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The first-order anisotropy energy term is ∆ E1 ∼ 1 − cos β, where β denotes the tilt of magnetic moments out of the xy-plane

Under the rigid-body rotation of Euler angles ( α, β, γ), the spin-orbit vector has the form O = Rz(α)Ry(β)Rz (γ), where Ri(θ) denotes the rotation matrix about axis i through an

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Rigid-Body Anisotropy in Noncollinear Antiferromagnets

cond-mat.mtrl-sci · 2025-07-14 · conditional · novelty 7.0

The paper derives a spin-group representation framework that expresses magnetic anisotropy and anomalous Hall anisotropy in noncollinear antiferromagnets as polynomial expansions in a spin-orbit vector, demonstrating first-order spin-orbit anisotropy in Mn3Sn.

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  • Rigid-Body Anisotropy in Noncollinear Antiferromagnets cond-mat.mtrl-sci · 2025-07-14 · conditional · none · ref 3

    The paper derives a spin-group representation framework that expresses magnetic anisotropy and anomalous Hall anisotropy in noncollinear antiferromagnets as polynomial expansions in a spin-orbit vector, demonstrating first-order spin-orbit anisotropy in Mn3Sn.