Superfluid-insulator transition of two-dimensional disordered Bose gases
arXiv:1408.5022 · doi:10.1103/PhysRevA.90.031603
Abstract
We study the two-dimensional weakly repulsive Bose gas at zero temperature in the presence of correlated disorder. Using large-scale simulations, we show that the low-energy Bogoliubov cumulative density of states remains quadratic up to a critical disorder strength, beyond which a power law with disorder-dependent exponent sets in. We associate this threshold behavior with the transition from superfluid to Bose glass, and compare the resulting mean-field phase diagram with scaling laws and the Thomas-Fermi percolation threshold of the mean-field density profile.
Published version, 5 pages, 4 figures
References in corpus (13)
- Anderson Transitions
- The Kernel Polynomial Method
- Extension of Bogoliubov theory to quasi-condensates
- Ultracold Bose Gases in 1D Disorder: From Lifshits Glass to Bose-Einstein Condensate
- Bogoliubov Excitations of Disordered Bose-Einstein Condensates
- Phase transition of interacting disordered bosons in one dimension
- The insulating phases and superfluid-insulator transition of disordered boson chains
- Polariton Condensation in a One-Dimensional Disordered Potential
- Superfluid to Bose-glass transition in a 1D weakly interacting Bose gas
- Dirty Bosons: Twenty Years Later
- Excitations of the One Dimensional Bose-Einstein Condensates in a Random Potential
- Correlation function of weakly interacting bosons in a disordered lattice
- Disordered bosons in one dimension: from weak to strong randomness criticality