A systematic formalism using spin point groups to derive the symmetry-adapted form of crystal tensors in magnets, separating SOC-free effects from SOC-driven ones.
55) in its paramagnetic phase and below 21K exhibits a collinear magnetic structure [45], with propagation vector k = 0 and MSG P b′am (OG No
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Crystal tensor properties of magnetic materials with and without spin-orbit coupling. Application of spin point groups as approximate symmetries
A systematic formalism using spin point groups to derive the symmetry-adapted form of crystal tensors in magnets, separating SOC-free effects from SOC-driven ones.