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Giant conductance oscillations in mesoscopic Andreev interferometers

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Giant conductance oscillations in mesoscopic Andreev interferometers. / Allsopp, N K ; Cañizares, J S ; Raimondi, R et al.
In: Journal of Physics: Condensed Matter, Vol. 8, No. 26, 1996, p. L377-L384.

Research output: Contribution to Journal/MagazineLetterpeer-review

Harvard

Allsopp, NK, Cañizares, JS, Raimondi, R & Lambert, C 1996, 'Giant conductance oscillations in mesoscopic Andreev interferometers', Journal of Physics: Condensed Matter, vol. 8, no. 26, pp. L377-L384. https://doi.org/10.1088/0953-8984/8/26/001

APA

Allsopp, N. K., Cañizares, J. S., Raimondi, R., & Lambert, C. (1996). Giant conductance oscillations in mesoscopic Andreev interferometers. Journal of Physics: Condensed Matter, 8(26), L377-L384. https://doi.org/10.1088/0953-8984/8/26/001

Vancouver

Allsopp NK, Cañizares JS, Raimondi R, Lambert C. Giant conductance oscillations in mesoscopic Andreev interferometers. Journal of Physics: Condensed Matter. 1996;8(26):L377-L384. doi: 10.1088/0953-8984/8/26/001

Author

Allsopp, N K ; Cañizares, J S ; Raimondi, R et al. / Giant conductance oscillations in mesoscopic Andreev interferometers. In: Journal of Physics: Condensed Matter. 1996 ; Vol. 8, No. 26. pp. L377-L384.

Bibtex

@article{2b201772e5f347379764e8ca20c41084,
title = "Giant conductance oscillations in mesoscopic Andreev interferometers",
abstract = "We analyse the electrical conductance G(phi) of a two-dimensional, phase-coherent structure in contact with two superconductors, which is known to be an oscillatory function of the phase difference phi between the superconductors. It is predicted that for a ballistic sample, the amplitude of oscillation will be enhanced by placing a normal barrier at the normal-superconducting interface, and that by tuning the strength of the barrier, it can be made orders of magnitude greater than values observed in recent experiments. Giant oscillations can also be obtained without a barrier, provided that a crucial sum rule is broken. This can be achieved by disorder-induced normal scattering. In the absence of zero-phase inter-channel scattering, the conductance possesses a zero-phase minimum and a maximum at phi = pi.",
author = "Allsopp, {N K} and Ca{\~n}izares, {J S} and R Raimondi and Colin Lambert",
year = "1996",
doi = "10.1088/0953-8984/8/26/001",
language = "English",
volume = "8",
pages = "L377--L384",
journal = "Journal of Physics: Condensed Matter",
issn = "0953-8984",
publisher = "IOP Publishing Ltd",
number = "26",

}

RIS

TY - JOUR

T1 - Giant conductance oscillations in mesoscopic Andreev interferometers

AU - Allsopp, N K

AU - Cañizares, J S

AU - Raimondi, R

AU - Lambert, Colin

PY - 1996

Y1 - 1996

N2 - We analyse the electrical conductance G(phi) of a two-dimensional, phase-coherent structure in contact with two superconductors, which is known to be an oscillatory function of the phase difference phi between the superconductors. It is predicted that for a ballistic sample, the amplitude of oscillation will be enhanced by placing a normal barrier at the normal-superconducting interface, and that by tuning the strength of the barrier, it can be made orders of magnitude greater than values observed in recent experiments. Giant oscillations can also be obtained without a barrier, provided that a crucial sum rule is broken. This can be achieved by disorder-induced normal scattering. In the absence of zero-phase inter-channel scattering, the conductance possesses a zero-phase minimum and a maximum at phi = pi.

AB - We analyse the electrical conductance G(phi) of a two-dimensional, phase-coherent structure in contact with two superconductors, which is known to be an oscillatory function of the phase difference phi between the superconductors. It is predicted that for a ballistic sample, the amplitude of oscillation will be enhanced by placing a normal barrier at the normal-superconducting interface, and that by tuning the strength of the barrier, it can be made orders of magnitude greater than values observed in recent experiments. Giant oscillations can also be obtained without a barrier, provided that a crucial sum rule is broken. This can be achieved by disorder-induced normal scattering. In the absence of zero-phase inter-channel scattering, the conductance possesses a zero-phase minimum and a maximum at phi = pi.

U2 - 10.1088/0953-8984/8/26/001

DO - 10.1088/0953-8984/8/26/001

M3 - Letter

VL - 8

SP - L377-L384

JO - Journal of Physics: Condensed Matter

JF - Journal of Physics: Condensed Matter

SN - 0953-8984

IS - 26

ER -