2019
DOI: 10.1103/physrevb.99.144504
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Cross-correlated shot noise in three-terminal superconducting hybrid nanostructures

Abstract: We work out a unified theory describing both non-local electron transport and cross-correlated shot noise in a three-terminal normal-superconducting-normal (NSN) hybrid nanostructure. We describe noise cross correlations both for subgap and overgap bias voltages and for arbitrary distribution of channel transmissions in NS contacts. We specifically address a physically important situation of diffusive contacts and demonstrate a non-trivial behavior of non-local shot noise exhibiting both positive and negative … Show more

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Cited by 18 publications
(17 citation statements)
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“…Shot noise cross-correlations vanish at V 2 = −V 1 in transparent limit which has also been predicted in Ref. [52]. In the subsections below, we try to understand the reasons for the plots shown in Fig.…”
Section: Processes At Playsupporting
confidence: 65%
See 2 more Smart Citations
“…Shot noise cross-correlations vanish at V 2 = −V 1 in transparent limit which has also been predicted in Ref. [52]. In the subsections below, we try to understand the reasons for the plots shown in Fig.…”
Section: Processes At Playsupporting
confidence: 65%
“…As predicted in Ref. [52], shot noise cross-correlations for swave superconductor in transparent limit at zero temperature reduces to,…”
Section: Transparent Limitsupporting
confidence: 64%
See 1 more Smart Citation
“…In coherent modeling, we employ the Landauer approach with Andreev reflection 43,46 for calculating the local thermoelectric current; Lorentzian resonance line shapes are employed for transport in the quantum dots 35,44,47,48 . For the non-local current, we employ a standard crossed Andreev reflection formalism 2,[49][50][51] . In our incoherent theory, based on scattering matrix formalism 1,4,52 , we also include the influence of internal thermally generated current sources and their back-action effect owing to the environmental impedance caused by graphene ribbons.…”
Section: Methodsmentioning
confidence: 99%
“…( 2), γ AR depends on the number of conduction channels N α in the junction and the junction resistance R Tα in relation to the resistance quantum R K [20,33,38]. The non-local processes depend instead on the total junction resistances versus quasiparticle diffusion away from the junction area set by R S [39] but not on N α nor R K . In addition, the non-local processes have an exponential suppression e −l/ξ for increasing distance l between the two junctions.…”
mentioning
confidence: 99%