Saved in:
Bibliographic Details
Main Authors: Sharma, Gargee, Goswami, Pallab, Tewari, Sumanta
Format: Preprint
Published: 2015
Subjects:
Online Access:https://arxiv.org/abs/1507.05606
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866914683669184512
author Sharma, Gargee
Goswami, Pallab
Tewari, Sumanta
author_facet Sharma, Gargee
Goswami, Pallab
Tewari, Sumanta
contents Weyl semimetals (WSM) are topologically protected three dimensional materials whose low energy excitations are linearly dispersing massless Dirac fermions, possessing a non-trivial Berry curvature. Using semi-classical Boltzmann dynamics in the relaxation time approximation for a lattice model of time reversal (TR) symmetry broken WSM, we compute both magnetic field dependent and anomalous contributions to the Nernst coefficient. In addition to the magnetic field dependent Nernst response, which is present in both Dirac and Weyl semimetals, we show that, contrary to previous reports, the TR-broken WSM also has an anomalous Nernst response due to a non-vanishing Berry curvature. We also compute the thermal conductivities of a WSM in the Nernst (${\nabla T} \perp \mathbf{B}$) and the longitudinal (${\nabla T} \parallel \mathbf{B}$) set-up and confirm from our lattice model that in the parallel set-up, the Wiedemann-Franz law is violated between the longitudinal thermal and electrical conductivities due to chiral anomaly.
format Preprint
id arxiv_https___arxiv_org_abs_1507_05606
institution arXiv
publishDate 2015
record_format arxiv
spellingShingle Nernst and magneto-thermal conductivity in a lattice model of Weyl fermions
Sharma, Gargee
Goswami, Pallab
Tewari, Sumanta
Strongly Correlated Electrons
Weyl semimetals (WSM) are topologically protected three dimensional materials whose low energy excitations are linearly dispersing massless Dirac fermions, possessing a non-trivial Berry curvature. Using semi-classical Boltzmann dynamics in the relaxation time approximation for a lattice model of time reversal (TR) symmetry broken WSM, we compute both magnetic field dependent and anomalous contributions to the Nernst coefficient. In addition to the magnetic field dependent Nernst response, which is present in both Dirac and Weyl semimetals, we show that, contrary to previous reports, the TR-broken WSM also has an anomalous Nernst response due to a non-vanishing Berry curvature. We also compute the thermal conductivities of a WSM in the Nernst (${\nabla T} \perp \mathbf{B}$) and the longitudinal (${\nabla T} \parallel \mathbf{B}$) set-up and confirm from our lattice model that in the parallel set-up, the Wiedemann-Franz law is violated between the longitudinal thermal and electrical conductivities due to chiral anomaly.
title Nernst and magneto-thermal conductivity in a lattice model of Weyl fermions
topic Strongly Correlated Electrons
url https://arxiv.org/abs/1507.05606