“…In the conventional spinwave scheme, the spin deviations in each sublattice diverge in the one-dimensional (1D) antiferromagnets, but the quantum as well as thermal divergence of the number of bosons can be overcome in the Takahashi scheme [17] that will be applied to the present antiferromagnetic F-F-AF chain. The AF-AF-F chain is a ferrimagnet, whose magnetization should be nonzero in the ground state but zero at finite temperature, leading to that we can apply the Yamamoto scheme [21,22], where the Lagrange multiplier was introduced directly in the free energy, to our present ferrimagnetic AF-AF-F chain. The detail derivations of the MSW formalism are collected in Appendix A, where the linear modified spin-wave (LMSW) theory, which is up to the order of O(S 1 ), and the perturbational interacting modified spin-wave (PIMSW) theory, which is up to the order of O(S 0 ), are included.…”