Hydrodynamic approach to electronic transport in graphene: energy relaxation
arXiv:2102.00207 · doi:10.3389/fphy.2021.640649
Abstract
In nearly compensated graphene, disorder-assisted electron-phonon scattering or "supercollisions" are responsible for both quasiparticle recombination and energy relaxation. Within the hydrodynamic approach, these processes contribute weak decay terms to the continuity equations at local equilibrium, i.e., at the level of "ideal" hydrodynamics. Here we report the derivation of the decay term due to weak violation of energy conservation. Such terms have to be considered on equal footing with the well-known recombination terms due to nonconservation of the number of particles in each band. At high enough temperatures in the "hydrodynamic regime" supercollisions dominate both types of the interaction). We also discuss the contribution of supercollisions to the heat transfer equation (generalizing the continuity equation for the energy density in viscous hydrodynamics).
7 pages
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- Corbino magnetoresistance in neutral graphene
- Restoring time-reversal covariance in relaxed hydrodynamics
- Hall viscosity and hydrodynamic inverse Nernst effect in graphene
- Observability of cyclotron resonance in the hydrodynamic regime of bilayer graphene
- Hydrodynamic approach to many-body systems: exact conservation laws
- Energy relaxation dynamics in a nodal-line semimetal