Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versa

In this paper, we study the nonequilibrium dynamics of the Bose–Hubbard model with the nearest-neighbor repulsion by using time-dependent Gutzwiller (GW) methods. In particular, we vary the hopping parameters in the Hamiltonian as a function of time, and investigate the dynamics of the system from t...

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Main Authors: Keita Shimizu, Takahiro Hirano, Jonghoon Park, Yoshihito Kuno, Ikuo Ichinose
Format: Article
Language:English
Published: IOP Publishing 2018-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/aad5f9
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author Keita Shimizu
Takahiro Hirano
Jonghoon Park
Yoshihito Kuno
Ikuo Ichinose
author_facet Keita Shimizu
Takahiro Hirano
Jonghoon Park
Yoshihito Kuno
Ikuo Ichinose
author_sort Keita Shimizu
collection DOAJ
description In this paper, we study the nonequilibrium dynamics of the Bose–Hubbard model with the nearest-neighbor repulsion by using time-dependent Gutzwiller (GW) methods. In particular, we vary the hopping parameters in the Hamiltonian as a function of time, and investigate the dynamics of the system from the density wave (DW) to the superfluid (SF) crossing a first-order phase transition and vice versa. From the DW to SF, we find scaling laws for the correlation length and vortex density with respect to the quench time. This is a reminiscence of the Kibble–Zurek scaling for continuous phase transitions and contradicts the common expectation. We give a possible explanation for this observation. On the other hand from SF to DW, the system evolution depends on the initial SF state. When the initial state is the ground state obtained by the static GW methods, a coexisting state of the SF and DW domains forms after passing through the critical point. Coherence of the SF order parameter is lost as the system evolves. This is a phenomenon similar to the glass transition in classical systems. When the state starts from the SF with small local phase fluctuations, the system obtains a large size DW domain structure with thin domain walls.
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spelling doaj.art-ecbe9144e4ed408d9da24856c881ec942023-08-08T14:53:29ZengIOP PublishingNew Journal of Physics1367-26302018-01-0120808300610.1088/1367-2630/aad5f9Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versaKeita Shimizu0Takahiro Hirano1Jonghoon Park2Yoshihito Kuno3Ikuo Ichinose4Department of Applied Physics, Nagoya Institute of Technology , Nagoya 466-8555, JapanDepartment of Applied Physics, Nagoya Institute of Technology , Nagoya 466-8555, JapanDepartment of Applied Physics, Nagoya Institute of Technology , Nagoya 466-8555, JapanDepartment of Physics, Graduate School of Science, Kyoto University , Kyoto 606-8502, JapanDepartment of Applied Physics, Nagoya Institute of Technology , Nagoya 466-8555, JapanIn this paper, we study the nonequilibrium dynamics of the Bose–Hubbard model with the nearest-neighbor repulsion by using time-dependent Gutzwiller (GW) methods. In particular, we vary the hopping parameters in the Hamiltonian as a function of time, and investigate the dynamics of the system from the density wave (DW) to the superfluid (SF) crossing a first-order phase transition and vice versa. From the DW to SF, we find scaling laws for the correlation length and vortex density with respect to the quench time. This is a reminiscence of the Kibble–Zurek scaling for continuous phase transitions and contradicts the common expectation. We give a possible explanation for this observation. On the other hand from SF to DW, the system evolution depends on the initial SF state. When the initial state is the ground state obtained by the static GW methods, a coexisting state of the SF and DW domains forms after passing through the critical point. Coherence of the SF order parameter is lost as the system evolves. This is a phenomenon similar to the glass transition in classical systems. When the state starts from the SF with small local phase fluctuations, the system obtains a large size DW domain structure with thin domain walls.https://doi.org/10.1088/1367-2630/aad5f9ultra-cold atomic gasesBose–Hubburd modelquantum dynamical phase transitionfirst-order phase transitionsuperfluiddensity wave
spellingShingle Keita Shimizu
Takahiro Hirano
Jonghoon Park
Yoshihito Kuno
Ikuo Ichinose
Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versa
New Journal of Physics
ultra-cold atomic gases
Bose–Hubburd model
quantum dynamical phase transition
first-order phase transition
superfluid
density wave
title Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versa
title_full Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versa
title_fullStr Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versa
title_full_unstemmed Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versa
title_short Dynamics of first-order quantum phase transitions in extended Bose–Hubbard model: from density wave to superfluid and vice versa
title_sort dynamics of first order quantum phase transitions in extended bose hubbard model from density wave to superfluid and vice versa
topic ultra-cold atomic gases
Bose–Hubburd model
quantum dynamical phase transition
first-order phase transition
superfluid
density wave
url https://doi.org/10.1088/1367-2630/aad5f9
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