Abstract

Near equilibrium, the rate of relaxation to equilibrium and the transport properties of excitations (bogolons) in a dilute Bose-Einstein condensate (BEC) are determined by three collision integrals, G12\mathcal{G}^{12}, G22\mathcal{G}^{22}, and G31\mathcal{G}^{31}. All three collision integrals conserve momentum and energy during bogolon collisions, but only G22 \mathcal{G}^{22} conserves bogolon number. Previous works have considered the contribution of only two collision integrals, G22 \mathcal{G}^{22} and G12 \mathcal{G}^{12}. In this work, we show that the third collision integral G31 \mathcal{G}^{31} makes a significant contribution to the bogolon number relaxation rate and needs to be retained when computing relaxation properties of the BEC. We provide values of relaxation rates in a form that can be applied to a variety of dilute Bose-Einstein condensates.Comment: 18 pages, 4 figures, accepted by Journal of Low Temperature Physics 7/201

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