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Effect of disorder on the transverse magnetoresistance of Weyl semimetals

ORAL

Abstract

We study the effect of random potential created by different types of impurities on the transverse magnetoresistance of Weyl semimetals. It is shown that the magnetic field and temperature dependence of magnetoresistance is strongly affected by the type of impurity potential. Two limiting cases are analyzed in detail: (i) the ultra-quantum limit, when the applied magnetic field is so high that only the zeroth and first Landau levels contribute to the magnetotransport, and (ii) the semiclassical situation, for which a large number of Landau levels comes into play. A formal diagrammatic approach allowed us to obtain expressions for the components of the electrical conductivity tensor in both limits. In contrast to the oversimplified case of the δ-correlated disorder, the long-range impurity potential (including that of Coulomb impurities) introduces an additional length scale, which changes the geometry and physics of the problem. It is shown that the magnetoresistance can deviate from the linear behavior as a function of magnetic field for a certain class of impurity potentials.

[1] https://arxiv.org/abs/1506.07556
Phys. Rev. B, in press.

Presenters

  • Yaroslav Rodionov

    Theoretical Condensed matter physics, Institute for Theoretical and Applied Electrodynamics, Russian Academy of Sciences

Authors

  • Yaroslav Rodionov

    Theoretical Condensed matter physics, Institute for Theoretical and Applied Electrodynamics, Russian Academy of Sciences

  • Kliment I Kugel

    Theoretical Condensed matter physics, Institute for Theoretical and Applied Electrodynamics, Russian Academy of Sciences

  • Boris A Aronzon

    Condensed matter physics, P. N. Lebedev Physical Institute, Russian Academy of Sciences

  • Franco Nori

    RIKEN, Japan and Univ. Michigan, USA, RIKEN, Japan, RIKEN; and Univ. Michigan., RIKEN, Japan; and Univ. Michigan, USA, Riken Japan and Univ. Michigan USA, RIKEN, Japan and Univ Michigan, USA, Theoretical Quantum Physics Laboratory, Department of Physics, RIKEN Cluster for Pioneering Research, The University of Michigan, RIKEN and Univ. of Michigan, Riken Japan and Univ Michigan USA, RIKEN; and University of Michigan, RIKEN and Univ. Michigan, RIKEN and Univ of Michigan, Theoretical Quantum Physics Laboratory, RIKEN Cluster for Pioneering Research, Wako-shi, Saitama 351-0198, Japan, RIKEN, and University of Michigan, Theoretical Quantum Physics, Riken, Japan, RIKEN, Japan; and Univ Michigan, USA, Theoretical Quantum Physics Laboratory, RIKEN, RIKEN, Japan; Univ. Michigan, USA, RIKEN, Japan; Uni. Michigan, USA