Superfluid to Bose-glass transition in a 1D weakly interacting Bose gas
arXiv:0904.3643 · doi:10.1103/PhysRevLett.103.030403
Abstract
We study the one-dimensional Bose gas in spatially correlated disorder at zero temperature, using an extended density-phase Bogoliubov method. We analyze in particular the decay of the one-body density matrix and the behaviour of the Bogoliubov excitations across the phase boundary. We observe that the transition to the Bose glass phase is marked by a power-law divergence of the density of states at low energy. A measure of the localization length displays a power-law energy dependence in both regions, with the exponent equal to -1 at the boundary. We draw the phase diagram of the superfluid-insulator transition in the limit of small interaction strength.
4 pages, 4 figures
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Cited by in corpus (11)
- Anderson localization in Bose-Einstein condensates
- Bogoliubov Excitations of Disordered Bose-Einstein Condensates
- Localization of Bogoliubov quasiparticles in interacting Bose gases with correlated disorder
- Polariton Condensation in a One-Dimensional Disordered Potential
- Correlation function of weakly interacting bosons in a disordered lattice
- Fragmentation and the Bose-glass phase transition of the disordered 1D Bose gas
- Ground-state and dynamic properties of hard-core bosons in one-dimensional incommensurate optical lattices with harmonic trap
- Superfluid-insulator transition of two-dimensional disordered Bose gases
- Quantum criticality in disordered bosonic optical lattices
- Quench-induced delocalization
- Reentrant transition of bosons in a quasiperiodic potential