1998
DOI: 10.1063/1.55281
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Methods of quasiclassical Green’s functions in the theory of transport phenomena in superconducting mesoscopic structures

Abstract: A short introduction to the theory of matrix quasiclassical Green's functions is given and possible applications of this theory to transport properties of mesoscopic superconducting-normal metal (S/N) structures are considered. We discuss a simplified version of these equations in the diffusive regime and in the case of a weak proximity effect. These equations are used for the calculation of the conductance of different S/N structures and for analysis of kinetic phenomena in these structures. We discuss the su… Show more

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Cited by 9 publications
(19 citation statements)
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References 26 publications
(56 reference statements)
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“…This non-monotonic behaviour has been observed both in very short S/N contacts [9] and in longer mesoscopic S/N structures [10][11][12]21]. In ref [6] it was noted that the conductance δG = G − G n consists of two contributions. The first, δG DOS , is negative due to a proximity effect induced decrease in the density of states (DOS) of the normal wire which makes contact with a superconducting strip [13].…”
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confidence: 99%
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“…This non-monotonic behaviour has been observed both in very short S/N contacts [9] and in longer mesoscopic S/N structures [10][11][12]21]. In ref [6] it was noted that the conductance δG = G − G n consists of two contributions. The first, δG DOS , is negative due to a proximity effect induced decrease in the density of states (DOS) of the normal wire which makes contact with a superconducting strip [13].…”
mentioning
confidence: 99%
“…In this case Nazarov and Stoof [4] (also see [5][6][7]) argued that the temperature dependence of the conductance G has a similar non-monotonic behaviour with a maximum at a temperature comparable with the Thouless energy, while simultaniously Volkov, Allsopp and Lambert [8] predicted that the voltage dependence of the conductance in an S/N mesoscopic structure (Andreev interferometer) has a similar form with a maximum at eV m ≈ ǫ T h . This non-monotonic behaviour has been observed both in very short S/N contacts [9] and in longer mesoscopic S/N structures [10][11][12]21].…”
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“…Thus, quantum ballistic electron propagation dominates in small-scale Sc systems. The interplay between phase-coherent electron propagation in Sc and macroscopic phase coherence in S gives rise to interesting new physics [6][7][8][9].…”
Section: Introductionmentioning
confidence: 99%