Orbital altermagnetism is defined as a symmetry-protected order of orbital magnetic moments with d-wave-like momentum locking, shown via tight-binding models and DFT in materials such as CuBr2, VS2, MoO and CrO.
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In a V-shaped 1D chain the nonmagnetic magnetoelectric response peaks near apex angle 0.6π because geometry induces an effective spin-orbit term whose angular factor sinθ sin(θ/2) matches Kubo-formula numerics.
Derives corrected orbital magnetic moment matrix elements for non-degenerate Bloch states including Berry connection contributions and shows reduced orbital Hall conductivity in bilayer TMDC and graphene systems.
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Orbital Altermagnetism
Orbital altermagnetism is defined as a symmetry-protected order of orbital magnetic moments with d-wave-like momentum locking, shown via tight-binding models and DFT in materials such as CuBr2, VS2, MoO and CrO.
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Shape dependence of Edelstein and magnetoelectric effects in the V-shaped model
In a V-shaped 1D chain the nonmagnetic magnetoelectric response peaks near apex angle 0.6π because geometry induces an effective spin-orbit term whose angular factor sinθ sin(θ/2) matches Kubo-formula numerics.
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Orbital Hall effect from orbital magnetic moments of Bloch states: the role of a new correction term
Derives corrected orbital magnetic moment matrix elements for non-degenerate Bloch states including Berry connection contributions and shows reduced orbital Hall conductivity in bilayer TMDC and graphene systems.