Second sound in 2D Bose gas: from the weakly interacting to the strongly interacting regime
arXiv:1712.05022 · doi:10.1103/PhysRevA.97.033604
Abstract
Using Landau's theory of two-fluid hydrodynamics, we investigate first and second sound propagating in a two-dimensional Bose gas. We study the temperature and interaction dependence of both sound modes and show that their behaviour exhibits a deep qualitative change as the gas evolves from the weakly interacting to the strongly interacting regime. Special emphasis is given to the jump of both sounds at the Berezinskii-Kosterlitz-Thouless transition, caused by the discontinuity of the superfluid density. We find that the excitation of second sound through a density perturbation becomes weaker and weaker as the interaction strength increases as a consequence of the decrease of the thermal expansion coefficient. Our results can be relevant for future experiments on the propagation of sound in the BEC side of the BCS-BEC crossover of a 2D superfluid Fermi gas.
14 pages, 6 figures
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- Low-energy collective oscillations and Bogoliubov sound in an exciton-polariton condensate
- Collisionless Dynamics in Two-Dimensional Bosonic Gases
- Signatures of a universal jump in the superfluid density in two-dimensional Bose gas with finite number of particles
- Sound propagation in a two-dimensional Bose gas across the superfluid transition
- Propagation of first and second sound in a two-dimensional Fermi superfluid
- Observation of Algebraic Time Order for Two-Dimensional Dipolar Excitons
- Second sound with ultracold atoms: A brief historical account
- Berezinskii-Kosterlitz-Thouless phase transition with Rabi-coupled bosons
- Sound modes in collisional superfluid Bose gases
- Dynamical Kosterlitz-Thouless Theory for Two-Dimensional Ultracold Atomic Gases
- Superfluid properties of bright solitons in a ring
- Berezinskii-Kosterlitz-Thouless phase induced by dissipating quasisolitons
- First and second sound in a dilute Bose gas across the BKT transition