The platform will undergo maintenance on Sep 14 at about 7:45 AM EST and will be unavailable for approximately 2 hours.
2001
DOI: 10.1103/physrevb.64.081304
|View full text |Cite
|
Sign up to set email alerts
|

Nonlocal effects in the shot noise of diffusive superconductor–normal-metal systems

Abstract: A cross-shaped diffusive system with two superconducting and two normal electrodes is considered. A voltage eV < ∆ is applied between the normal leads. Even in the absence of average current through the superconducting electrodes their presence increases the shot noise at the normal electrodes and doubles it in the case of a strong coupling to the superconductors. The nonequilibrium noise at the superconducting electrodes remains finite even in the case of a vanishingly small transport current due to the absen… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
4
0

Year Published

2002
2002
2021
2021

Publication Types

Select...
4

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(4 citation statements)
references
References 19 publications
0
4
0
Order By: Relevance
“…The normal NW segments on both sides of the S contact are assumed to be much longer than the superconducting coherence length and the applied voltage is much higher than the Thouless energy, L D/eV , D/∆, where D is the diffusion coefficient. This allows to neglect the penetration of the superconducting condensate from the proximity region underneath the S contact into the normal segments and treat them as metallic diffusive conductors [18,19]. The length of the S segment (the part of the device consisting of a part of NW and S contact above it) is assumed to be much larger than both the NW diameter and the superconducting coherence length, which enables to us to describe the quasiparticle transport via this segment as effectively one-dimensional and neglect the processes of Cooper pair splitting and elastic cotunneling [29].…”
Section: Semiclassical Modelmentioning
confidence: 99%
See 3 more Smart Citations
“…The normal NW segments on both sides of the S contact are assumed to be much longer than the superconducting coherence length and the applied voltage is much higher than the Thouless energy, L D/eV , D/∆, where D is the diffusion coefficient. This allows to neglect the penetration of the superconducting condensate from the proximity region underneath the S contact into the normal segments and treat them as metallic diffusive conductors [18,19]. The length of the S segment (the part of the device consisting of a part of NW and S contact above it) is assumed to be much larger than both the NW diameter and the superconducting coherence length, which enables to us to describe the quasiparticle transport via this segment as effectively one-dimensional and neglect the processes of Cooper pair splitting and elastic cotunneling [29].…”
Section: Semiclassical Modelmentioning
confidence: 99%
“…Following the semiclassical approach of Nagaev and Büttiker [18,19] we calculate the EEDs f 1 (ε) and f 2 (ε) on the two boundaries of the S segment at x = x 1 and x = x 2 , see Fig. 1.…”
Section: Energy Distributionsmentioning
confidence: 99%
See 2 more Smart Citations