1,769 research outputs found
Cooper pair splitting in a nanoSQUID geometry at high transparency
We describe a Josephson device composed of two superconductors separated by
two interacting quantum dots in parallel, as a probe for Cooper pair splitting.
In addition to sequential tunneling of electrons through each dot, an
additional transport channel exists in this system: crossed Andreev reflection,
where a Cooper pair from the source is split between the two dots and
recombined in the drain superconductor. Unlike non-equilibrium scenarios for
Cooper pair splitting which involves superconducting/normal metal "forks", our
proposal relies on an Aharonov-Bohm measurement of the DC Josephson current
when a flux is inserted between the two dots. We provide a path integral
approach to treat arbitrary transparencies, and we explore all contributions
for the individual phases ( or ) of the quantum dots. We propose a
definition of the Cooper pair splitting efficiency for arbitrary
transparencies, which allows us to find the phase associations which favor the
crossed Andreev process. Possible applications to experiments using nanowires
as quantum dots are discussed.Comment: 12 pages, 13 figure
Hanbury Brown and Twiss noise correlations in a topological superconductor beam splitter
We study Hanbury-Brown and Twiss current cross-correlations in a
three-terminal junction where a central topological superconductor (TS)
nanowire, bearing Majorana bound states at its ends, is connected to two normal
leads. Relying on a non-perturbative Green function formalism, our calculations
allow us to provide analytical expressions for the currents and their
correlations at subgap voltages, while also giving exact numerical results
valid for arbitrary external bias. We show that when the normal leads are
biased at voltages and smaller than the gap, the sign of the
current cross-correlations is given by -\mbox{sgn}(V_1 \, V_2). In
particular, this leads to positive cross-correlations for opposite voltages, a
behavior in stark contrast with the one of a standard superconductor, which
provides a direct evidence of the presence of the Majorana zero-mode at the
edge of the TS. We further extend our results, varying the length of the TS
(leading to an overlap of the Majorana bound states) as well as its chemical
potential (driving it away from half-filling), generalizing the boundary TS
Green function to those cases. In the case of opposite bias voltages,
\mbox{sgn}(V_1 \, V_2)=-1, driving the TS wire through the topological
transition leads to a sign change of the current cross-correlations, providing
yet another signature of the physics of the Majorana bound state.Comment: 14 pages, 8 figure
Multipair DC-Josephson Resonances in a biased all-superconducting Bijunction
An all-superconducting bijunction consists of a central superconductor
contacted to two lateral superconductors, such that non-local crossed Andreev
reflection is operating. Then new correlated transport channels for the Cooper
pairs appear in addition to those of separated conventional Joseph- son
junctions. We study this system in a configuration where the superconductors
are connected through gate-controllable quantum dots. Multipair phase-coherent
resonances and phase-dependent multiple Andreev reflections are both obtained
when the voltages of the lateral superconductors are commensurate, and they add
to the usual local dissipative transport due to quasiparticles. The two-pair
resonance (quartets) as well as some other higher order multipair resonances
are {\pi}-shifted at low voltage. Dot control can be used to dramatically
enhance the multipair current when the voltages are resonant with the dot
levels.Comment: 6 page
Proposal for the observation of nonlocal multipair production: the biSQUID
We propose an all-superconducting three-terminal setup consisting in a carbon
nanotube (or semiconducting nanowire) contacted to three superconducting leads.
The resulting device, referred to as a "biSQUID", is made of four quantum dots
arranged in two loops of different surface area. We show how this biSQUID can
prove a useful tool to probe nonlocal quantum phenomena in an interferometry
setup. We study the measured critical current as a function of the applied
magnetic field, which shows peaks in its Fourier spectrum, providing clear
signatures of multipair Josephson processes. The device does not require any
specific fine-tuning as these features are observed for a wide range of
microscopic parameters -- albeit with a non-trivial dependence. Competing
effects which may play a significant role in actual experimental realizations
are also explored.Comment: 13 pages, 9 figure
Giant shot noise from Majorana zero modes in topological trijunctions
The clear-cut experimental identification of Majorana bound states in
transport measurements still poses experimental challenges. We here show that
the zero-energy Majorana state formed at a junction of three topological
superconductor wires is directly responsible for giant shot noise amplitudes,
in particular at low voltages and for small contact transparency. The only
intrinsic noise limitation comes from the current-induced dephasing rate due to
multiple Andreev reflection processes
Weak-field Hall effect and static polarizability of Bloch electrons
A theory of the weak field Hall effect of Bloch electrons based on the
analysis of the forces acting on electrons is presented. It is argued that the
electric current is composed of two contributions, that driven by the electric
field along current flow and the non-dissipative contribution originated in
demagnetization currents. The Hall resistance as a function of the electron
concentration for the tight-binding model of a crystal with square lattice and
body-centered cubic lattice is described in detail. For comparison the effect
of strong magnetic fields is also discussed
Euclidean versus hyperbolic congestion in idealized versus experimental networks
This paper proposes a mathematical justification of the phenomenon of extreme
congestion at a very limited number of nodes in very large networks. It is
argued that this phenomenon occurs as a combination of the negative curvature
property of the network together with minimum length routing. More
specifically, it is shown that, in a large n-dimensional hyperbolic ball B of
radius R viewed as a roughly similar model of a Gromov hyperbolic network, the
proportion of traffic paths transiting through a small ball near the center is
independent of the radius R whereas, in a Euclidean ball, the same proportion
scales as 1/R^{n-1}. This discrepancy persists for the traffic load, which at
the center of the hyperbolic ball scales as the square of the volume, whereas
the same traffic load scales as the volume to the power (n+1)/n in the
Euclidean ball. This provides a theoretical justification of the experimental
exponent discrepancy observed by Narayan and Saniee between traffic loads in
Gromov-hyperbolic networks from the Rocketfuel data base and synthetic
Euclidean lattice networks. It is further conjectured that for networks that do
not enjoy the obvious symmetry of hyperbolic and Euclidean balls, the point of
maximum traffic is near the center of mass of the network.Comment: 23 pages, 4 figure
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