A spin-1 Kitaev-Gamma chain with single-ion anisotropy exhibits a Kitaev-to-large-D crossover and a changeover to an SU(2)₂ WZW continuous transition with emergent conformal symmetry.
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The Kitaev-J3 model hosts deconfined magnetic phases in which zigzag or antiferromagnetic order coexists with remnant Z2 topological structure inherited from the Kitaev spin liquid through vison-pair condensation.
Non-Hermitian Gamma interaction on the TFIM induces a PT-broken gapless phase with long- and short-range spin-nematic correlations, diagnosable via dynamical nematic correlators.
Magnetic fields applied to anisotropic Kitaev chains produce ordered phases with four-site, large-unit-cell, and six-site uniform-chirality periodicities, explained by an effective model containing transverse Ising, Dzyaloshinskii-Moriya, and further-neighbor Ising interactions.
NLCE calculations on the J-K-Γ model for α-RuCl3 show that the linear magnetostriction coefficient perpendicular to the plane exhibits a dip-like feature tied to the suppression of magnetic order.
citing papers explorer
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Crossover and Changeover in Spin-1 Kitaev-$\Gamma$ Chain with Uniaxial Single-ion Anisotropy
A spin-1 Kitaev-Gamma chain with single-ion anisotropy exhibits a Kitaev-to-large-D crossover and a changeover to an SU(2)₂ WZW continuous transition with emergent conformal symmetry.
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Evidence for Deconfined Magnetic Order in the Kitaev-$J_3$ Model
The Kitaev-J3 model hosts deconfined magnetic phases in which zigzag or antiferromagnetic order coexists with remnant Z2 topological structure inherited from the Kitaev spin liquid through vison-pair condensation.
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Dynamical spin-nematic correlation in a transverse field Ising chain with non-Hermitian Gamma interaction
Non-Hermitian Gamma interaction on the TFIM induces a PT-broken gapless phase with long- and short-range spin-nematic correlations, diagnosable via dynamical nematic correlators.
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Field-Induced Ordered Phases in Anisotropic Spin-1/2 Kitaev Chains
Magnetic fields applied to anisotropic Kitaev chains produce ordered phases with four-site, large-unit-cell, and six-site uniform-chirality periodicities, explained by an effective model containing transverse Ising, Dzyaloshinskii-Moriya, and further-neighbor Ising interactions.
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Magnetostriction in the $J$-$K$-$\Gamma$ model: Application of the numerical linked cluster expansion
NLCE calculations on the J-K-Γ model for α-RuCl3 show that the linear magnetostriction coefficient perpendicular to the plane exhibits a dip-like feature tied to the suppression of magnetic order.