Electronic thermal conductivity of disordered metals
arXiv:cond-mat/0402245 · doi:10.1103/PhysRevB.70.155109
Abstract
We calculate the thermal conductivity of interacting electrons in disordered metals. In our analysis we point out that the interaction affects thermal transport through two distinct mechanims, associated with quantum interference corrections and energy exchange of the quasi particles with the electromagnetic environment, respectively. The latter is seen to lead to a violation of the Wiedemann-Franz law. Our theory predicts a strong enhancement of the Lorenz ratio over the value which is predicted by the Wiedemann-Franz law, when the electrons encounter a large environmental impedance.
4 pages
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- Berezinskii-Kosterlitz-Thouless transition in homogeneously disordered superconducting films
- Electron-electron interaction corrections to the thermal conductivity in disordered conductors
- Spin thermoelectrics in a disordered Fermi gas
- Deviation from the Wiedemann-Franz law induced by nonmagnetic impurities in overdoped La_{2-x}Sr_{x}CuO_{4}
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- Interaction corrections: temperature and parallel field dependencies of the Lorentz number in two-dimensional disordered metals
- Theory of thermal and charge transport in diffusive normal metal / superconductor junctions
- The role of electron-electron collisions for charge and heat transport at intermediate temperatures
- Renormalization group analysis of thermal transport in the disordered Fermi liquid
- Theory of Thermal Conductivity in the Disordered Electron Liquid
- Scale-dependent theory of the disordered electron liquid
- Non-linear sigma model with particle-hole asymmetry for the disordered two-dimensional electron gas
- Lorenz ratio of an impure compensated metal in the degenerate Fermi liquid regime
- Chiral second-sound collective mode at the edge of 2D systems with nontrivial Berry curvature
- Interaction corrections to the thermopower of the disordered two-dimensional electron gas