A Criterion for Strange Metallicity in the Lorenz Ratio
arXiv:2211.00665 · doi:10.1038/s41535-023-00598-z
Abstract
The Wiedemann-Franz (WF) law, stating that the Lorenz ratio between the thermal and electrical conductivities in a metal approaches a universal constant at low temperatures, is often interpreted as a signature of fermionic Landau quasi-particles. In contrast, we show that various models of weakly disordered non-Fermi liquids also obey the WF law at . Instead, we propose using the leading low-temperature correction to the WF law, (proportional to the inelastic scattering rate), to distinguish different types of strange metals. As an example, we demonstrate that in a solvable model of a marginal Fermi liquid, . Using the quantum Boltzmann equation (QBE) approach, we find analogous behavior in a class of marginal- and non-Fermi liquids with a weakly momentum-dependent inelastic scattering. In contrast, in a Fermi liquid, is proportional to . This holds even when the resistivity grows linearly with , due to linear quasi-elastic scattering (as in the case of electron-phonon scattering at temperatures above the Debye frequency). Finally, by exploiting the QBE approach, we demonstrate that the transverse Lorenz ratio, , exhibits the same behavior.
6 + 10 pages, published version includes a generalization of the criterion to the transverse Lorenz ratio
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Cited by in corpus (7)
- Tunable non-Fermi liquid phase from coupling to two-level systems
- The Wiedemann-Franz law in doped Mott insulators without quasiparticles
- Solvable models of two-level systems coupled to itinerant electrons: Robust non-Fermi liquid and quantum critical pairing
- The Lorenz ratio as a guide to scattering contributions to Planckian transport
- Extended strange metal regime from superconducting puddles
- Fermi Surface Bosonization for Non-Fermi Liquids
- Lorenz ratios of diagonal and Hall conductivities in a Dirac electron liquid