Temperature dependence of the normal-state Hall coefficient of a quasi-one-dimensional metal

dc.creatorYakovenko, Victor M.
dc.creatorZheleznyak, Anatoley T.
dc.date1998-07-03
dc.date1998-09-25
dc.date.accessioned2026-07-07T07:48:20Z
dc.date.available2026-07-07T07:48:20Z
dc.descriptionWe develop a systematic theory of the Hall effect in Q1D conductors in both weak and strong magnetic fields for a model where the electron relaxation time varies over the Fermi surface. At high temperatures, the Hall coefficient saturates at the value $-β/ecn$, where the dimensionless coefficient $β$ is determined by the curvature of the longitudinal dispersion law of electrons, $e$ the electron charge, $c$ is the speed of light, and $n$ is the hole concentration. At low temperatures, where a strong variation of the relaxation rate over the Fermi surface develops in the form of ``hot spots'', the Hall coefficient becomes temperature-dependent and may change sign for a particular choice of the transverse dispersion law parameters. In our model, the sign changes in a weak, but not in a strong magnetic field.
dc.description5 pages, 3 figures, submitted to Synthetic Metals, proceedings of International Conference on Synthetic Metals, 1998, Montpellier, France. v.2: few references are added
dc.identifierhttps://arxiv.org/abs/cond-mat/9807047
dc.identifierhttp://arxiv.org/abs/cond-mat/9807047
dc.identifierSynthetic Metals 103, 2202-2205 (1999)
dc.identifierdoi:10.1016/S0379-6779(98)00921-7
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/124463
dc.subjectCondensed Matter
dc.titleTemperature dependence of the normal-state Hall coefficient of a quasi-one-dimensional metal
dc.typetext

Files

Collections