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Role reversal in first and second sound in a relativistic superfluid

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arxiv 1310.5953 v2 pith:K3K7NREW submitted 2013-10-22 hep-ph cond-mat.othernucl-th

classification hep-phcond-mat.othernucl-th
keywords temperaturesoundsuperflowdensityfirstreversalrolesecond
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abstract

Relativistic superfluidity at arbitrary temperature, chemical potential and (uniform) superflow is discussed within a self-consistent field-theoretical approach. Our starting point is a complex scalar field with a $\varphi^4$ interaction, for which we calculate the 2-particle-irreducible effective action in the Hartree approximation. With this underlying microscopic theory, we can obtain the two-fluid picture of a superfluid, and compute properties such as the superfluid density and the entrainment coefficient for all temperatures below the critical temperature for superfluidity. We compute the critical velocity, taking into account the full self-consistent effect of the temperature and superflow on the quasiparticle dispersion. We also discuss first and second sound modes and how first (second) sound evolves from a density (temperature) wave at low temperatures to a temperature (density) wave at high temperatures. This role reversal is investigated for ultra-relativistic and near-non-relativistic systems for zero and nonzero superflow. For nonzero superflow, we also observe a role reversal as a function of the direction of the sound wave.

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Cited by 2 Pith papers

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  1. Coherence and Quantum Stability of Relativistic Superfluid States

    hep-th 2025-09 conditional novelty 7.0 of 10

    A charged scalar condensate is quantum-stable to all perturbative orders when it is described by the interacting vacuum of fluctuations, a non-Gaussian dressed coherent state that is an eigenstate of H minus mu Q.

  2. Dissipation triggers dynamical two-stream instability

    gr-qc 2019-08 conditional novelty 7.0 of 10

    Dissipation makes the relativistic two-stream instability dynamical exactly at the counterflow velocity where an ideal fluid would only show an energetic instability.

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