one of the
standard tools to probe junctions made in a variety of novel
materials. Here we study Shapiro steps in a widely tunable
graphene-based Josephson junction in which the
high-frequency dynamics is determined by the on-chip
environment. We investigate the variety of patterns that can
be obtained in this well-understood system depending on the
carrier density, temperature, RF frequency, and magnetic
field. Although the patterns of Shapiro steps can change
drastically when just one parameter is varied, the overall
trends can be understood and the behaviors straightforwardly
simulated, showing some key differences from the
conventional RCSJ model. The resulting understanding may
help interpret similar measurements in more complex
materials.},
Doi = {10.1021/acs.nanolett.0c01598},
Key = {fds353325}
}
@article{fds349693,
Author = {Zhao, L and Arnault, EG and Bondarev, A and Seredinski, A and Larson, T and Draelos, AW and Li, H and Watanabe, K and Taniguchi, T and Amet, F and Baranger, HU and Finkelstein, G},
Title = {Interference of Chiral Andreev Edge States},
Journal = {Nature Physics},
Volume = {16},
Number = {8},
Pages = {862-867},
Publisher = {Springer Nature},
Year = {2020},
Month = {May},
url = {https://arxiv.org/abs/1907.01722},
Abstract = {The search for topological excitations such as Majorana
fermions has spurred interest in the boundaries between
distinct quan- tum states. Here, we explore an interface
between two prototypical phases of electrons with
conceptually different ground states: the integer quantum
Hall insulator and the s-wave superconductor. We find clear
signatures of hybridized electron and hole states similar to
chiral Majorana fermions, which we refer to as chiral
Andreev edge states (CAESs). These propagate along the
interface in the direction determined by the magnetic field
and their interference can turn an incoming electron into an
out- going electron or hole, depending on the phase
accumulated by the CAESs along their path. Our results
demonstrate that these excitations can propagate and
interfere over a significant length, opening future
possibilities for their coherent manipulation.},
Doi = {10.1038/s41567-020-0898-5},
Key = {fds349693}
}
@article{fds359469,
Author = {Ke, CT and Draelos, AW and Seredinski, A and Wei, MT and Li, H and Hernandez-Rivera, M and Watanabe, K and Taniguchi, T and Yamamoto, M and Tarucha, S and Bomze, Y and Borzenets, IV and Amet, F and Finkelstein,
G},
Title = {Anomalous periodicity of magnetic interference patterns in
encapsulated graphene Josephson junctions},
Journal = {Physical Review Research},
Volume = {1},
Number = {3},
Pages = {033084},
Year = {2019},
Month = {November},
url = {https://doi.org/10.1103/PhysRevResearch.1.033084},
Abstract = {We investigate supercurrent interference patterns measured
as a function of magnetic field in ballistic graphene
Josephson junctions. At high doping, the expected
φ0-periodic "Fraunhofer"pattern is observed, indicating a
uniform current distribution. Close to the Dirac point, we
find anomalous interferences that are close to a 2φ0
periodicity, similar to that predicted for topological
Andreev bound states carrying a charge of e instead of 2e.
This feature persists with increasing temperature, ruling
out a nonsinusoidal current-phase relationship. It also
persists in junctions in which sharp vacuum edges are
eliminated. Our results indicate that the observed behavior
may originate from an intrinsic property of ballistic
graphene Josephson junctions, though the exact mechanism
remains unclear.},
Doi = {10.1103/PhysRevResearch.1.033084},
Key = {fds359469}
}
@article{fds346596,
Author = {Wei, MT and Draelos, AW and Seredinski, A and Ke, CT and Li, H and Mehta,
Y and Watanabe, K and Taniguchi, T and Yamamoto, M and Tarucha, S and Finkelstein, G and Amet, F and Borzenets, IV},
Title = {Chiral quasiparticle tunneling between quantum Hall edges in
proximity with a superconductor},
Journal = {Physical Review B},
Volume = {100},
Number = {12},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevB.100.121403},
Abstract = {We study a two-terminal graphene Josephson junction with
contacts shaped to form a narrow constriction, less than
100nm in length. The contacts are made from type-II
superconducting contacts and able to withstand magnetic
fields high enough to reach the quantum Hall regime in
graphene. In this regime, the device conductance is
determined by edge states, plus the contribution from the
constricted region. In particular, the constriction area can
support supercurrents up to fields of ∼2.5T. Additionally,
enhanced conductance is observed through a wide range of
magnetic fields and gate voltages. This additional
conductance and the appearance of supercurrent is attributed
to the tunneling between counterpropagating quantum Hall
edge states along opposite superconducting
contacts.},
Doi = {10.1103/PhysRevB.100.121403},
Key = {fds346596}
}
@article{fds347442,
Author = {Seredinski, A and Draelos, AW and Arnault, EG and Wei, M-T and Li, H and Fleming, T and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein,
G},
Title = {Quantum Hall-based superconducting interference
device.},
Journal = {Science advances},
Volume = {5},
Number = {9},
Pages = {eaaw8693},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1126/sciadv.aaw8693},
Abstract = {We present a study of a graphene-based Josephson junction
with dedicated side gates carved from the same sheet of
graphene as the junction itself. These side gates are highly
efficient and allow us to modulate carrier density along
either edge of the junction in a wide range. In particular,
in magnetic fields in the 1- to 2-T range, we are able to
populate the next Landau level, resulting in Hall plateaus
with conductance that differs from the bulk filling factor.
When counter-propagating quantum Hall edge states are
introduced along either edge, we observe a supercurrent
localized along that edge of the junction. Here, we study
these supercurrents as a function of magnetic field and
carrier density.},
Doi = {10.1126/sciadv.aaw8693},
Key = {fds347442}
}
@article{fds342477,
Author = {Draelos, AW and Silverman, A and Eniwaye, B and Arnault, EG and Ke, CT and Wei, MT and Vlassiouk, I and Borzenets, IV and Amet, F and Finkelstein,
G},
Title = {Subkelvin lateral thermal transport in diffusive
graphene},
Journal = {Physical Review B},
Volume = {99},
Number = {12},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevB.99.125427},
Abstract = {In this work, we report on hot carrier diffusion in graphene
across large enough length scales that the carriers are not
thermalized across the crystal. The carriers are injected
into graphene at one site and their thermal transport is
studied as a function of applied power and distance from the
heating source, up to tens of micrometers away.
Superconducting contacts prevent out-diffusion of hot
carriers to isolate the electron-phonon coupling as the sole
channel for thermal relaxation. As local thermometers, we
use the amplitude of the universal conductance fluctuations,
which varies monotonically as a function of temperature. By
measuring the electron temperature simultaneously along the
length we observe a thermal gradient which results from the
competition between electron-phonon cooling and lateral heat
flow.},
Doi = {10.1103/PhysRevB.99.125427},
Key = {fds342477}
}
@article{fds341505,
Author = {Draelos, AW and Wei, M-T and Seredinski, A and Li, H and Mehta, Y and Watanabe, K and Taniguchi, T and Borzenets, IV and Amet, F and Finkelstein, G},
Title = {Supercurrent Flow in Multiterminal Graphene Josephson
Junctions.},
Journal = {Nano letters},
Volume = {19},
Number = {2},
Pages = {1039-1043},
Year = {2019},
Month = {February},
url = {http://dx.doi.org/10.1021/acs.nanolett.8b04330},
Abstract = {We investigate the electronic properties of ballistic planar
Josephson junctions with multiple superconducting terminals.
Our devices consist of monolayer graphene encapsulated in
boron nitride with molybdenum-rhenium contacts. Resistance
measurements yield multiple resonant features, which are
attributed to supercurrent flow among adjacent and
nonadjacent Josephson junctions. In particular, we find that
superconducting and dissipative currents coexist within the
same region of graphene. We show that the presence of
dissipative currents primarily results in electron heating
and estimate the associated temperature rise. We find that
the electrons in encapsulated graphene are efficiently
cooled through the electron-phonon coupling.},
Doi = {10.1021/acs.nanolett.8b04330},
Key = {fds341505}
}
@article{fds340250,
Author = {Seredinski, A and Draelos, A and Wei, MT and Ke, CT and Fleming, T and Mehta, Y and Mancil, E and Li, H and Taniguchi, T and Watanabe, K and Tarucha, S and Yamamoto, M and Borzenets, IV and Amet, F and Finkelstein, G},
Title = {Supercurrent in Graphene Josephson Junctions with Narrow
Trenches in the Quantum Hall Regime},
Journal = {MRS Advances},
Volume = {3},
Number = {47-48},
Pages = {2855-2864},
Publisher = {Cambridge University Press (CUP)},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1557/adv.2018.469},
Abstract = {Coupling superconductors to quantum Hall edge states is the
subject of intense investigation as part of the ongoing
search for non-abelian excitations. Our group has previously
observed supercurrents of hundreds of picoamperes in
graphene Josephson junctions in the quantum Hall regime. One
of the explanations of this phenomenon involves the coupling
of an electron edge state on one side of the junction to a
hole edge state on the opposite side. In our previous
samples, these states are separated by several microns.
Here, a narrow trench perpendicular to the contacts creates
counterpropagating quantum Hall edge channels tens of
nanometres from each other. Transport measurements
demonstrate a change in the low-field Fraunhofer
interference pattern for trench devices and show a
supercurrent in both trench and reference junctions in the
quantum Hall regime. The trench junctions show no
enhancement of quantum Hall supercurrent and an unexpected
supercurrent periodicity with applied field, suggesting the
need for further optimization of device parameters.},
Doi = {10.1557/adv.2018.469},
Key = {fds340250}
}
@article{fds329564,
Author = {Finkelstein, G and Amet, F},
Title = {Superconductivity: When Andreev meets Hall},
Journal = {Nature Physics},
Volume = {13},
Number = {7},
Pages = {625-626},
Publisher = {Springer Nature},
Year = {2017},
Month = {July},
url = {http://dx.doi.org/10.1038/nphys4195},
Doi = {10.1038/nphys4195},
Key = {fds329564}
}
@article{fds329748,
Author = {Draelos, A and Wei, MT and Seredinski, A and Ke, C and Watanabe, K and Taniguchi, T and Yamamoto, M and Tarucha, S and Borzenets, I and Amet,
F and Finkelstein, G},
Title = {Investigation of Supercurrent in the Quantum Hall Regime in
Graphene Josephson Junctions},
Journal = {Submitted to the Journal of Low Temperature
Physics},
Volume = {191},
Number = {5-6},
Pages = {288-300},
Year = {2017},
url = {http://dx.doi.org/10.1007/s10909-018-1872-9},
Abstract = {In this study, we examine multiple encapsulated graphene
Josephson junctions to determine which mechanisms may be
responsible for the supercurrent observed in the quantum
Hall (QH) regime. Rectangular junctions with various widths
and lengths were studied to identify which parameters affect
the occurrence of QH supercurrent. We also studied
additional samples where the graphene region is extended
beyond the contacts on one side, making that edge of the
mesa significantly longer than the opposite edge. This is
done in order to distinguish two potential mechanisms: (a)
supercurrents independently flowing along both non-contacted
edges of graphene mesa, and (b) opposite sides of the mesa
being coupled by hybrid electron–hole modes flowing along
the superconductor/graphene boundary. The supercurrent
appears suppressed in extended junctions, suggesting the
latter mechanism.},
Doi = {10.1007/s10909-018-1872-9},
Key = {fds329748}
}
@article{fds322476,
Author = {Borzenets, IV and Amet, F and Ke, CT and Draelos, AW and Wei, MT and Seredinski, A and Watanabe, K and Taniguchi, T and Bomze, Y and Yamamoto, M and Tarucha, S and Finkelstein, G},
Title = {Ballistic Graphene Josephson Junctions from the Short to the
Long Junction Regimes.},
Journal = {Physical review letters},
Volume = {117},
Number = {23},
Pages = {237002},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.117.237002},
Abstract = {We investigate the critical current I_{C} of ballistic
Josephson junctions made of encapsulated
graphene-boron-nitride heterostructures. We observe a
crossover from the short to the long junction regimes as the
length of the device increases. In long ballistic junctions,
I_{C} is found to scale as ∝exp(-k_{B}T/δE). The
extracted energies δE are independent of the carrier
density and proportional to the level spacing of the
ballistic cavity. As T→0 the critical current of a long
(or short) junction saturates at a level determined by the
product of δE (or Δ) and the number of the junction's
transversal modes.},
Doi = {10.1103/physrevlett.117.237002},
Key = {fds322476}
}
@article{fds322477,
Author = {Ke, CT and Borzenets, IV and Draelos, AW and Amet, F and Bomze, Y and Jones, G and Craciun, M and Russo, S and Yamamoto, M and Tarucha, S and Finkelstein, G},
Title = {Critical Current Scaling in Long Diffusive Graphene-Based
Josephson Junctions.},
Journal = {Nano letters},
Volume = {16},
Number = {8},
Pages = {4788-4791},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1021/acs.nanolett.6b00738},
Abstract = {We present transport measurements on long, diffusive,
graphene-based Josephson junctions. Several junctions are
made on a single-domain crystal of CVD graphene and feature
the same contact width of ∼9 μm but vary in length from
400 to 1000 nm. As the carrier density is tuned with the
gate voltage, the critical current in these junctions ranges
from a few nanoamperes up to more than 5 μA, while the
Thouless energy, ETh, covers almost 2 orders of magnitude.
