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Quantum states of ultracold Bose gases in 1D random potentials

Pierre Lugan, David Clément, Philippe Bouyer, Alain Aspect, Maciej Lewenstein, Laurent Sanchez-Palencia

Published Mar 1, 2010• 0 citations
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Finite temperature correlations in the Bose-Hubbard model: application of the Gauge $P$ representation

Saeed Ghanbari, Joel Frederick Corney, Tien D. Kieu

We study ultracold Bose gases in periodic potentials as described by the Bose-Hubbard model. In 1D and at finite temperature, we simulate ultracold Bose gases in imaginary time with the gauge $P$ representation. We study various quantities including the Luttinger parameter $K$, which is important for locating the boundaries of the Mott insulator lobes, and find a simple relation for the kinetic energy part of the Bose-Hubbard Hamiltonian. We show that for J=0, the stepwise pattern of the average number of particles per lattice site versus the chemical potential vanishes at temperatures above $T \approx 0.1 U$. Also, at chemical potential $μ=0.5 U$ and temperature $T=0.5 U$ by increasing $J$, the relative value of the number fluctuation decreases and approaches that of a coherent state.

arXiv:1002.4735•Feb 25, 2010•1 citation
Finite temperature correlations in the Bose-Hubbard model: application of the Gauge PPP representation
We study ultracold Bose gases in periodic potentials as described by the Bose-Hubbard model. In 1D and at finite temperature, we simulate ultracold Bose gases in imaginary time with the gauge PPP representation. We study various quantities including the Luttinger parameter KKK, which is important for locating the boundaries of the Mott insulator lobes, and find a simple relation for the kinetic energy part of the Bose-Hubbard Hamiltonian. We show that for J=0, the stepwise pattern of the average number of particles per lattice site versus the chemical potential vanishes at temperatures above T≈0.1UT \approx 0.1 UT≈0.1U. Also, at chemical potential μ=0.5Uμ=0.5 Uμ=0.5U and temperature T=0.5UT=0.5 UT=0.5U by increasing JJJ, the relative value of the number fluctuation decreases and approaches that of a coherent state.