Quantum critical transport in clean graphene

dc.creatorFritz, Lars
dc.creatorSchmalian, Joerg
dc.creatorMueller, Markus
dc.creatorSachdev, Subir
dc.date2008-02-29
dc.date2008-03-09
dc.date.accessioned2026-07-07T09:56:07Z
dc.date.available2026-07-07T09:56:07Z
dc.descriptionWe describe electrical transport in ideal single-layer graphene at zero applied bias. There is a crossover from collisionless transport at frequencies larger than k_B T/hbar (T is the temperature) to collision-dominated transport at lower frequencies. The d.c. conductivity is computed by the solution of a quantum Boltzmann equation. Due to a logarithmic singularity in the collinear scattering amplitude (a consequence of relativistic dispersion in two dimensions) quasi-particles and -holes moving in the same direction tend to an effective equilibrium distribution whose parameters depend on the direction of motion. This property allows us to find the non-equilibrium distribution functions and the quantum critical conductivity exactly to leading order in 1/|ln(alpha)| where alpha is the coupling constant characterizing the Coulomb interactions.
dc.description19 pages, 1 figure; (v2) added comment on hydrodynamic long-time tails
dc.identifierhttps://arxiv.org/abs/0802.4289
dc.identifierhttp://arxiv.org/abs/0802.4289
dc.identifierPhysical Review B 78, 085416 (2008)
dc.identifierdoi:10.1103/PhysRevB.78.085416
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/166868
dc.subjectMesoscale and Nanoscale Physics
dc.subjectStrongly Correlated Electrons
dc.titleQuantum critical transport in clean graphene
dc.typetext

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