Over much of this range, the product of the critical current
and the normal resistance ICRN is found to scale linearly
with ETh, as expected from theory. However, the value of the
ratio ICRN/ETh is found to be 0.1-0.2, which much smaller
than the predicted ∼10 for long diffusive SNS
junctions.},
Doi = {10.1021/acs.nanolett.6b00738},
Key = {fds322477}
}
@article{fds322478,
Author = {Amet, F and Ke, CT and Borzenets, IV and Wang, J and Watanabe, K and Taniguchi, T and Deacon, RS and Yamamoto, M and Bomze, Y and Tarucha, S and Finkelstein, G},
Title = {Supercurrent in the quantum Hall regime.},
Journal = {Science (New York, N.Y.)},
Volume = {352},
Number = {6288},
Pages = {966-969},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1126/science.aad6203},
Abstract = {A promising route for creating topological states and
excitations is to combine superconductivity and the quantum
Hall (QH) effect. Despite this potential, signatures of
superconductivity in the QH regime remain scarce, and a
superconducting current through a QH weak link has been
challenging to observe. We demonstrate the existence of a
distinct supercurrent mechanism in encapsulated graphene
samples contacted by superconducting electrodes, in magnetic
fields as high as 2 tesla. The observation of a supercurrent
in the QH regime marks an important step in the quest for
exotic topological excitations, such as Majorana fermions
and parafermions, which may find applications in
fault-tolerant quantum computing.},
Doi = {10.1126/science.aad6203},
Key = {fds322478}
}
@article{fds322479,
Author = {Zhang, X and Gutierrez, Y and Li, P and Barreda, AI and Watson, AM and Alcaraz De La Osa and R and Finkelstein, G and Gonzalez, F and Ortiz, D and Saiz, JM and Sanz, JM and Everitt, HO and Liu, J and Moreno,
F},
Title = {Plasmonics in the UV range with Rhodium nanocubes},
Journal = {Proceedings of SPIE - The International Society for Optical
Engineering},
Volume = {9884},
Publisher = {SPIE},
Year = {2016},
Month = {January},
ISBN = {9781510601291},
url = {http://dx.doi.org/10.1117/12.2227674},
Abstract = {Plasmonics in the UV-range constitutes a new challenge due
to the increasing demand to detect, identify and destroy
biological toxins, enhance biological imaging, and
characterize semiconductor devices at the nanometer scale.
Silver and aluminum have an effcient plasmonic performance
in the near UV region, but oxidation reduces its performance
in this range. Recent studies point out rhodium as one of
the most promising metals for this purpose: it has a good
plasmonic response in the UV and, as gold in the visible, it
presents a low tendency to oxidation. Moreover, its easy
fabrication through chemical means and its potential for
photocatalytic applications, makes this material very
attractive for building plasmonic tools in the UV. In this
work, we will show an overview of our recent collaborative
research with rhodium nanocubes (NC) for Plasmonics in the
UV.},
Doi = {10.1117/12.2227674},
Key = {fds322479}
}
@article{fds329565,
Author = {Amet, F and Finkelstein, G},
Title = {Valleytronics: Could use a break},
Journal = {Nature Physics},
Volume = {11},
Number = {12},
Pages = {989-990},
Publisher = {Springer Nature},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1038/nphys3587},
Doi = {10.1038/nphys3587},
Key = {fds329565}
}
@article{fds245936,
Author = {Watson, AM and Zhang, X and Alcaraz de la Osa and R and Marcos Sanz and J and González, F and Moreno, F and Finkelstein, G and Liu, J and Everitt,
HO},
Title = {Rhodium nanoparticles for ultraviolet plasmonics.},
Journal = {Nano letters},
Volume = {15},
Number = {2},
Pages = {1095-1100},
Year = {2015},
Month = {February},
ISSN = {1530-6984},
url = {http://dx.doi.org/10.1021/nl5040623},
Abstract = {The nonoxidizing catalytic noble metal rhodium is introduced
for ultraviolet plasmonics. Planar tripods of 8 nm Rh
nanoparticles, synthesized by a modified polyol reduction
method, have a calculated local surface plasmon resonance
near 330 nm. By attaching p-aminothiophenol, local
field-enhanced Raman spectra and accelerated photodamage
were observed under near-resonant ultraviolet illumination,
while charge transfer simultaneously increased fluorescence
for up to 13 min. The combined local field enhancement and
charge transfer demonstrate essential steps toward
plasmonically enhanced ultraviolet photocatalysis.},
Doi = {10.1021/nl5040623},
Key = {fds245936}
}
@article{fds245937,
Author = {Li, J and Ke, C-T and Liu, K and Li, P and Liang, S and Finkelstein, G and Wang, F and Liu, J},
Title = {Importance of diameter control on selective synthesis of
semiconducting single-walled carbon nanotubes.},
Journal = {ACS nano},
Volume = {8},
Number = {8},
Pages = {8564-8572},
Year = {2014},
Month = {August},
ISSN = {1936-0851},
url = {http://dx.doi.org/10.1021/nn503265g},
Abstract = {The coexistence of semiconducting and metallic single-walled
carbon nanotubes (SWNTs) during synthesis is one of the
major bottlenecks that prevent their broad application for
the next-generation nanoelectronics. Herein, we present more
understanding and demonstration of the growth of highly
enriched semiconducting SWNTs (s-SWNTs) with a narrow
diameter distribution. An important fact discovered in our
experiments is that the selective elimination of metallic
SWNTs (m-SWNTs) from the mixed arrays grown on quartz is
diameter-dependent. Our method emphasizes controlling the
diameter distribution of SWNTs in a narrow range where
m-SWNTs can be effectively and selectively etched during
growth. In order to achieve narrow diameter distribution,
uniform and stable Fe-W nanoclusters were used as the
catalyst precursors. About 90% of as-prepared SWNTs fall
into the diameter range 2.0-3.2 nm. Electrical measurement
results on individual SWNTs confirm that the selectivity of
s-SWNTs is ∼95%. The present study provides an effective
strategy for increasing the purity of s-SWNTs via
controlling the diameter distribution of SWNTs and adjusting
the etchant concentration. Furthermore, by carefully
comparing the chirality distributions of Fe-W-catalyzed and
Fe-catalyzed SWNTs under different water vapor
concentrations, the relationship between the
diameter-dependent and electronic-type-dependent etching
mechanisms was investigated.},
Doi = {10.1021/nn503265g},
Key = {fds245937}
}
@article{fds245939,
Author = {Liu, DE and Zheng, H and Finkelstein, G and Baranger,
HU},
Title = {Tunable quantum phase transitions in a resonant level
coupled to two dissipative baths},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {89},
Number = {8},
Pages = {085116},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {February},
ISSN = {1098-0121},
url = {http://dx.doi.org/10.1103/PhysRevB.89.085116},
Abstract = {We study tunneling through a resonant level connected to two
dissipative bosonic baths: one is the resistive environment
of the source and drain leads, while the second comes from
coupling to potential fluctuations on a resistive gate. We
show that several quantum phase transitions (QPT) occur in
such a model, transitions which emulate those found in
interacting systems such as Luttinger liquids or Kondo
systems. We first use bosonization to map this dissipative
resonant level model to a resonant level in a Luttinger
liquid, one with, curiously, two interaction parameters.
Drawing on methods for analyzing Luttinger liquids at both
weak and strong coupling, we obtain the phase diagram. For
strong dissipation, a Berezinsky-Kosterlitz-Thouless QPT
separates strong-coupling and weak-coupling (charge
localized) phases. In the source-drain symmetric case, all
relevant backscattering processes disappear at strong
coupling, leading to perfect transmission at zero
temperature. In fact, a QPT occurs as a function of the
coupling asymmetry or energy of the resonant level: the two
phases are (i) the system is cut into two disconnected
pieces (zero transmission), or (ii) the system is a single
connected piece with perfect transmission, except for a
disconnected fractional degree of freedom. The latter arises
from the competition between the two fermionic leads (source
and drain), as in the two-channel Kondo effect. © 2014
American Physical Society.},
Doi = {10.1103/PhysRevB.89.085116},
Key = {fds245939}
}
@article{fds245938,
Author = {Pilo-Pais, M and Watson, A and Demers, S and LaBean, TH and Finkelstein,
G},
Title = {Surface-enhanced Raman scattering plasmonic enhancement
using DNA origami-based complex metallic
nanostructures.},
Journal = {Nano letters},
Volume = {14},
Number = {4},
Pages = {2099-2104},
Year = {2014},
Month = {January},
ISSN = {1530-6984},
url = {http://dx.doi.org/10.1021/nl5003069},
Abstract = {DNA origami is a novel self-assembly technique allowing one
to form various two-dimensional shapes and position matter
with nanometer accuracy. We use DNA origami templates to
engineer surface-enhanced Raman scattering substrates.
