Andreev levels in a single-channel conductor
| dc.creator | Titov, M. | |
| dc.creator | Mortensen, N. A. | |
| dc.creator | Schomerus, H. | |
| dc.creator | Beenakker, C. W. J. | |
| dc.date | 2001-03-21 | |
| dc.date | 2001-03-23 | |
| dc.date.accessioned | 2026-07-07T02:40:48Z | |
| dc.date.available | 2026-07-07T02:40:48Z | |
| dc.description | We calculate the subgap density of states of a disordered single-channel normal metal connected to a superconductor at one end (NS junction) or at both ends (SNS junction). The probability distribution of the energy of a bound state (Andreev level) is broadened by disorder. In the SNS case the two-fold degeneracy of the Andreev levels is removed by disorder leading to a splitting in addition to the broadening. The distribution of the splitting is given precisely by Wigner's surmise from random-matrix theory. For strong disorder the mean density of states is largely unaffected by the proximity to the superconductor, because of localization, except in a narrow energy region near the Fermi level, where the density of states is suppressed with a log-normal tail. | |
| dc.description | 12 pages, 5 figures | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0103445 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0103445 | |
| dc.identifier | Phys. Rev. B 64, 134206 (2001) | |
| dc.identifier | doi:10.1103/PhysRevB.64.134206 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/17509 | |
| dc.subject | Mesoscale and Nanoscale Physics | |
| dc.subject | Disordered Systems and Neural Networks | |
| dc.title | Andreev levels in a single-channel conductor | |
| dc.type | text |