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Magnetization-dependent and stacking-tunable Edelstein effect in the two-dimensional magnet
Phys. Rev. B 114, 125129 – Published 24 August, 2026
DOI: https://doi.org/10.1103/48gx-cpg2
Abstract
The Edelstein effect in magnetic systems enables magnetization switching via the coupling between current-induced spin accumulation and intrinsic magnetic order and is therefore highly promising for next-generation spintronic devices. Realizing and manipulating the Edelstein effect in two-dimensional (2D) magnetic systems is particularly desirable for achieving high-efficiency and multifunctional spintronic applications. In this work, based on first-principles calculations and symmetry analysis, we demonstrate that the Edelstein effect can intrinsically arise in the 2D in-plane ferromagnetic semiconductor , with its behavior strongly dependent on the magnetization orientation. For monolayer with crystal symmetry, under an applied current along the direction, only the time-reversal-even component and the time-reversal-odd component of the spin accumulation are allowed when the magnetization is aligned along . For ferromagnetic bilayer in AB or BA stacking, where the crystal symmetry is reduced to , additional spin components emerge with the presence of in-plane magnetization. Specifically, for magnetization along , besides and , extra components such as become allowed. Notably, these additional components can be reversibly switched by changing the stacking configuration from AB to BA via interlayer sliding, which is equivalent to applying a operation. The parity dependence of Edelstein coefficients on the in-plane magnetization is also evaluated. Our results not only deepen the understanding of current-induced spin accumulation in 2D magnetic systems from both symmetry and first-principles perspectives but also identify materials as a promising platform for realizing intrinsic and tunable Edelstein effects in high-efficiency spin-orbit torque devices.
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