Specifically, gold nanoparticles were selectively placed on
the corners of rectangular origami and subsequently enlarged
via solution-based metal deposition. The resulting
assemblies exhibit "hot spots" of enhanced electromagnetic
field between the nanoparticles. We observed a significant
Raman signal enhancement from molecules covalently attached
to the assemblies, as compared to control nanoparticle
samples that lack interparticle hot spots. Furthermore,
Raman molecules are used to map out the hot spots'
distribution, as they are burned when experiencing a
threshold electric field. Our method opens up the prospects
of using DNA origami to rationally engineer and assemble
plasmonic structures for molecular spectroscopy.},
Doi = {10.1021/nl5003069},
Key = {fds245938}
}
@article{fds245942,
Author = {Borzenets, IV and Coskun, UC and Mebrahtu, HT and Bomze, YV and Smirnov,
AI and Finkelstein, G},
Title = {Phonon bottleneck in graphene-based Josephson junctions at
millikelvin temperatures.},
Journal = {Physical review letters},
Volume = {111},
Number = {2},
Pages = {027001},
Year = {2013},
Month = {July},
url = {http://www.ncbi.nlm.nih.gov/pubmed/23889431},
Abstract = {We examine the nature of the transitions between the normal
and superconducting branches in superconductor-graphene-superconductor
Josephson junctions. We attribute the hysteresis between the
switching (superconducting to normal) and retrapping (normal
to superconducting) transitions to electron overheating. In
particular, we demonstrate that the retrapping current
corresponds to the critical current at an elevated
temperature, where the heating is caused by the retrapping
current itself. The superconducting gap in the leads
suppresses the hot electron outflow, allowing us to further
study electron thermalization by phonons at low temperatures
(T≲1 K). The relationship between the applied power and
the electron temperature was found to be P∝T3, which we
argue is consistent with cooling due to electron-phonon
interactions.},
Doi = {10.1103/physrevlett.111.027001},
Key = {fds245942}
}
@article{fds245941,
Author = {Chung, CH and Le Hur and K and Finkelstein, G and Vojta, M and Wölfle,
P},
Title = {Nonequilibrium quantum transport through a dissipative
resonant level},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {87},
Number = {24},
Pages = {245310},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {June},
ISSN = {1098-0121},
url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000320767700003&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
Abstract = {The resonant-level model represents a paradigmatic quantum
system which serves as a basis for many other quantum
impurity models. We provide a comprehensive analysis of the
nonequilibrium transport near a quantum phase transition in
a spinless dissipative resonant-level model, extending
earlier work. A detailed derivation of a rigorous mapping of
our system onto an effective Kondo model is presented. A
controlled energy-dependent renormalization-group approach
is applied to compute the nonequilibrium current in the
presence of a finite bias voltage V. In the linear-response
regime V→0, the system exhibits as a function of the
dissipative strength a localized-delocalized quantum
transition of the Kosterlitz-Thouless (KT) type. We address
fundamental issues of the nonequilibrium transport near the
quantum phase transition: Does the bias voltage play the
same role as temperature to smear out the transition? What
is the scaling of the nonequilibrium conductance near the
transition? At finite temperatures, we show that the
conductance follows the equilibrium scaling for V<T, while
it obeys a distinct nonequilibrium profile for V>T. We
furthermore provide different signatures of the transition
in the finite-frequency current noise and ac conductance via
a recently developed functional renormalization group (FRG)
approach. The generalization of our analysis to
nonequilibrium transport through a resonant level coupled to
two chiral Luttinger liquid leads, generated by fractional
quantum Hall edge states, is discussed. Our work on the
dissipative resonant level has direct relevance to
experiments on a quantum dot coupled to a resistive
environment, such as H. Mebrahtu,. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevB.87.245310},
Key = {fds245941}
}
@article{fds245940,
Author = {Mebrahtu, HT and Borzenets, IV and Zheng, H and Bomze, YV and Smirnov,
AI and Florens, S and Baranger, HU and Finkelstein,
G},
Title = {Observation of majorana quantum critical behaviour in a
resonant level coupled to a dissipative environment},
Journal = {Nature Physics},
Volume = {9},
Number = {11},
Pages = {732-737},
Year = {2013},
Month = {January},
ISSN = {1745-2473},
url = {http://dx.doi.org/10.1038/nphys2735},
Abstract = {A quantum phase transition is an abrupt change between two
distinct ground states of a many-body system, driven by an
external parameter. In the vicinity of the quantum critical
point (QCP) where the transition occurs, a new phase may
emerge that is determined by quantum fluctuations and is
very different from either phase. In particular, a
conducting system may exhibit non-Fermi-liquid behaviour.
Although this scenario is well established theoretically,
controllable experimental realizations are rare. Here, we
experimentally investigate the nature of the QCP in a simple
nanoscale system - a spin-polarized resonant level coupled
to dissipative contacts. We fine-tune the system to the QCP,
realized exactly on-resonance and when the coupling between
the level and the two contacts is symmetric. Several
anomalous transport scaling laws are demonstrated, including
a striking non-Fermi-liquid scattering rate at the QCP,
indicating fractionalization of the resonant level into two
Majorana quasiparticles. © 2013 Macmillan Publishers
Limited.},
Doi = {10.1038/nphys2735},
Key = {fds245940}
}
@article{fds245958,
Author = {Yoon, I and Hamaguchi, K and Borzenets, IV and Finkelstein, G and Mooney, R and Donald, BR},
Title = {Intracellular Neural Recording with Pure Carbon Nanotube
Probes.},
Journal = {PLoS One},
Volume = {8},
Number = {6},
Pages = {e65715},
Year = {2013},
url = {http://dx.doi.org/10.1371/journal.pone.0065715},
Abstract = {The computational complexity of the brain depends in part on
a neuron's capacity to integrate electrochemical information
from vast numbers of synaptic inputs. The measurements of
synaptic activity that are crucial for mechanistic
understanding of brain function are also challenging,
because they require intracellular recording methods to
detect and resolve millivolt- scale synaptic potentials.
Although glass electrodes are widely used for intracellular
recordings, novel electrodes with superior mechanical and
electrical properties are desirable, because they could
extend intracellular recording methods to challenging
environments, including long term recordings in freely
behaving animals. Carbon nanotubes (CNTs) can theoretically
deliver this advance, but the difficulty of assembling CNTs
has limited their application to a coating layer or assembly
on a planar substrate, resulting in electrodes that are more
suitable for in vivo extracellular recording or
extracellular recording from isolated cells. Here we show
that a novel, yet remarkably simple, millimeter-long
electrode with a sub-micron tip, fabricated from
self-entangled pure CNTs can be used to obtain intracellular
and extracellular recordings from vertebrate neurons in
vitro and in vivo. This fabrication technology provides a
new method for assembling intracellular electrodes from
CNTs, affording a promising opportunity to harness
nanotechnology for neuroscience applications.},
Doi = {10.1371/journal.pone.0065715},
Key = {fds245958}
}
@article{fds303661,
Author = {Mebrahtu, HT and Borzenets, IV and Zheng, H and Bomze, YV and Smirnov,
AI and Florens, S and Baranger, HU and Finkelstein,
G},
Title = {Observation of Majorana quantum critical behaviour in a
resonant level coupled to a dissipative environment},
Journal = {Nature Physics},
Volume = {9},
Number = {11},
Pages = {732-737},
Publisher = {Springer Science and Business Media LLC},
Year = {2013},
url = {http://arxiv.org/abs/1212.3857v1},
Abstract = {We investigate experimentally an exotic state of electronic
matter obtained by fine-tuning to a quantum critical point
(QCP), realized in a spin-polarized resonant level coupled
to strongly dissipative electrodes. Several transport
scaling laws near and far from equilibrium are measured, and
then accounted for theoretically. Our analysis reveals a
splitting of the resonant level into two quasi-independent
Majorana modes, one strongly hybridized to the leads, and
the other tightly bound to the quantum dot. Residual
interactions involving these Majorana fermions result in the
observation of a striking quasi-linear non-Fermi liquid
scattering rate at the QCP. Our devices constitute a viable
alternative to topological superconductors as a platform for
studying strong correlation effects within Majorana
physics.},
Doi = {10.1038/nphys2735},
Key = {fds303661}
}
@article{fds245961,
Author = {Mebrahtu, HT and Borzenets, IV and Liu, DE and Zheng, H and Bomze, YV and Smirnov, AI and Baranger, HU and Finkelstein, G},
Title = {Quantum phase transition in a resonant level coupled to
interacting leads.},
Journal = {Nature},
Volume = {488},
Number = {7409},
Pages = {61-64},
Year = {2012},
Month = {August},
url = {http://www.ncbi.nlm.nih.gov/pubmed/22859201},
Abstract = {A Luttinger liquid is an interacting one-dimensional
electronic system, quite distinct from the 'conventional'
Fermi liquids formed by interacting electrons in two and
three dimensions. Some of the most striking properties of
Luttinger liquids are revealed in the process of electron
tunnelling. For example, as a function of the applied bias
voltage or temperature, the tunnelling current exhibits a
non-trivial power-law suppression. (There is no such
suppression in a conventional Fermi liquid.) Here, using a
carbon nanotube connected to resistive leads, we create a
system that emulates tunnelling in a Luttinger liquid, by
controlling the interaction of the tunnelling electron with
its environment. We further replace a single tunnelling
barrier with a double-barrier, resonant-level structure and
investigate resonant tunnelling between Luttinger liquids.
At low temperatures, we observe perfect transparency of the
resonant level embedded in the interacting environment, and
the width of the resonance tends to zero. We argue that this
behaviour results from many-body physics of interacting
electrons, and signals the presence of a quantum phase
transition. Given that many parameters, including the
interaction strength, can be precisely controlled in our
samples, this is an attractive model system for studying
quantum critical phenomena in general, with wide-reaching
implications for understanding quantum phase transitions in
more complex systems, such as cold atoms and strongly
correlated bulk materials.},
Doi = {10.1038/nature11265},
Key = {fds245961}
}
@article{fds245956,
Author = {Borzenets, IV and Yoon, I and Prior, MW and Donald, BR and Mooney, RD and Finkelstein, G},
Title = {Erratum: Ultra-sharp metal and nanotube-based probes for
applications in scanning microscopy and neural recording
(Journal of Applied Physics (2012) 111 (074703))},
Journal = {Journal of Applied Physics},
Volume = {112},
Number = {2},
Pages = {029906-029906},
Publisher = {AIP Publishing},
Year = {2012},
Month = {July},
ISSN = {0021-8979},
url = {http://dx.doi.org/10.1063/1.4739526},
Doi = {10.1063/1.4739526},
Key = {fds245956}
}
@article{fds245960,
Author = {Borzenets, IV and Coskun, UC and Mebrahtu, H and Finkelstein,
G},
Title = {Pb-Graphene-Pb josephson junctions: Characterization in
magnetic field},
Journal = {IEEE Transactions on Applied Superconductivity},
Volume = {22},
Number = {5},
Pages = {1800104-1800104},
Publisher = {Institute of Electrical and Electronics Engineers
(IEEE)},
Year = {2012},
Month = {June},
ISSN = {1051-8223},
url = {http://dx.doi.org/10.1109/TASC.2012.2198472},
Abstract = {We fabricate superconductor-graphene-superconductor
Josephson junctions with superconducting regions made of
lead (Pb). The critical current through graphene may be
modulated by the external magnetic field; the resulting
Fraunhofer interference pattern shows several periods of
oscillations, suggesting that the junction is uniform.
Deviations from the perfect Fraunhofer pattern are observed,
and their cause is explained by a simulation that takes into
account the sample design. © 2002-2011 IEEE.},
Doi = {10.1109/TASC.2012.2198472},
Key = {fds245960}
}
@article{fds347587,
Author = {Borzenets, IV and Yoon, I and Prior, MM and Donald, BR and Mooney, RD and Finkelstein, G},
Title = {Ultra-sharp metal and nanotube-based probes for applications
in scanning microscopy and neural recording.},
Journal = {J Appl Phys},
Volume = {111},
Number = {7},
Pages = {74703-747036},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1063/1.3702802},
Abstract = {This paper discusses several methods for manufacturing
ultra-sharp probes, with applications geared toward, but not
limited to, scanning microscopy (STM, AFM) and
intra-cellular recordings of neural signals. We present
recipes for making tungsten, platinum/iridium alloy, and
nanotube fibril tips. Electrical isolation methods using
Parylene-C or PMMA are described.},
Doi = {10.1063/1.3702802},
Key = {fds347587}
}
@article{fds245945,
Author = {Mebrahtu, H and Borzenets, I and Bomze, Y and Finkelstein,
G},
Title = {Observation of unitary conductance for resonant tunneling
with dissipation},
Journal = {Journal of Physics: Conference Series},
Volume = {400},
Number = {PART 4},
Pages = {042007-042007},
Publisher = {IOP Publishing},
Year = {2012},
Month = {January},
ISSN = {1742-6588},
url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000314977100367&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
Abstract = {We investigate tunneling through a resonant level formed in
a carbon nanotube quantum dot contacted by resistive metal
wires. These contacts create a dissipative environment for
the electrons tunneling across the nanotube, thus
suppressing the tunneling rate. We study the shape of the
resonant peak in the nanotube conductance, with the
expectation that the peak width and height, both dependent
on the tunneling rate, will be suppressed. Instead, we find
that the behavior crucially depends on the ratio of the
tunneling rates from the resonant level to the two contacts.
