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.
Kitaev, Anyons in an exactly solved model and be- yond, Ann
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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.
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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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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.