Nonlinear Anomalous Hall Effect in Type I Weyl Metals
POSTER
Abstract
Within the framework of linear response, Anomalous Hall Effect (AHE) in time reversal (TR) invariant systems is prohibited,
yet in inversion symmetry (P) breaking system, AHE second order in the applied fields is expected.
The Fermi sea contribution to both linear and nonlinear AHE in Weyl semimetal is due to Berry dipoles and multipoles, however, in a doped metallic phase free carrier contribution at each node is large when the cone is titled. We calculate the second order optical AHE conductivity in tilted Weyl nodes and characterize disorder contributions in the DC limit of first and second order AHE. We discuss the implications of our findings in the context of P-breaking TR-invariant system of Weyl nodes at nonzero chemical potential.
yet in inversion symmetry (P) breaking system, AHE second order in the applied fields is expected.
The Fermi sea contribution to both linear and nonlinear AHE in Weyl semimetal is due to Berry dipoles and multipoles, however, in a doped metallic phase free carrier contribution at each node is large when the cone is titled. We calculate the second order optical AHE conductivity in tilted Weyl nodes and characterize disorder contributions in the DC limit of first and second order AHE. We discuss the implications of our findings in the context of P-breaking TR-invariant system of Weyl nodes at nonzero chemical potential.
Presenters
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Aydin Keser
University of New South Wales & FLEET ARC, University of New South Wales, ARC FLEET, School of Physics, University of New South Wales
Authors
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Aydin Keser
University of New South Wales & FLEET ARC, University of New South Wales, ARC FLEET, School of Physics, University of New South Wales
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Dimitrie Culcer
University of New South Wales & FLEET ARC, University of New South Wales, ARC FLEET, School of Physics, University of New South Wales