We discuss the implication of our findings for a boundary
quantum phase transition in this system. © Published under
licence by IOP Publishing Ltd.},
Doi = {10.1088/1742-6596/400/4/042007},
Key = {fds245945}
}
@article{fds245962,
Author = {Li, P and Wu, PM and Bomze, Y and Borzenets, IV and Finkelstein, G and Chang, AM},
Title = {Retrapping current, self-heating, and hysteretic
current-voltage characteristics in ultranarrow
superconducting aluminum nanowires},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {84},
Number = {18},
Pages = {184508},
Publisher = {American Physical Society (APS)},
Year = {2011},
Month = {November},
ISSN = {1098-0121},
url = {http://prb.aps.org/abstract/PRB/v84/i18/e184508},
Abstract = {Hysteretic I-V (current-voltage) curves are studied in
narrow Al nanowires. The nanowires have a cross section as
small as 50 nm2. We focus on the retrapping current in a
down-sweep of the current, at which a nanowire re-enters the
superconducting state from a normal state. The retrapping
current is found to be significantly smaller than the
switching current at which the nanowire switches into the
normal state from a superconducting state during a current
up-sweep. For wires of different lengths, we analyze the
heat removal due to various processes, including electron
and phonon processes. For a short wire 1.5μm in length,
electronic thermal conduction is effective; for longer wires
10μm in length, phonon conduction becomes important. We
demonstrate that the measured retrapping current as a
function of temperature can be quantitatively accounted for
by the self-heating occurring in the normal portions of the
nanowires to better than 20% accuracy. For the phonon
processes, the extracted thermal conduction parameters
support the notion of a reduced phase-space below three
dimensions, consistent with the phonon thermal wavelength
having exceeded the lateral dimensions at temperatures below
∼1.3 K. Nevertheless, surprisingly the best fit was
achieved with a functional form corresponding to
three-dimensional phonons, albeit requiring parameters far
exceeding known values in the literature. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevB.84.184508},
Key = {fds245962}
}
@article{fds245963,
Author = {Borzenets, IV and Coskun, UC and Jones, SJ and Finkelstein,
G},
Title = {Phase diffusion in graphene-based Josephson
junctions.},
Journal = {Physical review letters},
Volume = {107},
Number = {13},
Pages = {137005},
Year = {2011},
Month = {September},
url = {http://www.ncbi.nlm.nih.gov/pubmed/22026894},
Abstract = {We report on graphene-based Josephson junctions with
contacts made from lead. The high transition temperature of
this superconductor allows us to observe the supercurrent
branch at temperatures up to ∼2 K, at which point we can
detect a small, but nonzero, resistance. We attribute this
resistance to the phase diffusion mechanism, which has not
been yet identified in graphene. By measuring the resistance
as a function of temperature and gate voltage, we can
further characterize the nature of the electromagnetic
environment and dissipation in our samples.},
Doi = {10.1103/physrevlett.107.137005},
Key = {fds245963}
}
@article{fds304540,
Author = {Li, P and Wu, PM and Bomze, Y and Borzenets, IV and Finkelstein, G and Chang, AM},
Title = {Switching currents limited by single phase slips in
one-dimensional superconducting Al nanowires.},
Journal = {Physical review letters},
Volume = {107},
Number = {13},
Pages = {137004},
Year = {2011},
Month = {September},
url = {http://www.ncbi.nlm.nih.gov/pubmed/22026893},
Abstract = {An aluminum nanowire switches from superconducting to normal
as the current is increased in an upsweep. The switching
current (I(s)) averaged over upsweeps approximately follows
the depairing critical current (I(c)) but falls below it.
Fluctuations in I(s) exhibit three distinct regions of
behaviors and are nonmonotonic in temperature: saturation
well below the critical temperature T(c), an increase as
T(2/3) at intermediate temperatures, and a rapid decrease
close to T(c). Heat dissipation analysis indicates that a
single phase slip is able to trigger switching at low and
intermediate temperatures, whereby the T(2/3) dependence
arises from the thermal activation of a phase slip, while
saturation at low temperatures provides striking evidence
that the phase slips by macroscopic quantum
tunneling.},
Doi = {10.1103/physrevlett.107.137004},
Key = {fds304540}
}
@article{fds245966,
Author = {Pilo-Pais, M and Goldberg, S and Samano, E and Labean, TH and Finkelstein, G},
Title = {Connecting the nanodots: programmable nanofabrication of
fused metal shapes on DNA templates.},
Journal = {Nano letters},
Volume = {11},
Number = {8},
Pages = {3489-3492},
Year = {2011},
Month = {August},
url = {http://www.ncbi.nlm.nih.gov/pubmed/21732612},
Abstract = {We present a novel method for producing complex metallic
nanostructures of programmable design. DNA origami
templates, modified to have DNA binding sites with a
uniquely coded sequence, were adsorbed onto silicon dioxide
substrates. Gold nanoparticles functionalized with the cDNA
sequence were then attached. These seed nanoparticles were
later enlarged, and even fused, by electroless deposition of
silver. Using this method, we constructed a variety of
metallic structures, including rings, pairs of bars, and H
shapes.},
Doi = {10.1021/nl202066c},
Key = {fds245966}
}
@article{fds245965,
Author = {Samano, EC and Pilo-Pais, M and Goldberg, S and Vogen, BN and Finkelstein, G and LaBean, TH},
Title = {Self-Assembling DNA Templates for Programmed Artificial
Biomineralization},
Journal = {Soft Matter},
Volume = {7},
Number = {7},
Pages = {3240-3245},
Publisher = {Royal Society of Chemistry (RSC)},
Year = {2011},
Month = {January},
ISSN = {1744-683X},
url = {http://pubs.rsc.org/en/Content/ArticleLanding/2011/SM/c0sm01318h},
Abstract = {Complex materials with micron-scale dimensions and
nanometre-scale feature resolution created via engineered
DNA self-assembly represent an important new class of soft
matter. These assemblies are increasingly being exploited as
templates for the programmed assembly of functional
inorganic materials that have not conventionally lent
themselves to organization by molecular recognition
processes. The current challenge is to apply these
bioinspired DNA templates toward the fabrication of
composite materials for use in electronics, photonics, and
other fields of technology. This highlight focuses on
methods we consider most useful for integration of DNA
templated structures into functional composite
nanomaterials, particularly, organization of preformed
nanoparticles and metallization procedures. © The Royal
Society of Chemistry 2011.},
Doi = {10.1039/C0SM01318H},
Key = {fds245965}
}
@article{fds245968,
Author = {Bomze, Y and Borzenets, I and Mebrahtu, H and Makarovski, A and Baranger, HU and Finkelstein, G},
Title = {Two-stage Kondo effect and Kondo-box level spectroscopy in a
carbon nanotube},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {82},
Number = {16},
Pages = {161411R},
Publisher = {American Physical Society (APS)},
Year = {2010},
Month = {October},
ISSN = {1098-0121},
url = {http://hdl.handle.net/10161/4257 Duke open
access},
Abstract = {The concept of the "Kondo box" describes a single spin,
antiferromagnetically coupled to a quantum dot with a finite
level spacing. Here, a Kondo box is formed in a carbon
nanotube interacting with a localized electron. We
investigate the spins of its first few eigenstates and
compare them to a recent theory. In an "open" Kondo-box,
strongly coupled to the leads, we observe a nonmonotonic
temperature dependence of the nanotube conductance, which
results from a competition between the Kondo-box singlet and
the "conventional" Kondo state that couples the nanotube to
the leads. © 2010 The American Physical
Society.},
Doi = {10.1103/PhysRevB.82.161411},
Key = {fds245968}
}
@article{fds245969,
Author = {Bomze, Y and Mebrahtu, H and Borzenets, I and Makarovski, A and Finkelstein, G},
Title = {Resonant tunneling in a dissipative environment},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {79},
Number = {24},
Pages = {241402R},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {June},
ISSN = {1098-0121},
url = {http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=PRBMDO000079000024241402000001&idtype=cvips&gifs=yes},
Abstract = {We measure tunneling through a single quantum level in a
carbon nanotube quantum dot connected to resistive metal
leads. For the electrons tunneling to/from the nanotube, the
leads serve as a dissipative environment, which suppresses
the tunneling rate. In the regime of sequential tunneling,
the height of the single-electron conductance peaks
increases as the temperature is lowered, although it scales
more weakly than the conventional T-1. In the resonant
tunneling regime (temperature smaller than the level width),
the peak width approaches saturation, while the peak height
starts to decrease. Overall, the peak height shows a
nonmonotonic temperature dependence. We associate this
unusual behavior with the transition from the sequential to
the resonant tunneling through a single quantum level in a
dissipative environment. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevB.79.241402},
Key = {fds245969}
}
@article{fds245954,
Author = {Zhukov, AA and Finkelstein, G},
Title = {Dependence of transport through carbon nanotubes on local
coulomb potential},
Journal = {JETP Letters},
Volume = {89},
Number = {4},
Pages = {212-215},
Publisher = {Pleiades Publishing Ltd},
Year = {2009},
Month = {April},
ISSN = {0021-3640},
url = {http://dx.doi.org/10.1134/S0021364009040109},
Abstract = {In this paper, we present the results of helium temperature
transport measurements through carbon nanotubes using an AFM
conductive tip as a mobile gate for creation of a local
distributive Coulomb potential. In semiconducting nanotubes
we observe shifting of the conductance peaks with changing
of the AFM tip position. This result can be explained with a
particle in the box quantum model. In high quality metallic
nanotubes we observe that the local Coulomb potential does
not destroy the fourfold degeneracy of the energy levels. ©
2009 Pleiades Publishing, Ltd.},
Doi = {10.1134/S0021364009040109},
Key = {fds245954}
}
@article{fds245952,
Author = {Coskun, UC and Mebrahtu, H and Huang, PB and Huang, J and Sebba, D and Biasco, A and Makarovski, A and Lazarides, A and Labean, TH and Finkelstein, G},
Title = {Single-electron transistors made by chemical patterning of
silicon dioxide substrates and selective deposition of gold
nanoparticles},
Journal = {Applied Physics Letters},
Volume = {93},
Number = {12},
Pages = {123101-123101},
Publisher = {AIP Publishing},
Year = {2008},
Month = {September},
ISSN = {0003-6951},
url = {http://dx.doi.org/10.1063/1.2981705},
Abstract = {We describe a method to pattern SiO2 surfaces with colloidal
gold nanoparticles by e-beam lithography and selective
nanoparticle deposition. The simple technique allows us to
deposit nanoparticles in continuous straight lines, just one
nanoparticle wide and many nanoparticles long. We contact
the prepositioned nanoparticles with metal leads to form
single electron transistors. The Coulomb blockade pattern
surprisingly does not show the parasitic "offset charges" at
low temperatures, indicating relatively little surface
contamination. (C) 2008 American Institute of
Physics.},
Doi = {10.1063/1.2981705},
Key = {fds245952}
}
@article{fds245973,
Author = {Makarovski, A and Finkelstein, G},
Title = {Su(4) mixed valence regime in carbon nanotube quantum
dots},
Journal = {Physica B: Condensed Matter},
Volume = {403},
Number = {5-9},
Pages = {1555-1557},
Publisher = {Elsevier BV},
Year = {2008},
Month = {April},
ISSN = {0921-4526},
url = {http://dx.doi.org/10.1016/j.physb.2007.10.367},
Abstract = {We study the evolution of conductance regimes in carbon
nanotubes with doubly degenerate orbitals ("shells") by
controlling the contact transparency within the same sample.
