“…On the basis of a new magnetic ordering model (MOIF model) proposed by our group [17][18][19][20], we have successfully fitted the magnetic moments per formula of samples of Cr x Fe 3 À x O 4 (0.0r xr1.0) [17], Cr x Co 1 À x Fe 2 O 4 (0.0rx r1.0) [18], Cu x1 Cr x2 Fe 3 À x1 À x2 O 4 (0.0 rx 1 r0.284 with 1.04 Zx 2 Z0.656) [19], Cr x Ni 1 À x Fe 2 O 4 (0.0rx r0.3) [20] and Ni 0.68 À 0.8x Ti x Fe 2.32 À 0.2x O 4 (0 rx r0.312) [21] using the quantum mechanical potential barrier model (QMPB method) also earlier proposed by our group [22][23][24][25]. In the fitting process, we assumed that the magnetic moments of Cr 2 þ , Cr 3 þ and Mn 3 þ cations (number of 3d electrons, n d r4) were antiparallel to those of the Fe, Co, Ni, Cu cations and Mn 2 þ cations (n d Z5) whether at the (A) sites or the [B] sites, due to the fact that the spin directions of 3d electrons in the cations are constrained by Hund's rules.…”