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.
Smoothly cutting off thiskintegral byn 1/2 d can produce an approximater −γ form with 2< γ <3
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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.