For sufficiently open contacts, Kondo behavior is observed
for 1, 2, and 3 electrons in the topmost shell. As the
contacts are opened more, the sample enters the "mixed
valence" regime, where different charge states are strongly
hybridized by electron tunneling. Here, the conductance as a
function of gate voltage shows pronounced modulations with a
period of four electrons, and all single-electron features
are washed away at low temperature. We successfully describe
this behavior by a simple formula with no fitting
parameters. Finally, we find a surprisingly small energy
scale that controls the temperature evolution of conductance
and the tunneling density of states in the mixed valence
regime. © 2007 Elsevier B.V. All rights
reserved.},
Doi = {10.1016/j.physb.2007.10.367},
Key = {fds245973}
}
@article{fds245970,
Author = {Anders, FB and Logan, DE and Galpin, MR and Finkelstein,
G},
Title = {Zero-bias conductance in carbon nanotube quantum
dots.},
Journal = {Physical review letters},
Volume = {100},
Number = {8},
Pages = {086809},
Year = {2008},
Month = {February},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.100.086809},
Abstract = {We present numerical renormalization group calculations for
the zero-bias conductance of quantum dots made from
semiconducting carbon nanotubes. These explain and reproduce
the thermal evolution of the conductance for different
groups of orbitals, as the dot-lead tunnel coupling is
varied and the system evolves from correlated Kondo behavior
to more weakly correlated regimes. For integer fillings N=1,
2, 3 of an SU(4) model, we find universal scaling behavior
of the conductance that is distinct from the standard SU(2)
universal conductance, and concurs quantitatively with
experiment. Our results also agree qualitatively with
experimental differential conductance maps.},
Doi = {10.1103/physrevlett.100.086809},
Key = {fds245970}
}
@article{fds304539,
Author = {Park, SH and Finkelstein, G and LaBean, TH},
Title = {Stepwise self-assembly of DNA tile lattices using dsDNA
bridges.},
Journal = {Journal of the American Chemical Society},
Volume = {130},
Number = {1},
Pages = {40-41},
Year = {2008},
Month = {January},
url = {http://www.ncbi.nlm.nih.gov/pubmed/18072780},
Abstract = {The simple helical motif of double-strand DNA (dsDNA) has
typically been judged to be uninteresting for assembly in
DNA-based nanotechnology applications. In this letter, we
demonstrate construction of superstructures consisting of
heterogeneous DNA motifs using dsDNA in conjunction with
more complex, cross-tile building blocks. Incorporation of
dsDNA bridges in stepwise assembly processes can be used for
controlling length and directionality of superstructures and
is analogous to the "reprogramming" of sticky-ends displayed
on the DNA tiles. Two distinct self-assembled DNA lattices,
fixed-size nanoarrays, and extended 2D crystals of
nanotracks with nanobridges, are constructed and visualized
by high-resolution, liquid-phase atomic force
microscopy.},
Doi = {10.1021/ja078122f},
Key = {fds304539}
}
@article{fds245971,
Author = {Coskun, UC and Mebrahtu, H and Huang, P and Huang, J and Biasco, A and Makarovski, A and Lazarides, A and LaBean, T and Finkelstein,
G},
Title = {Chemical patterning of silicon dioxide substrates for
selective deposition of gold nanoparticles and fabrication
of single-electron transistors},
Journal = {Applied Physics Letters},
Volume = {93},
Pages = {123101},
Year = {2008},
Key = {fds245971}
}
@article{fds245972,
Author = {Park, SH and Finkelstein, G and Labean, TH},
Title = {Stepwise Self-Assembly of DNA Tile Lattices Using dsDNA
Bridges},
Journal = {Journal of the American Chemical Society},
Volume = {130},
Number = {40-41},
Pages = {40-41},
Year = {2008},
url = {http://www.ncbi.nlm.nih.gov/pubmed/18072780},
Abstract = {The simple helical motif of double-strand DNA (dsDNA) has
typically been judged to be uninteresting for assembly in
DNA-based nanotechnology applications. In this letter, we
demonstrate construction of superstructures consisting of
heterogeneous DNA motifs using dsDNA in conjunction with
more complex, cross-tile building blocks. Incorporation of
dsDNA bridges in stepwise assembly processes can be used for
controlling length and directionality of superstructures and
is analogous to the "reprogramming" of sticky-ends displayed
on the DNA tiles. Two distinct self-assembled DNA lattices,
fixed-size nanoarrays, and extended 2D crystals of
nanotracks with nanobridges, are constructed and visualized
by high-resolution, liquid-phase atomic force
microscopy.},
Doi = {10.1021/ja078122f},
Key = {fds245972}
}
@article{fds245974,
Author = {Makarovski, A and Zhukov, A and Liu, J and Finkelstein,
G},
Title = {Four-probe measurements of carbon nanotubes with narrow
metal contacts},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {76},
Number = {16},
Pages = {R161405},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {October},
ISSN = {1098-0121},
url = {http://dx.doi.org/10.1103/PhysRevB.76.161405},
Abstract = {We find that electrons in single-wall carbon nanotubes may
propagate substantial distances (tens of nanometers) under
metal contacts. We perform four-probe transport measurements
of the nanotube conductance and observe significant
deviations from the standard Kirchhoff's circuit rules. Most
noticeably, injecting current between two neighboring
contacts on one end of the nanotube induces a nonzero
voltage difference between two contacts on the other end. ©
2007 The American Physical Society.},
Doi = {10.1103/PhysRevB.76.161405},
Key = {fds245974}
}
@article{fds245977,
Author = {Prior, M and Makarovski, A and Finkelstein, G},
Title = {Low-temperature conductive tip atomic force microscope for
carbon nanotube probing and manipulation},
Journal = {Applied Physics Letters},
Volume = {91},
Number = {5},
Pages = {053112-053112},
Publisher = {AIP Publishing},
Year = {2007},
Month = {August},
ISSN = {0003-6951},
url = {http://dx.doi.org/10.1063/1.2759986},
Abstract = {The authors describe conductive tip atomic force microscope
used for imaging carbon nanotubes at low temperatures. The
instrument allows them to measure the tip-nanotube
conductance while performing the topographic scan of the
nanotubes on a nonconductive Si O2 substrate. For nanotubes
weakly coupled to the contacting electrode, they observe the
Coulomb blockade pattern in the tip-nanotube conductance.
They reversibly modified the conductance pattern by applying
the tip pressure. © 2007 American Institute of
Physics.},
Doi = {10.1063/1.2759986},
Key = {fds245977}
}
@article{fds245975,
Author = {Makarovski, A and Liu, J and Finkelstein, G},
Title = {Evolution of transport regimes in carbon nanotube quantum
dots.},
Journal = {Physical review letters},
Volume = {99},
Number = {6},
Pages = {066801},
Year = {2007},
Month = {August},
ISSN = {0031-9007},
url = {http://www.ncbi.nlm.nih.gov/pubmed/17930850},
Abstract = {We study the evolution of conductance regimes in carbon
nanotubes with doubly degenerate orbitals (shells) by
controlling the contact transparency within the same sample.
For sufficiently open contacts, Kondo behavior is observed
for 1, 2, and 3 electrons in the topmost shell. As the
contacts are opened more, the sample enters the "mixed
valence" regime, where different charge states are strongly
hybridized by electron tunneling. Here, the conductance as a
function of gate voltage shows pronounced modulations with a
period of four electrons, and all single-electron features
are washed away at low temperature. We successfully describe
this behavior by a simple formula with no fitting
parameters. Finally, we find a surprisingly small energy
scale that controls the temperature evolution of conductance
and the tunneling density of states in the mixed valence
regime.},
Doi = {10.1103/physrevlett.99.066801},
Key = {fds245975}
}
@article{fds304538,
Author = {Makarovski, A and Zhukov, A and Liu, J and Finkelstein,
G},
Title = {SU(2) and SU(4) Kondo effects in carbon nanotube quantum
dots},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {75},
Number = {24},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {June},
ISSN = {1098-0121},
url = {http://dx.doi.org/10.1103/PhysRevB.75.241407},
Abstract = {We study the SU(4) Kondo effect in carbon nanotube quantum
dots, where doubly degenerate orbitals form four-electron
"shells." The SU(4) Kondo behavior is investigated for one,
two, and three electrons in the topmost shell. While the
Kondo state of two electrons is quenched by a magnetic
field, in the case of an odd number of electrons two types
of SU(2) Kondo effect may survive. Namely, the spin SU(2)
state is realized in a magnetic field parallel to the
nanotube (inducing primarily orbital splitting). Application
of the perpendicular field (inducing Zeeman splitting)
results in the orbital SU(2) Kondo effect. © 2007 The
American Physical Society.},
Doi = {10.1103/PhysRevB.75.241407},
Key = {fds304538}
}
@article{fds245976,
Author = {Makarovski, A and Zhukov, A and Liu, J and Finkelstein,
G},
Title = {SU(4) and SU(2) Kondo Effects in Carbon Nanotube Quantum
Dots},
Journal = {Physical Review B},
Volume = {75},
Number = {24},
Pages = {R241407},
Year = {2007},
ISSN = {1098-0121},
url = {http://dx.doi.org/10.1103/PhysRevB.75.241407},
Abstract = {We study the SU(4) Kondo effect in carbon nanotube quantum
dots, where doubly degenerate orbitals form four-electron
"shells." The SU(4) Kondo behavior is investigated for one,
two, and three electrons in the topmost shell. While the
Kondo state of two electrons is quenched by a magnetic
field, in the case of an odd number of electrons two types
of SU(2) Kondo effect may survive. Namely, the spin SU(2)
state is realized in a magnetic field parallel to the
nanotube (inducing primarily orbital splitting). Application
of the perpendicular field (inducing Zeeman splitting)
results in the orbital SU(2) Kondo effect. © 2007 The
American Physical Society.},
Doi = {10.1103/PhysRevB.75.241407},
Key = {fds245976}
}
@article{fds245967,
Author = {Makarovski, A and An, L and Liu, J and Finkelstein,
G},
Title = {Persistent orbital degeneracy in carbon nanotubes},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {74},
Number = {15},
Pages = {155431},
Publisher = {American Physical Society (APS)},
Year = {2006},
Month = {November},
ISSN = {1098-0121},
url = {http://dx.doi.org/10.1103/PhysRevB.74.155431},
Abstract = {The quantum-mechanical orbitals in carbon nanotube quantum
dots are doubly degenerate over a large number of states. We
argue that this experimental observation indicates that
electrons are reflected without mode mixing at the
nanotube-metal contacts. Two electrons occupying a pair of
degenerate orbitals ("shell") are found to form a triplet
state starting from zero magnetic field. Finally, we observe
unexpected low-energy excitations at complete filling of a
four-electron shell. © 2006 The American Physical
Society.},
Doi = {10.1103/PhysRevB.74.155431},
Key = {fds245967}
}
@article{fds245950,
Author = {Park, SH and Prior, MW and LaBean, TH and Finkelstein,
G},
Title = {Optimized fabrication and electrical analysis of silver
nanowires templated on DNA molecules},
Journal = {Applied Physics Letters},
Volume = {89},
Number = {3},
Pages = {033901-033901},
Publisher = {AIP Publishing},
Year = {2006},
Month = {July},
ISSN = {0003-6951},
url = {http://dx.doi.org/10.1063/1.2234282},
Abstract = {We report on the electrical conductivity measurement of
silver nanowires templated on native X-bacteriophage and
synthetic double-stranded DNA molecules. After an
electroless chemical deposition, the metallized DNA wires
have a diameter down to 15 nm and are among the thinnest
metallic nanowires available to date. Two-terminal I-V
measurements demonstrating various conduction behaviors are
presented. DNA templated functional nanowires may, in the
near future, be targeted to connect at specific locations on
larger-scale circuits and represent a potential breakthrough
in the self-assembly of nanometer-scale structures for
electronics layout. © 2006 American Institute of
Physics.},
Doi = {10.1063/1.2234282},
Key = {fds245950}
}
@article{fds245978,
Author = {Park, SH and Prior, MW and LaBean, TH and Finkelstein,
G},
Title = {Silver nanowires templated on DNA molecules},
Journal = {Applied Physics Letters},
Volume = {89},
Pages = {033901},
Year = {2006},
Abstract = {We report on the electrical conductivity measurement of
silver nanowires templated on native λ-bacteriophage
and synthetic double- stranded DNA molecules. After an
electroless chemical deposition, the metallized DNA wires
have a diameter down to 15 nm, which are among the thinnest
metallic nanowires available to date. Two-terminal I-V
measurements demonstrating various conduction behaviors are
presented. DNA-templated functionalized nanowires represent
a potential breakthrough in the self-assembly of
nanometer-scale structures for electronics-layout because
they can be targeted to connect at specific locations on
larger-scale circuits.},
Key = {fds245978}
}
@article{fds245943,
Author = {Park, SH and Li, H and Yan, H and Reif, JH and Finkelstein, G and LaBean,
TH},
Title = {Self-assembled 1D DNA nanostructures as templates for silver
nanowires},
Journal = {2nd Conference on Foundations of Nanoscience: Self-Assembled
Architectures and Devices, FNANO 2005},
Pages = {193-196},
Year = {2005},
Month = {December},
Key = {fds245943}
}
@article{fds245979,
Author = {Park, SH and Barish, R and Li, H and Reif, JH and Finkelstein, G and Yan,
H and LaBean, TH},
Title = {Three-Helix Bundle DNA Tiles Self-Assemble into 2D Lattice
or 1D Templates for Silver Nanowires.},
Journal = {Nano Letters},
Volume = {5},
Number = {4},
Pages = {693},
Year = {2005},
Month = {March},
ISSN = {1530-6984},
url = {http://www.ncbi.nlm.nih.gov/pubmed/15826110},
Abstract = {We present a DNA nanostructure, the three- helix bundle
(3HB), which consists of three double helical DNA domains
connected by six immobile crossover junctions such that the
helix axes are not coplanar. The 3HB motif presents a
triangular cross-section with one helix lying in the groove
formed by the other two. By differential programming of
sticky- ends, 3HB tiles can be arrayed in two distinct
lattice conformations: one-dimensional filaments and
two-dimensional lattices. Filaments and lattices have been
visualized by high-resolution, tapping mode atomic force
microscopy (AFM) under buffer. Their dimensions are shown to
be in excellent agreement with designed structures. We also
demonstrate an electroless chemical deposition for
fabricating metallic nanowires templated on self-assembled
filaments. The metallized nanowires have diameters down to
20 nm and display Ohmic current-voltage characteristic.},
Doi = {10.1021/nl050108i},
Key = {fds245979}
}
@article{fds245992,
Author = {Park, SH and Yan, H and Reif, JH and LaBean, TH and Finkelstein,
G},
Title = {Electronic nanostructures templated on self-assembled DNA
scaffolds},
Journal = {Nanotechnology},
Volume = {15},
Number = {10},
Pages = {S525-S527},
Publisher = {IOP Publishing},
Year = {2004},
Month = {July},
url = {http://www.phy.duke.edu/~gleb/Pdf_FILES/nanotech.pdf},
Abstract = {We report on the self-assembly of one- and two-dimensional
DNA scaffolds, which serve as templates for the targeted
deposition of ordered nanoparticles and molecular arrays.
