📝 SummarXiv

Abstract

The nonlinear charge current $j_a=\sigma_{abc}E_bE_c$ 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 $j_a=\sigma_{ab,c}E_bB_c$ 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 $\tau$ 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.