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We use numerical linked cluster (NLC) expansions to compute the specific heat, C(T), and entropy, S(T), of a quantum spin ice model of Yb2Ti2O7 using anisotropic exchange interactions recently determined from inelastic neutron scattering measurements and find good agreement with experimental calorimetric data.
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To relate our presentation more directly to the compact lattice QED context set in Refs. [ 9 , 10 ] , in which confinement in three-dimensions is traditionally referred to the strong (electric charge) coupling, we refrain from using the language of “monopoles” employed in Ref. [ 12 ] to label local defects in the ice rule of the parent classical spin ice. We use instead the more traditional wording of spinon/antispinon to label finite energy excitations out of the 2in/2out spin ice manifold
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