Abstract
The Heisenberg-Ising Hamiltonian H=12{α(σxσx+σyσy)+ε(σzσz)} for rectangular one-, two-, or three-dimensional lattices are considered. The sum is over nearest neighbors and Δ=εα measures the anisotropy of the coupling. Upper and lower bounds for the ground-state energy are established and these bounds apply equally well to lattices of one, two, or three dimensions. Furthermore, it is shown that the ground-state energy per nearest-neighbor pair is nondecreasing as the dimension of the lattice (one, two or three) increases.