Andreev billiards
| dc.creator | Beenakker, C. W. J. | |
| dc.date | 2004-06-01 | |
| dc.date | 2004-07-09 | |
| dc.date.accessioned | 2026-07-25T15:36:07Z | |
| dc.description | This is a review of recent advances in our understanding of how Andreev reflection at a superconductor modifies the excitation spectrum of a quantum dot. The emphasis is on two-dimensional impurity-free structures in which the classical dynamics is chaotic. Such Andreev billiards differ in a fundamental way from their non-superconducting counterparts. Most notably, the difference between chaotic and integrable classical dynamics shows up already in the level density, instead of only in the level--level correlations. A chaotic billiard has a gap in the spectrum around the Fermi energy, while integrable billiards have a linearly vanishing density of states. The excitation gap E_gap corresponds to a time scale h/E_gap which is classical (h-independent, equal to the mean time t_dwell between Andreev reflections) if t_dwell is sufficiently large. There is a competing quantum time scale, the Ehrenfest time t_E, which depends logarithmically on h. Two phenomenological theories provide a consistent description of the t_E-dependence of the gap, given qualitatively by E_gap min(h/t_dwell,h/t_E). The analytical predictions have been tested by computer simulations but not yet experimentally. | |
| dc.description | 22 pages including 24 figures; [v2] new sections III, VI.C; [v3] major revision of section VIII.B, correcting the effective RMT of cond-mat/0208192 | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0406018 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0406018 | |
| dc.identifier | Lect. Notes Phys. 667, 131 (2005) | |
| dc.identifier | doi:10.1007/11358817_4 | |
| dc.identifier.uri | https://dspace.dare.co.zw/handle/123456789/35282 | |
| dc.subject | Mesoscale and Nanoscale Physics | |
| dc.title | Andreev billiards | |
| dc.type | text |