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Anomalously long lifetimes in two-dimensional Fermi liquids

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arxiv 2210.16300 v2 pith:QUXOESJK submitted 2022-10-28 cond-mat.mes-hall cond-mat.quant-gascond-mat.stat-mech

classification cond-mat.mes-hallcond-mat.quant-gascond-mat.stat-mech
keywords regimedecayfermiliquidsodd-paritytemperaturestransportanomalously
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abstract

A precise characterization of the recently discovered crossover to hydrodynamic transport in electron liquids, and in particular of a conjectured exotic odd-parity transport regime, requires a full solution of the Fermi-liquid collision integral at all temperatures beyond state-of-the-art analytic leading-logarithmic approximations. We develop a general basis expansion of the linearized collision integral applicable at all temperatures, and employ this to determine the decay rates of Fermi surface perturbations in two-dimensional electron liquids. In particular, we provide exhaustive data on the decay rates for a new odd-parity regime, in which parity-even Fermi surface deformations decay rapidly but odd-parity modes are anomalously long lived. We find that this transport regime exists at fairly large temperatures $T \lesssim 0.1 T_F$, putting this regime within the reach of current experiments.

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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. Fourth-order closure obstruction and chiral nonlocality in circular kinetic magnetotransport

    cond-mat.mes-hall 2026-07 conditional novelty 7.0 of 10

    Closing a two-dimensional kinetic hierarchy at the stress level omits a definite fourth-order operator term, −κ4Δ² with κ4 = ν²/γ3, fixed by the relaxation rate of the m = 3 Fermi-surface harmonic.

  2. Complete kinematic null for local kinetic dissipation in a sixfold-driven electron fluid

    cond-mat.mes-hall 2026-08 conditional novelty 6.0 of 10

    A sixfold D12 drive creates a symmetry-forced point where current and its full gradient vanish, so local hydrodynamic heating is absent and an m=3 kinetic mode becomes the leading observable.

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