“…3 features (a) spin-1 operators S i instead of spin-1/2, (b) a more isotropic exchange term S i • S j , and (c) an additional term for the local onsite anisotropy D. While the TFIC model in Eq. 2 can be studied analytically, the Hamiltonian for NiNb 2 O 6 has been studied numerically by exact diagonalization and density matrix renormalization group methods [52]. Some 'in-between' situations of these two distinct models, including the Blume-Capel model, which deal with (a) and (c) but with an Ising exchange term and without the coupling to external field, can also be rigorously solved [69][70][71][72].…”