Nonequilibrium States of a Quenched Bose Gas
arXiv:1401.2390 · doi:10.1103/PhysRevA.90.063626
Abstract
Yin and Radzihovsky [1] recently developed a self-consistent extension of a Bogoliubov theory, in which the condensate number density is treated as a mean field that changes with time, in order to analyze a JILA experiment by Makotyn et al. [2] on a Rb Bose gas following a deep quench to a large scattering length. We apply this theory to construct a closed set of equations that highlight the role of , which is to induce an effective interaction between quasiparticles. We show analytically that such a system supports a steady state characterized by a constant condensate density and a steady but periodically changing momentum distribution, whose time average is described exactly by the generalized Gibbs ensemble. We discuss how the -induced effective interaction, which cannot be ignored on the grounds of the adiabatic approximation for modes near the gapless Goldstone mode, can significantly affect condensate populations and Tan's contact for a Bose gas that has undergone a deep quench.
12 pages, 6 figures; v2: significantly expanded
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- Dynamical excitation of maxon and roton modes in a Rydberg-Dressed Bose-Einstein Condensate
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- Early-time dynamics of Bose gases quenched into the strongly interacting regime
- Long-lived universal resonant Bose gases
- High Temperature Virial Expansion to Universal Quench Dynamics
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- Topological study of a Bogoliubov-de Gennes system of pseudo spin- bosons with conserved magnetization in a honeycomb lattice
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