Heat diffusion in the disordered electron gas
arXiv:1509.02519 · doi:10.1103/PhysRevB.93.115121
Abstract
We study the thermal conductivity of the disordered two-dimensional electron gas. To this end we analyze the heat density-heat density correlation function concentrating on the scattering processes induced by the Coulomb interaction in the sub-temperature energy range. These scattering processes are at the origin of logarithmic corrections violating the Wiedemann-Franz law. Special care is devoted to the definition of the heat density in the presence of the long-range Coulomb interaction. To clarify the structure of the correlation function, we present details of a perturbative calculation. While the conservation of energy strongly constrains the general form of the heat density-heat density correlation function, the balance of various terms turns out to be rather different from that for the correlation functions of other conserved quantities such as the density-density or spin density-spin density correlation function.
23 pages, 12 figures
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Cited by in corpus (10)
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- Scale-dependent theory of the disordered electron liquid
- Non-linear sigma model with particle-hole asymmetry for the disordered two-dimensional electron gas
- Flexural phonons in supported graphene: from pinning to localization
- Lorenz ratio of an impure compensated metal in the degenerate Fermi liquid regime
- Interaction corrections to the thermopower of the disordered two-dimensional electron gas