A SOC-enabled uniaxial spin space-group quasi-symmetry determines whether the weak ferromagnetic moment induced in altermagnets is linear, quadratic, or cubic in spin-orbit coupling, explaining the material-dependent amplitude of the FM moment.
Weak Ferromagnetism in Altermagnets from Alternating $g$-Tensor Anisotropy
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abstract
Altermagnets are magnetic materials with antiferromagnetic spin ordering but exhibit ferromagnetic properties. Understanding the microscopic origin of the latter is a central problem. Ferromagnet-like properties such as the anomalous Hall effect are linked with weak ferromagnetism, whose microscopic origin in altermagnets remains unclear however. We show theoretically that the alternating $g$-tensor anisotropy in altermagnets can induce weak ferromagnetism even when the Dzyaloshinskii-Moriya interaction is forbidden. We demonstrate this mechanism to explain weak ferromagnetism for both collinear and noncollinear spin altermagnets. Our findings provide new insights into the origin of weak ferromagnetism and suggest orbital-based ways for manipulating magnetic configurations in altermagnets.
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Quasi-symmetry Constrained Spin Ferromagnetism in Altermagnets
A SOC-enabled uniaxial spin space-group quasi-symmetry determines whether the weak ferromagnetic moment induced in altermagnets is linear, quadratic, or cubic in spin-orbit coupling, explaining the material-dependent amplitude of the FM moment.