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Nonequilibrium Dynamical Mean-Field Theory for Bosonic Lattice Models
Department of Physics, University of Fribourg, Fribourg, Switzerland.ORCID-id: 0000-0002-7263-4403
Max Planck Research Department for Structural Dynamics, University of Hamburg-CFEL, Hamburg, Germany.
Department of Physics, University of Fribourg, Fribourg, Switzerland.
2015 (engelsk)Inngår i: Physical Review X, E-ISSN 2160-3308, Vol. 5, nr 1, artikkel-id 011038Artikkel i tidsskrift (Fagfellevurdert) Published
Abstract [en]

We develop the nonequilibrium extension of bosonic dynamical mean-field theory and a Nambu real-time strong-coupling perturbative impurity solver. In contrast to Gutzwiller mean-field theory and strong-coupling perturbative approaches, nonequilibrium bosonic dynamical mean-field theory captures not only dynamical transitions but also damping and thermalization effects at finite temperature. We apply the formalism to quenches in the Bose-Hubbard model, starting from both the normal and the Bose-condensed phases. Depending on the parameter regime, one observes qualitatively different dynamical properties, such as rapid thermalization, trapping in metastable superfluid or normal states, as well as long-lived or strongly damped amplitude oscillations. We summarize our results in nonequilibrium “phase diagrams” that map out the different dynamical regimes.

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American Physical Society, 2015. Vol. 5, nr 1, artikkel-id 011038
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URN: urn:nbn:se:oru:diva-89997DOI: 10.1103/PhysRevX.5.011038ISI: 000352197800001Scopus ID: 2-s2.0-84926163472OAI: oai:DiVA.org:oru-89997DiVA, id: diva2:1531396
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Funding Agency:

FP7 ERC starting Grant 278023

Tilgjengelig fra: 2021-02-26 Laget: 2021-02-26 Sist oppdatert: 2024-01-17bibliografisk kontrollert

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