“…The development of spintronic devices requires the generation and control of highly spin-polarized currents or pure spin currents . A way of obtaining a highly spin polarized current is by using a spin filtering effect through ferromagnetic-insulator-ferromagnetic tunnel barriers. , The same effect can be obtained simply by using a ferromagnetic insulating barrier. , However, ferromagnetic insulators (FMI) are very scarce; among the few FMI known double perovskite (DP) oxides, like La 2 NiMnO 6 (LNMO) and La 2 CoMnO 6 , have attracted considerable attention due to their high Curie temperature, T C , and magnetodielectric properties. − In both cases, the ferromagnetic (FM) ordering is explained by superexchange interaction between Mn 4+ and Ni 2+ or Co 2+ according to the Goodenough-Kanamori rules, and it is very sensitive to the ordered distribution of cations in the B-sublattice of the DP structure . In the case of LNMO, cationic order gives rise to 180° ferromagnetic interactions between Ni 2+ (d 8 , t 2g 6 e g 2 , S = 1) and Mn 4+ (d 3 , t 2g 3 e g 0 , S = 3/2) ions and results in a T C very close to RT ( T C ≈ 280 K).…”