Thermal and quantum fluctuations of confined Bose-Einstein condensate beyond the Bogoliubov approximation
arXiv:1604.05900 · doi:10.1016/j.aop.2016.12.020
Abstract
The formulation for zero mode of a Bose-Einstein condensate beyond the Bogoliubov approximation at zero temperature [Y.Nakamura et al., Phys. Rev. A 89, 013613 (2014)] is extended to finite temperature. Both thermal and quantum fluctuations are considered in a manner consistent with a concept of spontaneous symmetry breakdown for a finite-size system. Therefore, we need a proper treatment of the zero mode operators, which invoke non-trivial enhancements in depletion condensate and thermodynamical quantities such as the specific heat. The enhancements are visible in the weak interaction case. Our approach reproduces the results of a homogeneous system in the Bogoliubov approximation in a large particle number limit.
arXiv comment18 pages, 6 figures
References in corpus (7)
- Conserving and Gapless Approximations for an Inhomogeneous Bose Gas at Finite Temperatures
- Quantum Monte Carlo Calculations for a large number of bosons in a harmonic trap
- The critical temperature of a trapped, weakly interacting Bose gas
- Precision Monte Carlo Test of the Hartree-Fock Approximation for a trapped Bose Gas
- Formulation for zero mode of Bose-Einstein condensate beyond Bogoliubov approximation
- Conserving Gapless Mean-Field Theory for Bose-Einstein Condensates
- Effective field theory of Bose-Einstein condensation of clusters and Nambu-Goldstone-Higgs states in C
Cited by in corpus (3)
- Bose polaron in spherical trap potentials: Spatial structure and quantum depletion
- Bose polaron in spherically symmetric trap potentials: Ground states with zero and lower angular momenta
- Self-Energy Renormalization for Inhomogeneous Nonequilibrium Systems and Field Expansion via Complete Set of Time-Dependent Wave Functions