Anomalous quantum glass of bosons in a random potential in two dimensions
arXiv:1110.3213 · doi:10.1103/PhysRevLett.114.105303
Abstract
We present a quantum Monte Carlo study of the "quantum glass" phase of the 2D Bose-Hubbard model with random potentials at filling . In the narrow region between the Mott and superfluid phases the compressibility has the form with and vanishing or very small. Thus, at the system is either incompressible (a Mott glass) or nearly incompressible (a Mott-glass-like anomalous Bose glass). At stronger disorder, where a glass reappears from the superfluid, we find a conventional highly compressible Bose glass. On a path connecting these states, away from the superfluid at larger Hubbard repulsion, a change of the disorder strength by only changes the low-temperature compressibility by more than four orders of magnitude, lending support to two types of glass states separated by a phase transition or a sharp cross-over.
Published version including supplementary material, 11 pages total, 15 figures
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Cited by in corpus (12)
- Random-Singlet Phase in Disordered Two-Dimensional Quantum Magnets
- A correlated Anderson insulator on the honeycomb lattice
- Quantum critical behavior of the superfluid-Mott glass transition
- Quantum Critical Scaling of Dirty Bosons in Two Dimensions
- Directed-Loop Quantum Monte Carlo Method for Retarded Interactions
- Measuring the Edwards-Anderson order parameter of the Bose glass: a quantum gas microscope approach
- Bose and Mott Glass Phases in Dimerized Quantum Antiferromagnets
- Local Density of the Bose Glass Phase
- Quantum crystallography of Rydberg-dressed Bose gases on a square lattice
- Quantum transition between magnetically ordered and Mott glass phases
- Phase diagram of disordered Bose-Hubbard model based on mean-field and percolation analysis in two dimensions and at fixed filling
- Mott glass phase in a diluted bilayer Heisenberg quantum antiferromagnet