Stone-Wales defects in the gapless Kitaev spin liquid generate net chirality that opens a topological gap of 11 n_d and drives a finite-temperature transition to a chiral spin liquid via long-range Ising interactions.
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Defect density of order 10^{-4} to 10^{-2} in the Kitaev honeycomb model drives a true finite-T transition to a chiral spin liquid with T_c approximately 2 n_d, mediated by emergent r^{-2.7} ferromagnetic interactions between defect chiralities.
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Generation of chirality and orbital magnetization by Stone-Wales-type lattice defects in the Kitaev spin liquid
Stone-Wales defects in the gapless Kitaev spin liquid generate net chirality that opens a topological gap of 11 n_d and drives a finite-temperature transition to a chiral spin liquid via long-range Ising interactions.
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Chiral spin liquid instability of the Kitaev honeycomb model with crystallographic defects
Defect density of order 10^{-4} to 10^{-2} in the Kitaev honeycomb model drives a true finite-T transition to a chiral spin liquid with T_c approximately 2 n_d, mediated by emergent r^{-2.7} ferromagnetic interactions between defect chiralities.