Numerical calculations reveal a chiral p-wave roton mode at finite momentum and a d-wave nematic mode at zero momentum in the SU(2) symmetric chiral spin liquid phase of the J1-J2-Jχ model.
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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.
Long-range edge disorder enables Raman circular dichroism to probe chiral edge modes in Kitaev spin liquids, with a unique anisotropic Zeeman field fingerprint from boundary charge interactions.
Light-matter coupling expansion of the magnon Hamiltonian yields the Fleury-Loudon Raman vertex, directly connecting Raman circular dichroism to magnon band Berry curvature.
citing papers explorer
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Collective excitations in chiral spin liquid: chiral roton and long-wavelength nematic mode
Numerical calculations reveal a chiral p-wave roton mode at finite momentum and a d-wave nematic mode at zero momentum in the SU(2) symmetric chiral spin liquid phase of the J1-J2-Jχ model.
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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.
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Dichroic Raman probes for chiral edge modes
Long-range edge disorder enables Raman circular dichroism to probe chiral edge modes in Kitaev spin liquids, with a unique anisotropic Zeeman field fingerprint from boundary charge interactions.
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Light-Matter-Coupling formalism for magnons: probing quantum geometry with light
Light-matter coupling expansion of the magnon Hamiltonian yields the Fleury-Loudon Raman vertex, directly connecting Raman circular dichroism to magnon band Berry curvature.