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Hydrodynamic sound modes and Galilean symmetry breaking in a magnon fluid

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arxiv 1810.12333 v2 pith:S3RXWC6V submitted 2018-10-29 cond-mat.mes-hall

classification cond-mat.mes-hall
keywords hydrodynamicmagnonsoundregimespinsymmetrycollision-dominateddetected
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The non-interacting magnon gas description in ferromagnets breaks down at finite magnon density where momentum-conserving collisions between magnons become important. Observation of the collision-dominated regime, however, has been hampered by the lack of probes to access the energy and lengthscales characteristic of this regime. Here we identify a key signature of the collision-dominated hydrodynamic regime---a magnon sound mode---which governs dynamics at low frequencies and can be detected with recently-introduced spin qubit magnetometers. The magnon sound mode is an excitation of the longitudinal spin component with frequencies below the spin wave continuum in gapped ferromagnets. We also show that, in the presence of exchange interactions with SU(2) symmetry, the ferromagnet hosts an usual hydrodynamic regime that lacks Galilean symmetry at all energy and lengthscales. The hydrodynamic sound mode, if detected, can lead to a new platform to explore hydrodynamic behavior in quantum materials.

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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. Universal prethermal dynamics in Heisenberg ferromagnets

    cond-mat.stat-mech 2019-08 conditional novelty 7.0 of 10

    Universal prethermal scaling for magnons in Heisenberg ferromagnets has exponents alpha=0.65 and beta=0.30, distinct from BEC dynamics.

  2. Spin functional renormalization group for quantum Heisenberg ferromagnets: Magnetization and magnon damping in two dimensions

    cond-mat.stat-mech 2019-08 conditional novelty 6.0 of 10

    The spin functional renormalization group, closed with a Ward identity, yields the magnetic equation of state and magnon damping of a 2D Heisenberg ferromagnet, matching Monte Carlo at low temperatures for finite fields.

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