Skip to content

PRB.92.161110 Pallab Goswami

Optical activity as a test for dynamic chiral magnetic effect of Weyl semimetals

Journal Ref. Phys. Rev. B 92, 161110(R)(2015)

Keywords

Idea of the paper

A general formula for the dynamic chiral magnetic conductivity of the inversion symmetry breaking(ISB) Weyl semimetal is calculated. Shows that the measurement of the natural optical activity or rotary power provides a direct confirmation of the existence of dynamic chiral magnetic effect in Inversion symmetry breaking Weyl semimetal. (proposes an experimental test)

The natural optical activity can be used as a test for the existence of the real part of the dynamic chiral magnetic conductivity of inversion-symmetry-breaking WSMs such as TaAs and NbAs.

Summary

The currents due to Optical gyrotropy#Equation for gyrotropic current and Chiral magnetic effect#Equation for chiral magnetic current gives us the following relation, \(\(\sigma_{ch}(\textbf{q},w) = i\omega \sigma_g(\textbf{q},w)\)\) In the presence of a nonzero gyrotropic conductivity, the refractive indices for the left and the right circularly polarized light become different, which in turn causes a rotation of the plane of polarization for the transmitted light, even in the absence of a uniform external magnetic field. The amount of rotation of the plane of polarization per unit length is known as the rotary power, and the imaginary part of the gyrotropic conductivity governs the size of the rotary power

Hamiltonian

Tight-binding model of an WSM with broken P symmetry.

Experimental systems such as TaAs and NbAs are body-centered tetragonal systems which possess 12 pairs of right and left-handed Weyl fermions (altogether 24 Weyl points). There exists no simple Tight-binding model for such materials.

\(\(H = \sum_k \psi_k^\dagger[N_{0,k}\sigma_0 + \mathbf{N_k}\cdot\mathbf{\sigma}]\psi_k\)\) where the spin-independent hopping term \(N_{0,k}\) and the spin-orbit coupling terms \(\mathbf{N_k}\)are respectively even and odd under spatial inversion. We only choose NN hopping terms and obtain \(\mathbf{N_k} = t_{SO}[sin(k_1a),sin(k_2a),sin(k_3a)]\) and \(\mathbf{N_0} = -2t_1[cos(k_1a),cos(k_2a),cos(k_3a)]\) with \(t_1 << t_{SO}\)

The Weyl excitations occur around the eight high symmetry points can be seen below (For computational implementation, see Weyl points ISB)

WSM_ISB.jpg

In addition, \(\Gamma\) and M points act as the four right-handed Weyl points, while R and X points are the four left-handed Weyl points. In the vicinity of these points, quasiparticles possess linear dispersion and the Berry curvature acquires the characteristic form of a monopole (antimonopole)

The spin-independent hopping term shifts the Weyl points in the energy space, and gives rise to the chiral chemical potential