{ "id": "cond-mat/0310429", "version": "v1", "published": "2003-10-17T18:52:28.000Z", "updated": "2003-10-17T18:52:28.000Z", "title": "The Ehrenfest Oscillations in The Level Statistics of Chaotic Quantum Dots", "authors": [ "Chushun Tian", "Anatoly I. Larkin" ], "comment": "20 pages, 4 figures, submitted to Phys. Rev. B", "doi": "10.1103/PhysRevB.70.035305", "categories": [ "cond-mat.mes-hall" ], "abstract": "We study a crossover from classical to quantum picture in the electron energy statistics in a system with broken time-reversal symmetry. The perturbative and nonperturbative parts of the two level correlation function, $R(\\omega)$ are analyzed. We find that in the intermediate region, $\\Delta\\ll\\omega\\sim t_E^{-1}\\ll t_{erg}^{-1}$, where $t_E$ and $t_{erg}$ are the Ehrenfest and ergodic times, respectively, $R(\\omega)$ consists of a series of oscillations with the periods depending on $t_E$, deviating from the universal Wigner-Dyson statistics. These Ehrenfest oscillations have the period dependence as $t_E^{-1}$ in the perturbative part. [For systems with time-reversal symmetry, this oscillation in the perturbative part of $R(\\omega)$ was studied in an earlier work (I. L. Aleiner and A. I. Larkin, Phys. Rev. E {\\bf 55}, R1243 (1997))]. In the nonperturbative part they have the period dependence as $(\\Delta^{-1}+\\alpha t_E)^{-1}$ with $\\alpha$ a universal numerical factor. The amplitude of the leading order Ehrenfest oscillation in the nonperturbative part is larger than that of the perturbative part.", "revisions": [ { "version": "v1", "updated": "2003-10-17T18:52:28.000Z" } ], "analyses": { "keywords": [ "chaotic quantum dots", "level statistics", "nonperturbative part", "period dependence", "level correlation function" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. B" }, "note": { "typesetting": "TeX", "pages": 20, "language": "en", "license": "arXiv", "status": "editable" } } }