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Large-scale superconductivity-induced conductance suppression in mesoscopic normal-superconducting structures

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Large-scale superconductivity-induced conductance suppression in mesoscopic normal-superconducting structures. / Seviour, R.; Lambert, C. J. ; Leadbeater, M.
In: Superlattices and Microstructures, Vol. 25, No. 5-6, 05.1999, p. 639-645.

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Seviour R, Lambert CJ, Leadbeater M. Large-scale superconductivity-induced conductance suppression in mesoscopic normal-superconducting structures. Superlattices and Microstructures. 1999 May;25(5-6):639-645. doi: 10.1006/spmi.1999.0722

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Seviour, R. ; Lambert, C. J. ; Leadbeater, M. / Large-scale superconductivity-induced conductance suppression in mesoscopic normal-superconducting structures. In: Superlattices and Microstructures. 1999 ; Vol. 25, No. 5-6. pp. 639-645.

Bibtex

@article{dec66a129ce14816a19e6442b9c76982,
title = "Large-scale superconductivity-induced conductance suppression in mesoscopic normal-superconducting structures",
abstract = "Experiments on hybrid superconducting normal-metal structures have revealed that even in the absence of tunnel junctions the onset of superconductivity can lead to a decrease in the electrical conductance by an amount many orders of magnitude greater than e(2)/h. In this paper, we provide a theory of this phenomenon which shows that it originates from an instability in the four-probe conductance which is absent from two-probe measurements. We compare the zero-bias, zero-temperature four-probe conductances GN and Gs of a normal diffusive metal in contact with a superconductor in both the normal (N) and superconducting (S) states, respectively. In the absence of tunnel barriers, the ensemble average of the difference delta G = G(S) - G(N) vanishes, in agreement with quasiclassical theory. However, we also predict that there exist macroscopic sample specific fluctuations in delta G, which lie beyond quasiclassical theory and allow large negative values of 6G to occur. (C) 1999 Academic Press.",
author = "R. Seviour and Lambert, {C. J.} and M. Leadbeater",
year = "1999",
month = may,
doi = "10.1006/spmi.1999.0722",
language = "English",
volume = "25",
pages = "639--645",
journal = "Superlattices and Microstructures",
issn = "0749-6036",
publisher = "Academic Press Inc.",
number = "5-6",

}

RIS

TY - JOUR

T1 - Large-scale superconductivity-induced conductance suppression in mesoscopic normal-superconducting structures

AU - Seviour, R.

AU - Lambert, C. J.

AU - Leadbeater, M.

PY - 1999/5

Y1 - 1999/5

N2 - Experiments on hybrid superconducting normal-metal structures have revealed that even in the absence of tunnel junctions the onset of superconductivity can lead to a decrease in the electrical conductance by an amount many orders of magnitude greater than e(2)/h. In this paper, we provide a theory of this phenomenon which shows that it originates from an instability in the four-probe conductance which is absent from two-probe measurements. We compare the zero-bias, zero-temperature four-probe conductances GN and Gs of a normal diffusive metal in contact with a superconductor in both the normal (N) and superconducting (S) states, respectively. In the absence of tunnel barriers, the ensemble average of the difference delta G = G(S) - G(N) vanishes, in agreement with quasiclassical theory. However, we also predict that there exist macroscopic sample specific fluctuations in delta G, which lie beyond quasiclassical theory and allow large negative values of 6G to occur. (C) 1999 Academic Press.

AB - Experiments on hybrid superconducting normal-metal structures have revealed that even in the absence of tunnel junctions the onset of superconductivity can lead to a decrease in the electrical conductance by an amount many orders of magnitude greater than e(2)/h. In this paper, we provide a theory of this phenomenon which shows that it originates from an instability in the four-probe conductance which is absent from two-probe measurements. We compare the zero-bias, zero-temperature four-probe conductances GN and Gs of a normal diffusive metal in contact with a superconductor in both the normal (N) and superconducting (S) states, respectively. In the absence of tunnel barriers, the ensemble average of the difference delta G = G(S) - G(N) vanishes, in agreement with quasiclassical theory. However, we also predict that there exist macroscopic sample specific fluctuations in delta G, which lie beyond quasiclassical theory and allow large negative values of 6G to occur. (C) 1999 Academic Press.

U2 - 10.1006/spmi.1999.0722

DO - 10.1006/spmi.1999.0722

M3 - Journal article

VL - 25

SP - 639

EP - 645

JO - Superlattices and Microstructures

JF - Superlattices and Microstructures

SN - 0749-6036

IS - 5-6

ER -