Re-examining the quadratic approximation in theory of a weakly interacting Bose gas with condensate: the role of nonlocal interaction potentials
Autor: | Yu. V. Slyusarenko, A. S. Peletminskii, Andrii Sotnikov, M. S. Bulakhov, S. V. Peletminskii |
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Rok vydání: | 2018 |
Předmět: |
Physics
Statistical Mechanics (cond-mat.stat-mech) Bose gas Spectrum (functional analysis) FOS: Physical sciences Position and momentum space Condensed Matter Physics 01 natural sciences Atomic and Molecular Physics and Optics 010305 fluids & plasmas Thermodynamic potential symbols.namesake Quadratic equation Quantum Gases (cond-mat.quant-gas) Ultracold atom Quantum mechanics 0103 physical sciences symbols Condensed Matter - Quantum Gases 010306 general physics Hamiltonian (quantum mechanics) Condensed Matter - Statistical Mechanics Order of magnitude |
Zdroj: | Journal of Physics B: Atomic, Molecular and Optical Physics |
ISSN: | 0953-4075 0368-3400 0038-5646 1054-660X 0132-6414 1063-7796 0367-2026 1742-6596 1751-8113 |
DOI: | 10.1088/1361-6455/aae061 |
Popis: | We derive and analyze the coupled equations of quadratic approximation of the Bogoliubov model for a weakly interacting Bose gas. The first equation determines the condensate density as a variational parameter and ensures the minimum of the grand thermodynamic potential. The second one provides a relation between the total number of particles and chemical potential. Their consistent theoretical analysis is performed for a number of model interaction potentials including contact (local) and nonlocal interactions, where the latter provide nontrivial dependencies in momentum space. We demonstrate that the derived equations have no solutions for the local potential, although they formally reproduce the well-known results of the Bogoliubov approach. At the same time, it is shown that these equations have the solutions for physically relevant nonlocal potentials. We show that in the regimes close to experimental realizations with ultracold atoms, the contribution of the terms originating from the quadratic part of the truncated Hamiltonian to the chemical potential can be of the same order of magnitude as from its $c$-number part. Due to this fact, in particular, the spectrum of single-particle excitations in the quadratic approximation acquires a gap. The issue of the gap is also discussed. 22 pages, 5 figures |
Databáze: | OpenAIRE |
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