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  • Letter
  • Open Access

Second-order anomalous Hall effect controlled by electric fields in altermagnets

Arnob Mukherjee, Biplab Sanyal, Annica M. Black-Schaffer*, and Ankita Bhattacharya*,†

  • *These authors contributed equally to this work.
  • †Contact author: ankita.bhattacharya@physics.uu.se

Phys. Rev. B 113, L220401 – Published 3 June, 2026

DOI: https://doi.org/10.1103/wb4y-tzln

Abstract

Altermagnets are a recently discovered class of compensated magnets with momentum-dependent spin splittings and unusual transport properties, even without a net magnetization. In the presence of combined fourfold rotation and time-reversal (C4T) symmetry, linear and also second order, driven by a Berry curvature dipole, anomalous Hall responses are forbidden in any pure d-wave altermagnet. Nevertheless, here we find that the nontrivial quantum metric of the occupied Bloch states allows for an electric field induced Berry curvature dipole, which generates a strong and tunable second-order Hall current, enabling it to be switched on or off by simply adjusting the relative orientation between the symmetry-reducing dc field and the ac probe field. Specifically, we investigate the electric field induced second-order anomalous Hall response in a two-dimensional Rashba-coupled altermagnet with varying dx2−y2 (B1g) and dxy (B2g) altermagnet symmetry to capture all possibilities. Crucially, the nonlinear signal is highly sensitive to the underlying symmetry of the altermagnetic order at specific doping levels, offering a purely electrical method to distinguish distinct altermagnetic orders. Our results position altermagnets as a promising platform for controllable nonlinear transport and spintronic applications.

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