The exact solution is given for a linear chain of N atoms of spin {} coupled together by the anisotropic Hamiltonian H=2JΣNi=1[SᵢᶻSᵢ₊₁ᶻ+(1-α)(SᵢˣSᵢ₊₁ˣ+SᵢʸSᵢ₊₁ʸ)]. The energy of the antiferromagnetic ground state is computed and comparison is made with a variational method. The parameter α is allowed to vary between 0 and 1, regulating the relative amount of Ising anisotropy. The short-range order, Σi^SᵢᶻSᵢ₊₁ᶻ, is calculated exactly from the variation of the ground-state energy with α. It is shown that a kink in the short-range order curve calculated using the variational method is fictitious, and the associated discontinuity in ∂²E∂α² is nonexistent. A discussion is given of long-range order and criticisms are presented regarding the predictions of the variational method.
No takes yet. Share an insight, caveat, or question.
R. Orbach (1958) studied this question.
Synapse has enriched 5 related papers. Consider them for comparative context: