2013/05/30 by Márton Kormos, Marton Kormos, Aditya Shashi +4 · 142 citations
Mathematics · Physics and Astronomy · #Bethe ansatz #Bose gas #Bose–Einstein condensate #Canonical ensemble #Cold Atom Physics and Bose-Einstein Condensates #Conserved quantity #Integrable system #Mathematical physics #Mathematics #Non-equilibrium thermodynamics #Physics #Quadratic equation #Quantum #Quantum many-body systems #Quantum mechanics #Quantum, superfluid, helium dynamics #Statistical physics #Thermalisation #cond-mat.quant-gas #cond-mat.stat-mech #hep-th
paper · pdf · doi:10.1103/physrevb.88.205131
published in Physical Review B 88(20) (American Physical Society) · Supersedes arXiv:1204.3889. 4+ pages + Supplementary Material
arxiv created 2013/05/30 · openalex publication_date 2013/11/22 · arxiv updated 2013/11/27 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
The nonequilibrium dynamics of integrable systems are highly constrained by the conservation of certain charges. There is substantial evidence that after a quantum quench they do not thermalize but their asymptotic steady state can be described by a generalized Gibbs ensemble (GGE) built from the conserved charges. Most of the studies on the GGE so far have focused on models that can be mapped to quadratic systems, while analytic treatment in nonquadratic systems remained elusive. We obtain results on interaction quenches in a nonquadratic continuum system, the one-dimensional (1D) Bose gas described by the integrable Lieb-Liniger model. The direct implementation of the GGE prescription is prohibited by the divergence of the conserved charges, which we conjecture to be endemic to any continuum integrable systems with contact interactions undergoing a sudden quench. We compute local correlators for a noninteracting initial state and arbitrary final interactions as well as two-point functions for quenches to the Tonks-Girardeau regime. We show that in the long time limit integrability leads to significant deviations from the predictions of the grand canonical ensemble, allowing for an experimental verification in cold-atom systems.