“…These are spinor and spatial constraints, respectively. The MOs of the ROHF state 11 B 1u are taken as starting orbitals for the CASSCF calculations, which means that the ten 3d-like orbitals build up the active space. Since these orbitals belong to the onedimensional irreps a g , a g , b 1u , b 1u , b 1g , a u , b 2u , b 3g , b 3u , and b 2g , the ferromagnetic Sϭ5 state belongs to irrep B 1u .…”