277 research outputs found
Excess Noise in Biased Superconducting Weak Links
Non-equilibrium excess noise of a short quasi one-dimensional constriction
between two superconductors is considered. A general expression for the
current-current correlation function valid for arbitrary temperatures and bias
voltages is derived. This formalism is applied to a current-carrying quantum
channel with perfect transparency. Contrary to a transparent channel separating
two normal conductors, a weak link between two superconductors exhibits a
finite level of noise. The source of noise is fractional Andreev scattering of
quasiparticles with energies greater than the half-width of the
superconducting gap. For high bias voltages, , the relation
between the zero-frequency limit of the noise spectrum, , and the excess
current reads . As both the excess noise and the excess current vanish linearly in
, %, their ratio being constant.Comment: 8 pages (Latex), 1 figur
Noise in a Quantum Point Contact due to a Fluctuating Impurity Configuration
We propose a theoretical model for the low-frequency noise observed in a
quantum point contact (QPC) electrostatically defined in the 2D electron gas at
a GaAs-AlGaAs interface. In such contacts electron scattering by soft impurity-
or boundary potentials coherently splits an incoming wave function between
different transverse modes. Interference between these modes have been
suggested to explain observed non-linearities in the QPC-conductance. In this
study we invoke the same mechanism and the time-dependent current due to soft
dynamical impurity scattering in order to analyze the low-frequency
(telegraph-like) noise which has been observed along with a nonlinear
conductance. For the simplified case of a channel with two extended (current
carrying) modes, a simple analytical formula for the noise intensity is
derived. Generally we have found qualitative similarities between the noise and
the square of the transconductance. Nevertheless, incidentally there may be
situations when noise is suppressed but transconductance enhanced.Comment: 9 revte
Quantum Scalar Field on the Massless (2+1)-Dimensional Black Hole Background
The behavior of a quantum scalar field is studied in the metric ground state
of the (2+1)-dimensional black hole of Ba\~nados, Teitelboim and Zanelli which
contains a naked singularity. The one-loop BTZ partition function and the
associate black hole effective entropy, the expectation value of the quantum
fluctuation as well as the renormalized expectation value of the stress tensor
are explicitly computed in the framework of the -function procedure.
This is done for all values of the coupling with the curvature, the mass of the
field and the temperature of the quantum state. In the massless conformally
coupled case, the found stress tensor is used for determining the quantum back
reaction on the metric due to the scalar field in the quantum vacuum state, by
solving the semiclassical Einstein equations. It is finally argued that, within
the framework of the 1/N expansion, the Cosmic Censorship Hypothesis is
implemented since the naked singularity of the ground state metric is shielded
by an event horizon created by the back reaction.Comment: 18 pages, RevTeX, no figures, minor changes, final version accepted
for publication in Phys. Rev.
Radiation from the extremal black holes
The radiation from extreme Reissner-Nordstr\"{o}m black holes is computed by
explicitly considering the collapse of a spherical charged shell. No neutral
scalar radiation is found but there is emission of charged particles, provided
the charge to mass ratio be different from one. The absence of thermal effects
is in accord with the predictions of the euclidean theory but since the body
emits charged particles the entropy issue is not the same as for eternal
extreme black holes.Comment: 4 pages, LaTex, no figure
Finite voltage shot noise in normal-metal - superconductor junctions
We express the low-frequency shot noise in a disordered normal-metal -
superconductor (NS) junction at finite (subgap) voltage in terms of the normal
scattering amplitudes and the Andreev reflection amplitude. In the multichannel
limit, the conductance exhibits resonances which are accompanied by an
enhancement of the (differential) shot noise. In the study of multichannel
single and double barrier junctions we discuss the noise properties of coherent
transport at low versus high voltage with respect to the Andreev level spacing.Comment: 6 pages, Latex, 2 eps-figures, to be published in PRB, Appendix on
Bogoliubov equation
Flicker Noise Induced by Dynamic Impurities in a Quantum Point Contact
We calculate low-frequency noise (LFN) in a quantum point contact (QPC) which
is electrostatically defined in a 2D electron gas of a GaAs-AlGaAs
heterostructure. The conventional source of LFN in such systems are scattering
potentials fluctuating in time acting upon injected electrons. One can
discriminate between potentials of different origin -- noise may be caused by
the externally applied gate- and source-drain voltages, the motion of defects
with internal degrees of freedom close to the channel, electrons hopping
between localized states in the doped region, etc. In the present study we
propose a model of LFN based upon the assumption that there are many dynamic
defects in the surrounding of a QPC. A general expression for the
time-dependent current-current correlation function is derived and applied to a
QPC with quantized conductance. It is shown that the level of LFN is
significantly different at and between the steps in a plot of the conductance
vs. gate voltage. On the plateaus, the level of noise is found to be low and
strongly model-dependent. At the steps, LFN is much larger and only weakly
model-dependent. As long as the system is biased to be at a fixed position
relative the conductance step,Comment: 26 revtex APR 94-4
Shot noise in normal metal-d-wave superconducting junctions
We present theoretical calculations and predictions for the shot noise in
voltage biased junctions of superconductors and normal metal
counter-electrodes. In the clean limit for the d-wave superconductor the shot
noise vanishes at zero voltage because of resonant Andreev reflection by
zero-energy surface bound states. We examine the sensitivity of this resonance
to impurity scattering. We report theoretical results for the magnetic field
dependence of the shot noise, as well the fingerprints of subdominant - and
pairing channels.Comment: 15 pages, 8 figures and 3 tables embedde
Shot noise in mesoscopic systems
This is a review of shot noise, the time-dependent fluctuations in the
electrical current due to the discreteness of the electron charge, in small
conductors. The shot-noise power can be smaller than that of a Poisson process
as a result of correlations in the electron transmission imposed by the Pauli
principle. This suppression takes on simple universal values in a symmetric
double-barrier junction (suppression factor 1/2), a disordered metal (factor
1/3), and a chaotic cavity (factor 1/4). Loss of phase coherence has no effect
on this shot-noise suppression, while thermalization of the electrons due to
electron-electron scattering increases the shot noise slightly. Sub-Poissonian
shot noise has been observed experimentally. So far unobserved phenomena
involve the interplay of shot noise with the Aharonov-Bohm effect, Andreev
reflection, and the fractional quantum Hall effect.Comment: 37 pages, Latex, 10 figures (eps). To be published in "Mesoscopic
Electron Transport," edited by L. P. Kouwenhoven, G. Schoen, and L. L. Sohn,
NATO ASI Series E (Kluwer Academic Publishing, Dordrecht
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