Bosonization and entanglement spectrum for one-dimensional polar bosons on disordered lattices

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autorschaft

  • Xiaolong Deng
  • Roberta Citro
  • Edmond Orignac
  • Anna Minguzzi
  • Luis Santos

Organisationseinheiten

Externe Organisationen

  • Universita di Salerno
  • École normale supérieure de Lyon (ENS de Lyon)
  • Université Grenoble Alpes (UGA)
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Details

OriginalspracheEnglisch
Aufsatznummer045023
FachzeitschriftNew Journal of Physics
Jahrgang15
PublikationsstatusVeröffentlicht - Apr. 2013

Abstract

Ultra cold polar bosons in a disordered lattice potential, described by the extended Bose-Hubbard model, display a rich phase diagram. In the case of uniform random disorder one finds two insulating quantum phases - the Mott-insulator and the Haldane insulator - in addition to a superfluid and a Bose glass phase. In the case of a quasiperiodic potential, further phases are found, e.g. the incommensurate density wave, adiabatically connected to the Haldane insulator. For the case of weak random disorder we determine the phase boundaries using a perturbative bosonization approach. We then calculate the entanglement spectrum for both types of disorder, showing that it provides a good indication of the various phases.

ASJC Scopus Sachgebiete

Zitieren

Bosonization and entanglement spectrum for one-dimensional polar bosons on disordered lattices. / Deng, Xiaolong; Citro, Roberta; Orignac, Edmond et al.
in: New Journal of Physics, Jahrgang 15, 045023, 04.2013.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Deng X, Citro R, Orignac E, Minguzzi A, Santos L. Bosonization and entanglement spectrum for one-dimensional polar bosons on disordered lattices. New Journal of Physics. 2013 Apr;15:045023. doi: 10.1088/1367-2630/15/4/045023
Deng, Xiaolong ; Citro, Roberta ; Orignac, Edmond et al. / Bosonization and entanglement spectrum for one-dimensional polar bosons on disordered lattices. in: New Journal of Physics. 2013 ; Jahrgang 15.
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