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Classification of electromagnetic responses by quantum geometry

Longjun Xiang, Jinxiong Jia, Fuming Xu, Jian Wang

Abstract

The nonlinear charge current $j_a=σ_{abc}E_bE_c$ of Bloch electrons in quantum materials under an electric field can be well characterized by the quantum geometry, as most exemplified by the extrinsic and intrinsic nonlinear Hall effects induced by the Berry curvature dipole and the quantum metric dipole, respectively. Nevertheless, a unified quantum geometric description for the bilinear charge current $j_a=σ_{ab,c}E_bB_c$ of Bloch electrons driven by the electromagnetic fields, including the ordinary Hall effect (OHE), the magnetononlinear Hall effect (MNHE), and the planar Hall effect (PHE), remains elusive. Herein, we show that this bilinear conductivity, as contributed by the orbital minimal coupling and the spin Zeeman coupling of the applied magnetic field, respectively, can be classified by the conventional quantum geometry and the recently proposed Zeeman quantum geometry, where the symmetry constraint from the fundamental response equation is encoded. Specifically, we uncover that the intrinsic orbital and spin bilinear currents--responsible for the orbital and spin MNHEs--are governed by the quantum metric quadrupole and the Zeeman quantum metric dipole, respectively. In contrast, the extrinsic orbital and spin bilinear currents, which are linear in the relaxation time $τ$ and lead to the orbital and spin PHEs, are governed by the Berry curvature quadrupole and the Zeeman Berry curvature dipole, respectively. Counterintuitively, we find that the OHE due to the Lorentz force can also include an interband contribution from the quantum metric quadrupole. After building the quantum geometric classification of this bilinear current, we study the rarely known spin PHE with the surface Dirac cone of three-dimensional topological insulators.

Classification of electromagnetic responses by quantum geometry

Abstract

The nonlinear charge current of Bloch electrons in quantum materials under an electric field can be well characterized by the quantum geometry, as most exemplified by the extrinsic and intrinsic nonlinear Hall effects induced by the Berry curvature dipole and the quantum metric dipole, respectively. Nevertheless, a unified quantum geometric description for the bilinear charge current of Bloch electrons driven by the electromagnetic fields, including the ordinary Hall effect (OHE), the magnetononlinear Hall effect (MNHE), and the planar Hall effect (PHE), remains elusive. Herein, we show that this bilinear conductivity, as contributed by the orbital minimal coupling and the spin Zeeman coupling of the applied magnetic field, respectively, can be classified by the conventional quantum geometry and the recently proposed Zeeman quantum geometry, where the symmetry constraint from the fundamental response equation is encoded. Specifically, we uncover that the intrinsic orbital and spin bilinear currents--responsible for the orbital and spin MNHEs--are governed by the quantum metric quadrupole and the Zeeman quantum metric dipole, respectively. In contrast, the extrinsic orbital and spin bilinear currents, which are linear in the relaxation time and lead to the orbital and spin PHEs, are governed by the Berry curvature quadrupole and the Zeeman Berry curvature dipole, respectively. Counterintuitively, we find that the OHE due to the Lorentz force can also include an interband contribution from the quantum metric quadrupole. After building the quantum geometric classification of this bilinear current, we study the rarely known spin PHE with the surface Dirac cone of three-dimensional topological insulators.

Paper Structure

This paper contains 1 section, 9 equations, 2 figures, 1 table.

Table of Contents

  1. Acknowledgements

Figures (2)

  • Figure 1: Quantum geometric classification of (a) the nonlinear charge current Eq. (\ref{['EEresponse']}) and (b) the bilinear charge current Eq. (\ref{['EBresponse']}). NDC FuBCD: nonlinear Drude current; ENHE FuBCD/INHE GaoY2014PRL: extrinsic/intrinsic nonlinear Hall effect; PHE PHE: planar Hall effect; MNHE GaoY2014PRLMNHE1: magnetononlinear Hall effect; OHE Nagaosa2010: ordinary Hall effect; BCD FuBCD: Berry curvature dipole; ZBCD xiangSHE; Zeeman BCD; QMD BPT1: quantum metric dipole; ZQMD xiangSHE: Zeeman QMD; BCQ KTLawPRB: Berry curvature quadrapole; QMQ QMQ1QMQ2QMQ3: quantum metric quadrapole; SBC Duan2024: square Berry curvature.
  • Figure 2: (a) Band dispersions of Eq. (\ref{['TIsurf']}). Here the horizontal dashed line denotes the chmeical potential $\mu$. (b) The "quantized" spin PHE conductivity. The $\boldsymbol{k}$-resolved Zeeman Berry curvature (c) $\mathcal{Z}_{-+}^{xx}$ and (d) $\mathcal{Z}_{-+}^{yx}$. Parameters: $\beta=1/8$SBZhangPRL, $B_x=1 \mathrm{T}$, $\tau=0.5 \mathrm{ps}$KTLawPRB and $g=10$gfactor.