Abstract
We consider the Bose-Hubbard model in a two-dimensional rotating optical lattice and investigate the consequences of the effective magnetic field created by rotation. Using a Gutzwiller-type variational wave function, we find an analytical expression for the Mott insulator (MI)-superfluid (SF) transition boundary in terms of the maximum eigenvalue of the Hofstadter butterfly. The dependence of phase boundary on the effective magnetic field is complex, reflecting the self-similar properties of the single particle energy spectrum. Finally, we argue that fractional quantum Hall phases exist close to the MI-SF transition boundaries, including MI states with particle densities greater than one. © 2007 The American Physical Society.
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CITATION STYLE
Umucalilar, R. O., & Oktel, M. Ö. (2007). Phase boundary of the boson Mott insulator in a rotating optical lattice. Physical Review A - Atomic, Molecular, and Optical Physics, 76(5). https://doi.org/10.1103/PhysRevA.76.055601
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