The ground-states of the spin-S antiferromagnetic chain HAF with a projection-based interaction and the spin-1/2 XXZ-chain HXXZ at anisotropy parameter Δ = cosh (λ) share a common loop representation in terms of a two-dimensional functional integral which is similar to the classical planar Q-state Potts model at Q=2S+1=2cosh(λ). The multifaceted relation is used here to directly relate the distinct forms of translation symmetry breaking which are manifested in the ground-states of these two models: dimerization for HAF at all S> 1 / 2 , and Néel order for HXXZ at λ> 0. The results presented include: (i) a translation to the above quantum spin systems of the results which were recently proven by Duminil–Copin–Li–Manolescu for a broad class of two-dimensional random-cluster models, and (ii) a short proof of the symmetry breaking in a manner similar to the recent structural proof by Ray–Spinka of the discontinuity of the phase transition for Q> 4. Altogether, the quantum manifestation of the change between Q= 4 and Q> 4 is a transition from a gapless ground-state to a pair of gapped and extensively distinct ground-states.
All Science Journal Classification (ASJC) codes
- Nuclear and High Energy Physics
- Statistical and Nonlinear Physics
- Mathematical Physics