1996
DOI: 10.1209/epl/i1996-00522-9
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Induced superconductivity distinguishes chaotic from integrable billiards

Abstract: Random-matrix theory is used to show that the proximity to a superconductor opens a gap in the excitation spectrum of an electron gas confined to a billiard with a chaotic classical dynamics. In contrast, a gapless spectrum is obtained for a non-chaotic rectangular billiard, and it is argued that this is generic for integrable systems. preprint: cond-mat/9604058

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Cited by 117 publications
(297 citation statements)
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“…However, this is true only for such a simple geometry. For samples of more complicated shapes the behavior of the DOS ν(ǫ) depends on whether the electron dynamics in the N region is chaotic or integrable Lodder and Yu.V.Nazarov, 1998;Melsen et al, 1996;Pilgram et al, 2000;Taras-Semchuk and Altland, 2001).…”
Section: A Superconductor-normal Metal Structuresmentioning
confidence: 99%
“…However, this is true only for such a simple geometry. For samples of more complicated shapes the behavior of the DOS ν(ǫ) depends on whether the electron dynamics in the N region is chaotic or integrable Lodder and Yu.V.Nazarov, 1998;Melsen et al, 1996;Pilgram et al, 2000;Taras-Semchuk and Altland, 2001).…”
Section: A Superconductor-normal Metal Structuresmentioning
confidence: 99%
“…The main signatures of classical integrability ͑or lack of it͒ on the statistics of energy levels and properties of the transport coefficients for closed and open systems, respectively, have been discussed in detail in various reviews. [1][2][3][4] Discussions on modifications owing to the possibility of Andreev reflection appear in more recent studies, 5,6,[9][10][11][12][13][14][15] mostly focusing on the features of the quantum mechanical level density.…”
Section: Introductionmentioning
confidence: 99%
“…Over the last decade, the Bohr-Sommerfeld approximation for the smoothed density of states has been successfully applied to Andreev billiards. 15,16,17,18,19,20,21,22,24,26,27,28 In the case of a normal dot confined by one N-S interface and infinitely high potential walls, the integrated density of states or smoothed state counting function in the BS approximation reads…”
mentioning
confidence: 99%