261 research outputs found
Shot noise in superconducting junctions with weak link formed by Anderson impurity
A theory is developed to study shot noise in superconducting (SAS) and hybrid
(SAN) junctions with singly occupied Anderson impurity (A) as a weak link. The
zero-frequency DC component of the shot noise spectral density is calculated at
zero temperature as a function of the bias at different Coulomb repulsion
strengths U, and show a remarkable structure resulting from combination of
electron-electron interaction and Andreev reflections.Comment: 4 two column pages including 4 .eps figure
Non-equilibrium current noise in mesoscopic disordered SNS junctions
Current noise in superconductor-normal metal-superconductor (SNS) junctions
is calculated within the scattering theory of multiple Andreev reflections
(MAR). It is shown that the noise exhibits subharmonic gap singularities at
, both in single-mode junctions with arbitrary
transparency and in multi-mode disordered junctions. The subharmonic
structure is superimposed with monotonic increase of the effective transferred
charge with decreasing bias voltage. Other features of the
noise include a step-like increase of in junctions with small , and a
divergence at small voltages and excess noise , where is the excess current, at large voltages, in
junctions with diffusive transport.Comment: 5 page
Follicular regulatory T cells control humoral autoimmunity via NFAT2-regulated CXCR5 expression
Maturation of high-affinity B lymphocytes is precisely controlled during the germinal center reaction. This is dependent on CD4(+)CXCR5(+) follicular helper T cells (TFH) and inhibited by CD4(+)CXCR5(+)Foxp3(+) follicular regulatory T cells (TFR). Because NFAT2 was found to be highly expressed and activated in follicular T cells, we addressed its function herein. Unexpectedly, ablation of NFAT2 in T cells caused an augmented GC reaction upon immunization. Consistently, however, TFR cells were clearly reduced in the follicular T cell population due to impaired homing to B cell follicles. This was TFR-intrinsic because only in these cells NFAT2 was essential to up-regulate CXCR5. The physiological relevance for humoral (auto-)immunity was corroborated by exacerbated lupuslike disease in the presence of NFAT2-deficient TFR cells
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
Current noise in long diffusive SNS junctions in the incoherent MAR regime
Spectral density of current fluctuations at zero frequency is calculated for
a long diffusive SNS junction with low-resistive interfaces. At low
temperature, T << Delta, the subgap shot noise approaches linear voltage
dependence, S=(2/ 3R)(eV + 2Delta), which is the sum of the shot noise of the
normal conductor and voltage independent excess noise. This result can also be
interpreted as the 1/3-suppressed Poisson noise for the effective charge q =
e(1+2Delta/eV) transferred by incoherent multiple Andreev reflections (MAR). At
higher temperatures, anomalies of the current noise develop at the gap
subharmonics, eV = 2Delta/n. The crossover to the hot electron regime from the
MAR regime is analyzed in the limit of small applied voltages.Comment: improved version, to be published in Phys. Rev.
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
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.
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
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