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Interaction Quench in the Hubbard Model

2008/02/29 by Michael Moeckel, M. Moeckel, Stefan Kehrein +1 · 29 citations
Physics and Astronomy · #Boltzmann equation #Cold Atom Physics and Bose-Einstein Condensates #Condensed matter physics #Distribution function #Fermi Gamma-ray Space Telescope #Fermi liquid theory #Hubbard model #Momentum (technical analysis) #Non-equilibrium thermodynamics #Opinion Dynamics and Social Influence #Physics #Quantum #Quantum electrodynamics #Quantum many-body systems #Quantum mechanics #Quasiparticle #Thermalisation #cond-mat.str-el

paper · pdf · doi:10.1103/physrevlett.100.175702

published as Phys. Rev. Lett. 100, 175702 (2008) · Final version as published

openalex publication_date 2008/05/02 · arxiv created 2008/05/09 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

Motivated 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 of the momentum distribution function with a temperature T proportional, variantU.

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