2012/11/30 by Maurizio Fagotti · 1 citation
Physics and Astronomy · #Advanced Thermodynamics and Statistical Mechanics #Physics of Superconductivity and Magnetism #Quantum many-body systems #cond-mat.stat-mech #quant-ph
paper · pdf · doi:10.1103/physrevb.87.165106
published as Phys. Rev. B 87, 165106 (2013) · 12 pages, 2 figures; V2: minor changes and reference added
arxiv created 2012/12/10 · openalex publication_date 2013/04/04 · arxiv updated 2013/04/05 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28
We consider the time evolution after sudden quenches of global parameters in translational invariant Hamiltonians and study the time average expectation values and entanglement entropies in finite chains. We show that in noninteracting models the time average of spin correlation functions is asymptotically equal to the infinite time limit in the infinite chain, which is known to be described by a generalized Gibbs ensemble. The equivalence breaks down considering nonlocal operators, and we establish that this can be traced back to the existence of conservation laws common to the Hamiltonian before and after the quench. We develop a method to compute the leading finite-size corrections. We find that the finite-size corrections are generally large in observables with large relaxation timescales.