TheDNAnanostructures are easy to reprogram, and we
demonstrate two distinct conformations: sheets and tubes.
The DNA tubes and individual DNA molecules are metallized in
solution to produce ultra-thin metal wires.},
Doi = {10.1088/0957-4484/15/10/005},
Key = {fds245992}
}
@article{fds245993,
Author = {Yan, H and Park, SH and Finkelstein, G and Reif, JH and LaBean,
TH},
Title = {DNA-Templated Self-Assembly of Protein Arrays and Highly
Conductive Nanowires},
Journal = {Science},
Volume = {301},
Number = {5641},
Pages = {1882},
Year = {2003},
Month = {September},
url = {http://www.ncbi.nlm.nih.gov/pubmed/14512621},
Abstract = {A DNA nanostructure consisting of four four-arm junctions
oriented with a square aspect ratio was designed and
constructed. Programmable self-assembly of 4 x 4 tiles
resulted in two distinct lattice morphologies: uniform-width
nanoribbons and two-dimensional nanogrids, which both
display periodic square cavities. Periodic protein arrays
were achieved by templated self-assembly of streptavidin
onto the DNA nanogrids containing biotinylated
oligonucleotides. On the basis of a two-step metallization
procedure, the 4 x 4 nanoribbons acted as an excellent
scaffold for the production of highly conductive,
uniform-width, silver nanowires.},
Doi = {10.1126/science.1089389},
Key = {fds245993}
}
@article{fds304537,
Author = {Tessmer, SH and Finkelstein, G and Glicofridis, PI and Ashoori,
RC},
Title = {Modeling subsurface charge accumulation images of a quantum
hall liquid},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {66},
Number = {12},
Pages = {1253081-1253086},
Publisher = {American Physical Society (APS)},
Year = {2002},
Month = {September},
ISSN = {0163-1829},
url = {http://dx.doi.org/10.1103/PhysRevB.66.125308},
Abstract = {Subsurface charge accumulation imaging is a cryogenic
scanning probe technique that has recently been used to
spatially probe incompressible strips formed in a
two-dimensional electron system (2DES) at high magnetic
fields. In this paper, we present a detailed numerical
modeling of these data. At a basic level, the method
produces results that agree well with the predictions of
models based on simple circuit elements. Moreover, the
modeling method is sufficiently advanced to simulate
spatially resolved measurements. By comparing directly the
simulations to the experimentally measured data, we can
extract quantitatively local electronic features of the
2DES. In particular, we deduce the electron density of
states inside the incompressible strips and electrical
resistance across them.},
Doi = {10.1103/PhysRevB.66.125308},
Key = {fds304537}
}
@article{fds245998,
Author = {Tessmer, SH and Finkelstein, G and Glicofridis, PI and Ashoori,
RC},
Title = {Modeling Subsurface Charge Accumulation Images of a Quantum
Hall Liquid},
Journal = {Phys. Rev. B},
Volume = {66},
Number = {12},
Pages = {125308},
Year = {2002},
Month = {August},
ISSN = {0163-1829},
Abstract = {Subsurface charge accumulation imaging is a cryogenic
scanning probe technique that has recently been used to
spatially probe incompressible strips formed in a
two-dimensional electron system (2DES) at high magnetic
fields. In this paper, we present a detailed numerical
modeling of these data. At a basic level, the method
produces results that agree well with the predictions of
models based on simple circuit elements. Moreover, the
modeling method is sufficiently advanced to simulate
spatially resolved measurements. By comparing directly the
simulations to the experimentally measured data, we can
extract quantitatively local electronic features of the
2DES. In particular, we deduce the electron density of
states inside the incompressible strips and electrical
resistance across them.},
Key = {fds245998}
}
@article{fds246000,
Author = {Zheng, B and Lu, C and Gu, G and Makarovski, A and Finkelstein, G and Liu,
J},
Title = {Efficient CVD Growth of Single-Walled Carbon Nanotubes on
Surfaces Using Carbon Monoxide Precursor},
Journal = {Nano Letters},
Volume = {2},
Number = {8},
Pages = {895-898},
Publisher = {American Chemical Society (ACS)},
Year = {2002},
Month = {August},
url = {http://dx.doi.org/10.1021/nl025634d},
Abstract = {Single Walled carbon nanotubes (SWNTs) were grown directly
on flat substrates using chemical vapor deposition (CVD)
method with carbon monoxide and hydrogen mixture as feeding
gas. Comparing with other CVD methods, this new approach
yields higher efficiency and more reproducible results in
obtaining high quality SWNTs separated as individual
nanotubes on substrates. Such samples can be used to
fabricate nanodevices directly with no further purification
or dispersion. Important factors that affect the nanotube
growth and possible mechanisms are also discussed.},
Doi = {10.1021/nl025634d},
Key = {fds246000}
}
@article{fds304536,
Author = {Glicofridis, PI and Finkelstein, G and Ashoori, RC and Shayegan,
M},
Title = {Determination of the resistance across incompressible strips
through imaging of charge motion},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {65},
Number = {12},
Pages = {1213121-1213124},
Year = {2002},
Month = {March},
ISSN = {0163-1829},
Abstract = {Using charge-accumulation imaging, we measure the charge
flow across an incompressible strip and follow its evolution
with magnetic field. The strip runs parallel to the edge of
a gate deposited on the sample and forms at positions where
an exact number of integer Landau levels is filled. An RC
model of charging fits the data well and enables us to
determine the resistance across the strip. Surprisingly, we
find that the strip becomes more resistive as its width
decreases.},
Key = {fds304536}
}
@article{fds245999,
Author = {Glicofridis, PI and Finkelstein, G and Ashoori, RC and Shayegan,
M},
Title = {Determination of the resistance across incompressible strips
through imaging of charge motion},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {65},
Number = {12},
Pages = {1-4},
Year = {2002},
Month = {January},
ISSN = {0163-1829},
url = {http://dx.doi.org/10.1103/PhysRevB.65.121312},
Abstract = {Using charge-accumulation imaging, we measure the charge
flow across an incompressible strip and follow its evolution
with magnetic field. The strip runs parallel to the edge of
a gate deposited on the sample and forms at positions where
an exact number of integer Landau levels is filled. An
(formula presented) model of charging fits the data well and
enables us to determine the resistance across the strip.
Surprisingly, we find that the strip becomes more resistive
as its width decreases. © 2002 The American Physical
Society.},
Doi = {10.1103/PhysRevB.65.121312},
Key = {fds245999}
}
@article{fds245995,
Author = {Finkelstein, G and Glicofridis, PI and Tessmer, SH and Ashoori, RC and Melloch, MR},
Title = {Imaging of Low Compressibility Strips in the Quantum Hall
Liquid},
Journal = {Phys. Rev. B},
Volume = {61},
Number = {24},
Pages = {R16 323},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {December},
ISSN = {0163-1829},
url = {http://dx.doi.org/10.1103/PhysRevB.61.R16323},
Abstract = {Using subsurface charge accumulation scanning microscopy, we
image strips of low compressibility corresponding to several
integer quantum Hall filling factors. We study in detail the
strips at Landau level filling factors (Formula presented)
and 4. The observed strips appear significantly wider than
predicted by theory. We present a model accounting for the
discrepancy by considering a disorder-induced nonzero
density of states in the cyclotron gap. © 2000 The American
Physical Society.},
Doi = {10.1103/PhysRevB.61.R16323},
Key = {fds245995}
}
@article{fds245996,
Author = {Finkelstein, G and Glicofridis, PI and Ashoori, RC and Shayegan,
M},
Title = {Topographic mapping of the quantum hall liquid using a
few-electron bubble},
Journal = {Science},
Volume = {289},
Number = {5476},
Pages = {90-94},
Publisher = {American Association for the Advancement of Science
(AAAS)},
Year = {2000},
Month = {July},
url = {http://dx.doi.org/10.1126/science.289.5476.90},
Abstract = {A scanning probe technique was used to obtain a
high-resolution map of the random electrostatic potential
inside the quantum Hall liquid. A sharp metal tip, scanned
above a semiconductor surface, sensed charges in an embedded
twodimensional (2D) electron gas. Under quantum Hall effect
conditions, applying a positive voltage to the tip locally
enhanced the 2D electron density and created a 'bubble' of
electrons in an otherwise unoccupied Landau revel as the tip
scanned along the sample surface, the bubble followed
underneath. The tip sensed the motions of single electrons
entering or leaving the bubble in response to changes in the
local 2D electrostatic potential.},
Doi = {10.1126/science.289.5476.90},
Key = {fds245996}
}
@article{fds245997,
Author = {Finkelstein, G and Glicofridis, PI and Tessmer, SH and Ashoori, RC and Melloch, MR},
Title = {Imaging the low compressibility strips formed by the Quantum
Hall liquid in a smooth potential gradient},
Journal = {Physica E: Low-Dimensional Systems and Nanostructures},
Volume = {6},
Number = {1},
Pages = {251-254},
Publisher = {Elsevier BV},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1016/S1386-9477(99)00131-9},
Abstract = {The two-dimensional electron gas (2DEG) in the quantum Hall
regime close to integer filling factors was studied. In a
smooth potential gradient, low-compressibility strips
corresponding to integer Landau level filling factors are
observed. These strips turn out to be significantly wider
than predicted by theory, which does not include the
disorder potential. The width of the strip is determined by
a low, but finite density of states between the Landau
levels.},
Doi = {10.1016/S1386-9477(99)00131-9},
Key = {fds245997}
}
@article{fds304535,
Author = {Finkelstein, G and Glicofridis, PI and Tessmer, SH and Ashoori, RC and Melloch, MR},
Title = {Imaging of low-compressibility strips in the quantum Hall
liquid},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {61},
Number = {24},
Pages = {R16323-R16326},
Year = {2000},
ISSN = {0163-1829},
Abstract = {Using subsurface charge accumulation scanning microscopy, we
image strips of low compressibility corresponding to several
integer quantum Hall filling factors. We study in detail the
strips at Landau level filling factors ν=2 and 4. The
observed strips appear significantly wider than predicted by
theory. We present a model accounting for the discrepancy by
considering a disorder-induced nonzero density of states in
the cyclotron gap. ©2000 The American Physical
Society.},
Key = {fds304535}
}
@article{fds245994,
Author = {Glasberg, S and Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Comparative study of the negatively and positively charged
excitons in gaas quantum wells},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {59},
Number = {16},
Pages = {R10425-R10428},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevB.59.R10425},
Abstract = {We compare the photoluminescence spectra of the negatively
and positively charged excitons in GaAs quantum wells. We
use a structure which enables us to observe both complexes
within the same sample. We find that their binding energy
and Zeeman splitting are very similar at zero magnetic
field, but evolve very differently at high fields. We
discuss the implications of these observations on our
understanding of the charge excitons structure in high
magnetic fields. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevB.59.R10425},
Key = {fds245994}
}
@article{fds245946,
Author = {Ciulin, V and Finkelstein, G and Haacke, S and Ganière, JD and Umansky,
V and Bar-Joseph, I and Deveaud, B},
Title = {Dynamics of charged excitons in GaAs quantum wells under
high magnetic field},
Journal = {Physica B: Condensed Matter},
Volume = {256-258},
Pages = {466-469},
Publisher = {Elsevier BV},
Year = {1998},
Month = {December},
url = {http://dx.doi.org/10.1016/S0921-4526(98)00582-1},
Abstract = {We report on time-resolved photoluminescence studies of
charged and neutral excitons in a modulation doped GaAs
quantum well under resonant excitation and high magnetic
field. The radiative lifetime of the charged exciton is
rather short, 60 ps at zero field, and is found to increase
by a factor of ∼2 up to 7 T. The short lifetimes suggest
that, under magnetic field, the exciton bound in the trion
is delocalized. © 1998 Elsevier Science B.V. All rights
reserved.},
Doi = {10.1016/S0921-4526(98)00582-1},
Key = {fds245946}
}
@booklet{Finkelstein98a,
Author = {Finkelstein, G},
Title = {Gustav Magnus and his house: Commissioned by the Deutsche
Physikalische Gesellschaft},
Journal = {Technology And Culture},
Volume = {39},
Number = {3},
Pages = {568-569},
Year = {1998},
Month = {July},
Key = {Finkelstein98a}
}
@booklet{Finkelstein98b,
Author = {Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Shake-up processes of a two-dimensional electron gas in
GaAs/AlGaAs quantum wells at high magnetic
fields},
Journal = {Physica B: Condensed Matter},
Volume = {249-251},
Pages = {575-579},
Publisher = {Elsevier BV},
Year = {1998},
Month = {June},
url = {http://dx.doi.org/10.1016/S0921-4526(98)00190-2},
Abstract = {Shake-up processes in the photoluminescence spectra of a
two-dimensional electron gas in a GaAs/AlGaAs quantum well
at high magnetic fields are studied at a range of filling
factors. We find that when the electrons occupy only the
lowest Landau level these processes are strongly suppressed.
