{ "id": "1211.4465", "version": "v2", "published": "2012-11-19T15:38:05.000Z", "updated": "2013-02-21T10:46:52.000Z", "title": "Relaxation and Thermalization after a Quantum Quench: Why Localization is Important", "authors": [ "Simone Ziraldo", "Giuseppe E. Santoro" ], "comment": "14 pages, 6 figures", "journal": "Phys. Rev. B 87, 064201 (2013)", "doi": "10.1103/PhysRevB.87.064201", "categories": [ "cond-mat.dis-nn", "cond-mat.stat-mech" ], "abstract": "We study the unitary dynamics and the thermalization properties of free-fermion-like Hamiltonians after a sudden quantum quench, extending the results of S. Ziraldo et al. [Phys. Rev. Lett. 109, 247205 (2012)]. With analytical and numerical arguments, we show that the existence of a stationary state and its description with a generalized Gibbs ensemble (GGE) depend crucially on the observable considered (local versus extensive) and on the localization properties of the final Hamiltonian. We present results on two one-dimensional (1D) models, the disordered 1D fermionic chain with long-range hopping and the disordered Ising/XY spin chain. We analytically prove that, while time averages of one-body operators are perfectly reproduced by GGE (even for finite-size systems, if time integrals are extended beyond revivals), time averages of many-body operators might show clear deviations from the GGE prediction when disorder-induced localization of the eigenstates is at play.", "revisions": [ { "version": "v2", "updated": "2013-02-21T10:46:52.000Z" } ], "analyses": { "subjects": [ "05.70.Ln", "75.10.Pq", "72.15.Rn", "02.30.Ik" ], "keywords": [ "localization", "relaxation", "time averages", "sudden quantum quench", "disordered 1d fermionic chain" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review B", "year": 2013, "month": "Feb", "volume": 87, "number": 6, "pages": "064201" }, "note": { "typesetting": "TeX", "pages": 14, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2013PhRvB..87f4201Z" } } }