Interaction Quench in the Hubbard model

dc.creatorMoeckel, M.
dc.creatorKehrein, S.
dc.date2008-02-21
dc.date2008-05-09
dc.date.accessioned2026-07-07T09:37:41Z
dc.date.available2026-07-07T09:37:41Z
dc.descriptionMotivated by recent experiments in ultracold atomic gases that explore the nonequilibrium dynamics of interacting quantum many-body systems, we investigate the opposite limit of Landau's Fermi liquid paradigm: We study a Hubbard model with a sudden interaction quench, that is the interaction is switched on at time t=0. Using the flow equation method, we are able to study the real time dynamics for weak interaction U in a systematic expansion and find three clearly separated time regimes: i) An initial buildup of correlations where the quasiparticles are formed. ii) An intermediate quasi-steady regime resembling a zero temperature Fermi liquid with a nonequilibrium quasiparticle distribution function. iii) The long time limit described by a quantum Boltzmann equation leading to thermalization with a temperature T proportional to U.
dc.descriptionFinal version as published
dc.identifierhttps://arxiv.org/abs/0802.3202
dc.identifierhttp://arxiv.org/abs/0802.3202
dc.identifierPhys. Rev. Lett. 100, 175702 (2008)
dc.identifierdoi:10.1103/PhysRevLett.100.175702
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/160544
dc.subjectStrongly Correlated Electrons
dc.titleInteraction Quench in the Hubbard model
dc.typetext

Files

Collections