Non-Gibbs states on a Bose-Hubbard lattice
arXiv:1809.05371 · doi:10.1103/PhysRevA.99.023603
Abstract
We study the equilibrium properties of the repulsive quantum Bose-Hubbard model at high temperatures in arbitrary dimensions, with and without disorder. In its microcanonical setting the model conserves energy and particle number. The microcanonical dynamics is characterized by a pair of two densities: energy density and particle number density . The macrocanonical Gibbs distribution also depends on two parameters: the inverse nonnegative temperature and the chemical potential . We prove the existence of non-Gibbs states, that is, pairs which cannot be mapped onto . The separation line in the density control parameter space between Gibbs and non-Gibbs states corresponds to infinite temperature . The non-Gibbs phase cannot be cured into a Gibbs one within the standard Gibbs formalism using negative temperatures.
8 pages, 1 figure, misprints corrected
References in corpus (4)
Cited by in corpus (11)
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- Dynamical freezing of relaxation to equilibrium
- Localization transition in the Discrete Non-Linear Schrödinger Equation: ensembles inequivalence and negative temperatures
- Condensation transition and ensemble inequivalence in the Discrete Nonlinear Schrödinger Equation
- Fragile Many Body Ergodicity
- Density Resolved Wave Packet Spreading in Disordered Gross-Pitaevskii Lattices
- Localization in the Discrete Non-Linear Schrödinger Equation and geometric properties of the microcanonical surface
- Equivalence of ensembles, condensation and glassy dynamics in the Bose-Hubbard Hamiltonian
- Quench dynamics in disordered two-dimensional Gross-Pitaevskii Lattices
- Thermal lifetime of breathers
- Transient ordering in the Gross-Pitaevskii lattice subject to an energy quench within the disordered phase