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Pseudo-spontaneous $U(1)$ Symmetry Breaking in Hydrodynamics and Holography

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arxiv 2111.10305 v2 pith:H6U5RKWX submitted 2021-11-19 hep-th cond-mat.mes-hallcond-mat.str-elnucl-th

classification hep-thcond-mat.mes-hallcond-mat.str-elnucl-th
keywords breakingsymmetryphaserelaxationexplicitgoldstonebulkholographic
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abstract

We investigate the low-energy dynamics of systems with pseudo-spontaneously broken $U(1)$ symmetry and Goldstone phase relaxation. We construct a hydrodynamic framework which is able to capture these, in principle independent, effects. We consider two generalisations of the standard holographic superfluid model by adding an explicit breaking of the $U(1)$ symmetry by either sourcing the charged bulk scalar or by introducing an explicit mass term for the bulk gauge field. We find agreement between the hydrodynamic dispersion relations and the quasi-normal modes of both holographic models. We verify that phase relaxation arises only due to the breaking of the inherent Goldstone shift symmetry. The interplay of a weak explicit breaking of the $U(1)$ and phase relaxation renders the DC electric conductivity finite but does not result in a Drude-like peak. In this scenario we show the validity of a universal relation, found in the context of translational symmetry breaking, between the phase relaxation rate, the mass of the pseudo-Goldstone and the Goldstone diffusivity.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Higher-form (Quasi)Hydrodynamics from Holography: Deformations and Dualities

    hep-th 2025-09 conditional novelty 6.0 of 10

    Massless and massive higher-form gauge fields in anti-de Sitter space yield a full low-energy map of diffusive, relaxing, and emergent-photon modes governed by double-trace deformations.

  2. Schwinger-Keldysh effective action for hydrodynamics with approximate symmetries

    hep-th 2024-11 conditional novelty 6.0 of 10

    The axial charge relaxation coefficient in the Schwinger-Keldysh effective theory of QCD must be of second order in the quark mass, Γ_A = γ_A m_q^2, subleading in the broken phase and leading in the restored phase.

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