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Testing the tomographic Fermi liquid hypothesis with high-order cyclotron resonance

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arxiv 2409.05147 v2 pith:VVVLEI26 submitted 2024-09-08 cond-mat.str-el physics.optics

classification cond-mat.str-elphysics.optics
keywords cyclotronresonancefermiliquidtomographichypothesisangulardistribution
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abstract

Recent theoretical studies of carrier-carrier scattering in degenerate two-dimensional systems have revealed radically different relaxation times for odd and even angular harmonics of distribution function. This theoretical concept, dubbed as 'tomographic Fermi liquid', is yet challenging to test with dc electrical measurements as electron scattering weakly affects the electrical resistivity. Here, we show that linewidth and amplitude of electromagnetic absorption at the multiple harmonics of the cyclotron resonance carries all necessary information to test the tomographic Fermi liquid hypothesis. Namely, the height and inverse width of $m$-th order cyclotron resonance ($m \ge 2$) is proportional to the lifetime of $m$-th angular harmonic of electron distribution function $\tau_m$, if probed at wavelengths exceeding the cyclotron radius $R_c$. Measurements of high-order cyclotron resonance at short wavelengths order of $R_c$ also enable a direct determination of all lifetimes $\tau_m$ from a simple linear system of equations that we hereby derive. Extraction of cyclotron resonance lifetimes from an experiment on terahertz photoconductivity in graphene shows that third-order resonance is systematically narrower than second-order one, supporting the prediction of tomographic Fermi liquid hypothesis.

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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. Bosonized theory of de Haas-van Alphen quantum oscillation in Fermi liquids

    cond-mat.str-el 2025-06 conditional novelty 7.0 of 10

    For a 2D Fermi liquid, the de Haas-van Alphen amplitudes are derived from the zero-mode sector of a coadjoint-orbit bosonized action, yielding LK-like low-T behavior and a second harmonic A2 that changes sign at high T.

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