Magnon spin angular momentum in bilayer CrSBr is renormalized by anisotropy and dipolar interactions and diverges at field-induced softening, creating a peak in the thermal spin Seebeck effect.
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Geometric percolation of Ti vacancies in 1T-TiS2 monolayers triggers half-metallic ferromagnetism at xc ≈ 12.5%, creating a functional window of 11% < x < 15% with 100% spin-polarized transport.
In a Kondo model on the triangular lattice with nested pockets at Gamma and M, classical spins form stable chiral tetrahedral orders that gap the bands and produce a quantum anomalous Hall conductivity of 4e²/h.
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Spin-caloritronic signatures of soft magnons in bilayer CrSBr
Magnon spin angular momentum in bilayer CrSBr is renormalized by anisotropy and dipolar interactions and diverges at field-induced softening, creating a peak in the thermal spin Seebeck effect.