Hall Coefficient in an Interacting Electron Gas

dc.creatorKhodas, M.
dc.creatorFinkel'stein, A. M.
dc.date2002-12-30
dc.date2004-01-18
dc.date.accessioned2026-07-07T02:48:57Z
dc.date.available2026-07-07T02:48:57Z
dc.descriptionThe Hall conductivity in a weak homogeneous magnetic field, $ω_{c}τ\ll 1$, is calculated. We have shown that to leading order in $1/ε_{F}τ$ the Hall coefficient $R_{H}$ is not renormalized by the electron-electron interaction. Our result explains the experimentally observed stability of the Hall coefficient in a dilute electron gas not too close to the metal-insulator transition. We avoid the currently used procedure that introduces an artificial spatial modulation of the magnetic field. The problem of the Hall effect is reformulated in a way such that the magnetic flux associated with the scattering process becomes the central element of the calculation.
dc.description23 pages, 15 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0212628
dc.identifierhttp://arxiv.org/abs/cond-mat/0212628
dc.identifierPhys. Rev. B 68, 155114 (2003)
dc.identifierdoi:10.1103/PhysRevB.68.155114
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/20608
dc.subjectStrongly Correlated Electrons
dc.titleHall Coefficient in an Interacting Electron Gas
dc.typetext

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