Exchange anisotropy Δ in X₂YCo(PO₄)₂ and X₂Co(SeO₃)₂ families is determined by the ratio of trigonal crystal field to spin-orbit coupling, providing a microscopic design rule for spin supersolids.
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SSD-based finite-size calculations show shoulder or double-peak specific heat in triangular and kagome antiferromagnets plus strong low-T susceptibility enhancement in kagome, indicating magnetic states dominate its excitations below 0.5J unlike the triangular case.
citing papers explorer
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A microscopic design rule for spin supersolids in triangular-lattice magnets
Exchange anisotropy Δ in X₂YCo(PO₄)₂ and X₂Co(SeO₃)₂ families is determined by the ratio of trigonal crystal field to spin-orbit coupling, providing a microscopic design rule for spin supersolids.
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Specific heat and susceptibility of S=1/2 antiferromagnets on square, triangular, and kagome lattices
SSD-based finite-size calculations show shoulder or double-peak specific heat in triangular and kagome antiferromagnets plus strong low-T susceptibility enhancement in kagome, indicating magnetic states dominate its excitations below 0.5J unlike the triangular case.