A peculiar dependence of a giant 'zeroth' shake-up line on
temperature and filling factor is reported. © 1998 Elsevier
Science B.V. All rights reserved.},
Doi = {10.1016/S0921-4526(98)00190-2},
Key = {Finkelstein98b}
}
@booklet{Finkelstein98c,
Author = {Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Shakeup processes in a two-dimensional electron gas in
GaAs/AlGaAs quantum wells at high magnetic
fields},
Journal = {Uspekhi Fizicheskikh Nauk},
Volume = {168},
Number = {2},
Pages = {121-123},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.3367/UFNr.0168.199802c.0121},
Doi = {10.3367/UFNr.0168.199802c.0121},
Key = {Finkelstein98c}
}
@booklet{Finkelstein98,
Author = {Finkelstein, G and Umansky, V and Bar-Joseph, I and Ciulin, V and Haacke, S and Ganière, J and Deveaud, B},
Title = {Charged exciton dynamics in GaAs quantum
wells},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {58},
Number = {19},
Pages = {12637-12640},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevB.58.12637},
Abstract = {We study the dynamics of the charged and neutral excitons in
a modulation-doped GaAs quantum well by time-resolved
photoluminescence under a resonant excitation. The radiative
lifetime of the charged exciton is found to be surprisingly
short, 60 ps. This time is temperature independent between 2
and 10 K, and increases by a factor of 2 at 6 T. We discuss
our findings in view of present theories of exciton
radiative decay. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevB.58.12637},
Key = {Finkelstein98}
}
@booklet{Finkelstein97,
Author = {Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Mechanism of shakeup processes in the photoluminescence of a
two-dimensional electron gas at high magnetic
fields},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {56},
Number = {16},
Pages = {10326-10331},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevB.56.10326},
Abstract = {We observe shakeup processes in the photoluminescence
spectra of a two-dimensional electron gas in a (Formula
presented) quantum well at high magnetic fields. We find
that when the electrons occupy only the lowest Landau level
these processes are strongly suppressed. We show that this
behavior can be accounted for by first-principles
calculations. We use the same considerations to explain the
giant intensity of the shakeup line, which appears just
below the main luminescence line. © 1997 The American
Physical Society.},
Doi = {10.1103/PhysRevB.56.10326},
Key = {Finkelstein97}
}
@booklet{Barjoseph97,
Author = {I. Barjoseph and G. Finkelstein},
Title = {Trions in GaAs quantum wells},
Journal = {Compound Semiconductors 1996},
Series = {INSTITUTE OF PHYSICS CONFERENCE SERIES},
Number = {155},
Pages = {711 -- 716},
Year = {1997},
Key = {Barjoseph97}
}
@booklet{Finkelstein96,
Author = {Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Optical spectroscopy of neutral and charged excitons in
GaAs/AlGaAs quantum wells in high magnetic
fields},
Journal = {Surface Science},
Volume = {361-362},
Number = {1-3},
Pages = {357-362},
Publisher = {Elsevier BV},
Year = {1996},
Month = {July},
url = {http://dx.doi.org/10.1016/0039-6028(96)00421-9},
Abstract = {We implement optical spectroscopy to study charged excitons
in modulation-doped GaAs/AlGaAs quantum wells. We report the
first observation of the positively charged exciton and of
the triplet state of the negatively charged exciton.
Applying a gate voltage at high magnetic fields, we
investigate the transition between metallic and insulating
states. We find that while the photoluminescence line of the
metallic two-dimensional electron gas transforms smoothly
into a negatively charged exciton, the Zeeman splitting of
this line exhibits an abrupt change at the metal-insulator
transition.},
Doi = {10.1016/0039-6028(96)00421-9},
Key = {Finkelstein96}
}
@booklet{Finkelstein96b,
Author = {Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Negatively and positively charged excitons in quantum
wells},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {53},
Number = {4},
Pages = {R1709-R1712},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevB.53.R1709},
Abstract = {We report the observation of the positively charged exciton
and of the triplet state of the negatively charged exciton
in modulation doped GaAs quantum wells. Applying a gate
voltage at high magnetic fields we find that the
photoluminescence line of the two-dimensional electron gas
smoothly transforms into a negatively charged exciton and
not into a neutral exciton. The Zeeman splitting of this
line exhibits an abrupt change at the metal-insulator
transition. © 1996 The American Physical
Society.},
Doi = {10.1103/PhysRevB.53.R1709},
Key = {Finkelstein96b}
}
@booklet{Finkelstein96a,
Author = {Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Shakeup processes in the recombination spectra of negatively
charged excitons},
Journal = {Physical Review B - Condensed Matter and Materials
Physics},
Volume = {53},
Number = {19},
Pages = {12593-12596},
Publisher = {American Physical Society (APS)},
Year = {1996},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevB.53.12593},
Abstract = {We report on shakeup processes in the luminescence spectra
of a negatively charged exciton ((Formula presented)) at
moderate magnetic fields. These processes manifest
themselves as a series of low-energy satellite peaks
emerging from the negatively charged exciton line. We
analyze the dependence of the (Formula presented) energy on
magnetic field. We conclude that at magnetic fields above
∼1 T the (Formula presented) structure can be viewed as an
electron at the lowest Landau level bound to an exciton. ©
1996 The American Physical Society.},
Doi = {10.1103/PhysRevB.53.12593},
Key = {Finkelstein96a}
}
@booklet{Finkelstein95,
Author = {Finkelstein, G and Bar-Joseph, I},
Title = {Charged excitons in GaAs quantum wells},
Journal = {Il Nuovo Cimento D},
Volume = {17},
Number = {11-12},
Pages = {1239-1245},
Publisher = {Springer Nature},
Year = {1995},
Month = {November},
ISSN = {0392-6737},
url = {http://dx.doi.org/10.1007/BF02457195},
Abstract = {We implement optical spectroscopy to study charged excitons
(trions) in modulation-doped GaAs/AlGaAs quantum wells. We
observe for the first time several new trions: the
positively charged exciton, the light-hole negatively
charged exciton and the triplet state of the negatively
charged exciton. © 1995 Società Italiana di
Fisica.},
Doi = {10.1007/BF02457195},
Key = {Finkelstein95}
}
@booklet{Barjoseph95,
Author = {Barjoseph, I and Finkelstein, G and Barad, S and Shtrikman, H and Levinson, Y},
Title = {4-wave-mixing in modulation-doped gaas quantum-wells under
strong magnetic-fields},
Journal = {Physica Status Solidi B-basic Research},
Volume = {188},
Number = {1},
Pages = {457-463},
Year = {1995},
Month = {March},
Key = {Barjoseph95}
}
@booklet{Finkelstein95a,
Author = {Finkelstein, G and Shtrikman, H and Bar-Joseph,
I},
Title = {Optical spectroscopy of a two-dimensional electron gas near
the metal-insulator transition},
Journal = {Physical Review Letters},
Volume = {74},
Number = {6},
Pages = {976-979},
Publisher = {American Physical Society (APS)},
Year = {1995},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.74.976},
Abstract = {We report on optical measurements of a two-dimensional
electron gas near the metal-insulator transition. We observe
the appearance of excitons and negatively charged excitons,
X-, at the onset of the transition. The fact that these
excitons appear at a relatively large average electron
density shows that transition is induced by localization of
single electrons in the electrostatic potential fluctuations
of the remote ionized donors. © 1995 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.74.976},
Key = {Finkelstein95a}
}
@article{fds322480,
Author = {Bar‐Joseph, I and Finkelstein, G and Bar‐Ad, S and Shtrikman, H and Levinson, Y},
Title = {Four‐wave mixing in modulation‐doped GaAs quantum wells
under strong magnetic fields},
Journal = {physica status solidi (b)},
Volume = {188},
Number = {1},
Pages = {457-463},
Publisher = {WILEY},
Year = {1995},
Month = {January},
url = {http://dx.doi.org/10.1002/pssb.2221880143},
Abstract = {Time‐resolved four‐wave mixing is used to study electron
scattering in modulation‐doped GaAs quantum wells in high
magnetic fields up to 8T. A strong increase in dephasing
times in strong magnetic fields is observed and attributed
to a decrease in the scattering rates relative to zero
field. An early time signal in high magnetic field is found,
which is due to a polarization interaction process. A strong
enhancement of the signal at the absorption edge is measured
which is attributed to the Fermi edge singularity. Copyright
© 1995 WILEY‐VCH Verlag GmbH & Co. KGaA},
Doi = {10.1002/pssb.2221880143},
Key = {fds322480}
}
@booklet{Barad94,
Author = {Bar-Ad, S and Bar-Joseph, I and Finkelstein, G and Levinson,
Y},
Title = {Biexcitons in short-pulse optical experiments in strong
magnetic fields in GaAs quantum wells},
Journal = {Physical Review B},
Volume = {50},
Number = {24},
Pages = {18375-18381},
Publisher = {American Physical Society (APS)},
Year = {1994},
Month = {January},
ISSN = {0163-1829},
url = {http://dx.doi.org/10.1103/PhysRevB.50.18375},
Abstract = {We present time-resolved differential-absorption data for
GaAs quantum wells, in which temporal oscillations
originating in a biexcitonic pairing appear. We interpret
the oscillations within a four-level model of the
exciton-biexciton system, and discuss the cases of
homogeneously and inhomogeneously broadened exciton
absorption lines. Our differential absorption measurements
in high magnetic fields normal to the quantum wells layers
show that both the oscillations frequency and phase depend
on the strength and direction of the magnetic field. The
frequency change corresponds to the exciton Zeeman splitting
in our samples. These findings are in excellent agreement
with the predictions of the model, and thus verify its
validity. © 1994 The American Physical Society.},
Doi = {10.1103/PhysRevB.50.18375},
Key = {Barad94}
}
@booklet{Finkelstein93,
Author = {Finkelstein, G and Bar-Ad, S and Carmel, O and Bar-Joseph, I and Levinson, Y},
Title = {Biexcitonic effects in transient nonlinear optical
experiments in quantum wells},
Journal = {Physical Review B},
Volume = {47},
Number = {19},
Pages = {12964-12967},
Publisher = {American Physical Society (APS)},
Year = {1993},
Month = {January},
ISSN = {0163-1829},
url = {http://dx.doi.org/10.1103/PhysRevB.47.12964},
Abstract = {We present a model for the nonlinear optical response of
quantum wells, which includes biexcitons. We show that
within this model, the interaction of two laser pulses,
mediated by the nonlinear susceptibility, results in
oscillations and in coupling between σ+ and σ- excitons.
