Strong-coupling perturbation theory for the two-dimensional Bose-Hubbard model in a magnetic field

M. Niemeyer, J. K. Freericks, and H. Monien
Phys. Rev. B 60, 2357 – Published 15 July 1999
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Abstract

The Bose-Hubbard model in an external magnetic field is investigated with strong-coupling perturbation theory. The lowest-order secular equation leads to the problem of a charged particle moving on a lattice in the presence of a magnetic field, which was first treated by Hofstadter. We present phase diagrams for the two-dimensional square and triangular lattices, showing a change in shape of the phase lobes away from the well-known power-law behavior in zero magnetic field. Some qualitative agreement with experimental work on Josephson-junction arrays is found for the insulating phase behavior at small fields.

  • Received 15 December 1998

DOI:https://doi.org/10.1103/PhysRevB.60.2357

©1999 American Physical Society

Authors & Affiliations

M. Niemeyer

  • Physikalisches Institut der Univerität Bonn, Nußallee 12, D-53115 Bonn, Germany

J. K. Freericks

  • Department of Physics, Georgetown University, Washington, D.C. 20057

H. Monien

  • Physikalisches Institut der Univerität Bonn, Nußallee 12, D-53115 Bonn, Germany

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Vol. 60, Iss. 4 — 15 July 1999

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