This explains the temporal behavior of the differential
absorption and four-wave mixing in recent experiments [Phys.
Rev. Lett. 68, 349 (1992); 68, 1880 (1992)]. The
oscillations have a frequency equal to the biexciton binding
energy, and are different from known interference and
quantum beat phenomena. © 1993 The American Physical
Society.},
Doi = {10.1103/PhysRevB.47.12964},
Key = {Finkelstein93}
}
@booklet{Pieprzyk88,
Author = {J. Pieprzyk and G. Finkelstein},
Title = {Towards effective nonlinear cryptosystem
design},
Journal = {Iee Proceedings-e Computers And Digital Techniques},
Volume = {135},
Number = {6},
Pages = {325 -- 335},
Year = {1988},
Month = {November},
Key = {Pieprzyk88}
}
%% Preprints
@article{fds375225,
Author = {Zhao, L and Arnault, EG and Larson, TFQ and Watanabe, K and Taniguchi,
T and Amet, F and Finkelstein, G},
Title = {Non-local transport measurements in hybrid quantum Hall -
superconducting devices},
Year = {2023},
Month = {October},
Abstract = {We develop the expressions for the non-local resistances of
hybrid quantum Hall -- superconductor devices. Our
approximation depends on the crucial assumption that the
superconducting phase correlations between contacts do not
play a role. We verify the validity of our approach in two
devices: in the first one, a single superconducting contact
couples to multiple edge states, while in the second, there
are multiple superconducting electrodes. The results
obtained for the second device suggest that the
superconducting phase coherence is not maintained over our
micron-scale graphene devices. Possible violations of this
assumption may be used as an indication that superconducting
phase coherence is induced in quantum Hall
edges.},
Key = {fds375225}
}
@article{fds368990,
Author = {Larson, TFQ and Zhao, L and Arnault, EG and Wei, M-T and Seredinski, A and Li, H and Watanabe, K and Tanaguchi, T and Amet, F and Finkelstein,
G},
Title = {Noise-induced stabilization of dynamical states in a
non-Markovian system},
Year = {2022},
Month = {December},
url = {https://arxiv.org/abs/2212.13952},
Abstract = {A Josephson junction subject to an external RF excitation
may experience the inverse AC Josephson effect, where the
phase across the junction locks to the drive. The resulting
``Shapiro steps'' of quantized voltage are currently
utilized in primary voltage standards. The effect has also
been a key technique in the search for topological
superconductivity. Here, we study a particularly interesting
regime in which the zero voltage state becomes unstable at
zero DC bias, and the junction spontaneously develops the
first Shapiro step with a voltage V=±ℏω/2e. The
switching time between the +ℏω/2e and −ℏω/2e states
ranges from milliseconds to hours. Most interestingly, we
find a surprising regime with a non-monotonic temperature
dependence, in which the switching time demonstrates a
pronounced minimum at intermediate temperatures. Tuning of
the measurement parameters is also shown to give rise to a
tristable switching behavior, showcasing the potential for
further experiments in stochastic physics and quantum
thermodynamics.},
Key = {fds368990}
}
@article{fds368991,
Author = {Zhao, L and Iftikhar, Z and Larson, TFQ and Arnault, EG and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein, G},
Title = {Loss and decoherence at the quantum Hall - superconductor
interface},
Volume = {131},
Number = {17},
Pages = {176604},
Year = {2022},
Month = {October},
url = {https://arxiv.org/abs/2210.04842},
Abstract = {We perform a systematic study of Andreev conversion at the
interface between a superconductor and graphene in the
quantum Hall (QH) regime. We find that the probability of
Andreev conversion from electrons to holes follows an
unexpected but clear trend: the dependencies on temperature
and magnetic field are nearly decoupled. We discuss these
trends and the role of the superconducting vortices, whose
normal cores could both absorb and dephase the individual
electrons in a QH edge. Our Letter may pave the road to
engineering a future generation of hybrid devices for
exploiting superconductivity proximity in chiral
channels.},
Doi = {10.1103/physrevlett.131.176604},
Key = {fds368991}
}
@article{fds368992,
Author = {Chiles, J and Arnault, EG and Chen, C-C and Larson, TFQ and Zhao, L and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein,
G},
Title = {Non-Reciprocal Supercurrents in a Field-Free Graphene
Josephson Triode},
Year = {2022},
Month = {October},
url = {https://arxiv.org/abs/2210.02644},
Abstract = {Superconducting diodes are proposed non-reciprocal circuit
elements that should exhibit non-dissipative transport in
one direction while being resistive in the opposite
direction. Multiple examples of such devices have emerged in
the past couple of years, however their efficiency is
typically limited, and most of them require magnetic field
to function. Here we present a device achieving efficiencies
upwards of 90% while operating at zero field. Our samples
consist of a network of three graphene Josephson junctions
linked by a common superconducting island, to which we refer
as a Josephson triode. The triode is tuned by applying a
control current to one of the contacts, thereby breaking the
time-reversal symmetry of the current flow. The triode's
utility is demonstrated by rectifying a small (tens of nA
amplitude) applied square wave. We speculate that devices of
this type could be realistically employed in the modern
quantum circuits.},
Key = {fds368992}
}
@article{fds368993,
Author = {Zhao, L and Arnault, EG and Larson, TFQ and Iftikhar, Z and Seredinski,
A and Fleming, T and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein, G},
Title = {Graphene-based quantum Hall interferometer with self-aligned
side gates},
Year = {2022},
Month = {June},
Key = {fds368993}
}
@article{fds368994,
Author = {Arnault, EG and Idris, S and McConnell, A and Zhao, L and Larson, TFQ and Watanabe, K and Taniguchi, T and Finkelstein, G and Amet,
F},
Title = {Dynamical Stabilization of Multiplet Supercurrents in
Multi-terminal Josephson Junctions},
Year = {2022},
Month = {January},
Key = {fds368994}
}
@article{fds368638,
Author = {Ethan G. Arnault and Gleb Finklestein and Athby H. Al-Tawhid and Salva Salmani-Rezaie and David A. Muller and Divine P. Kumah and Mohammad S. Bahramy and Kaveh Ahadi},
Title = {Anisotropic Superconductivity at Epitaxial KTaO3(111)
interfaces},
Journal = {submitted to Science Advances},
Year = {2022},
Abstract = {A two-dimensional, anisotropic superconductivity was
recently discovered at the KTaO3 (111) interfaces. The
nature of the anisotropic superconducting transition remains
a subject of debate. To investigate the origins of the
observed behavior, we grew epitaxial LaSrMnO3/KTaO3(111)
het- erostructures. We show that the superconductivity is
robust against the in-plane magnetic field and violates the
Pauli limit. We also show that the Cooper pairs are more
resilient when the bias is along [11 ̄2] (I ∥ [11 ̄2])
and the magnetic field is along [1 ̄10] (B ∥ [1 ̄10]).
We discuss the anisotropic nature of superconductivity in
the context of electronic structure, orbital character, and
spin texture at the KTaO3 (111) interfaces. The results
point to new opportunities to enhance superconducting tran-
sition temperatures and critical fields in crystalline,
two-dimensional superconductors with strong spin-orbit
coupling.},
Key = {fds368638}
}
@article{fds368995,
Author = {Seredinski, A and Arnault, EG and Costa, VZ and Zhao, L and Larson, TFQ and Watanabe, K and Taniguchi, T and Amet, F and Newaz, AKM and Finkelstein,
G},
Title = {One-Dimensional Edge Contact to Encapsulated MoS2 with a
Superconductor},
Year = {2021},
Month = {January},
Key = {fds368995}
}
@article{fds360646,
Author = {G. Finkelstein},
Title = {Inverse AC Josephson Effect in Ballistic Multiterminal
Graphene Josephson Junctions},
Pages = {103-104},
Booktitle = {Proceedings of the Workshop on Innovative Nanoscale Devices
and Systems, Hawaii, USA},
Year = {2021},
Key = {fds360646}
}
@article{fds368996,
Author = {Arnault, EG and Larson, T and Seredinski, A and Zhao, L and Idris, S and McConnell, A and Watanabe, K and Taniguchi, T and Borzenets, IV and Amet, F and Finkelstein, G},
Title = {The Multi-terminal Inverse AC Josephson Effect},
Year = {2020},
Month = {December},
Key = {fds368996}
}
@article{fds368997,
Author = {Larson, TFQ and Zhao, L and Arnault, EG and Wei, MT and Seredinski, A and Li, H and Watanabe, K and Taniguchi, T and Amet, F and Finkelstein,
G},
Title = {Zero-bias crossings and peculiar Shapiro maps in graphene
Josephson junctions},
Year = {2020},
Month = {March},
Key = {fds368997}
}
@article{fds368998,
Author = {Ke, CT and Draelos, AW and Seredinski, A and Wei, MT and Li, H and Hernandez-Rivera, M and Watanabe, K and Taniguchi, T and Yamamoto, M and Tarucha, S and Bomze, Y and Borzenets, IV and Amet, F and Finkelstein,
G},
Title = {2$Φ_{0}$-periodic magnetic interference in ballistic
graphene Josephson junctions},
Year = {2019},
Month = {June},
Key = {fds368998}
}
@article{fds368629,
Author = {Bomze, Y and Mebrahtu, H and Borzenets, I and Makarovski, A and Finkelstein, G},
Title = {Resonant Tunneling in a Dissipative Environment},
Year = {2010},
Month = {October},
Key = {fds368629}
}
@article{fds368630,
Author = {Anders, FB and Logan, DE and Galpin, MR and Finkelstein,
G},
Title = {Zero-bias conductance in carbon nanotube quantum
dots},
Year = {2007},
Month = {November},
Key = {fds368630}
}
@article{fds368631,
Author = {Makarovski, A and Zhukov, A and Liu, J and Finkelstein,
G},
Title = {Four-Probe Measurements of Carbon Nanotubes with Narrow
Metal Contacts},
Year = {2007},
Month = {September},
Key = {fds368631}
}
@article{fds368632,
Author = {Makarovski, A and Liu, J and Finkelstein, G},
Title = {Evolution of SU(4) Transport Regimes in Carbon Nanotube
Quantum Dots},
Year = {2006},
Month = {August},
Key = {fds368632}
}
@article{fds368633,
Author = {Makarovski, A and An, L and Liu, J and Finkelstein,
G},
Title = {Persistent Orbital Degeneracy in Carbon Nanotubes},
Year = {2005},
Month = {August},
Key = {fds368633}
}
@article{fds368634,
Author = {Glicofridis, PI and Finkelstein, G and Ashoori, RC and Shayegan,
M},
Title = {Direct observation of the charging of a 2D electron gas
through an incompressible strip in the quantum Hall
regime},
Year = {2001},
Month = {October},
Key = {fds368634}
}
@article{fds368635,
Author = {Finkelstein, G and Glicofridis, PI and Tessmer, SH and Ashoori, RC and Melloch, MR},
Title = {Imaging of Low Compressibility Strips in the Quantum Hall
Liquid},
Year = {1999},
Month = {October},
Key = {fds368635}
}