“…For the insulators and semiconductors, the charge carriers cannot freely move and are localized on the donor layers, providing various magnetic ground states. The range of ground states include antiferromagnetic and canted ferromagnetic orderings, spin density wave, 1D and 2D Heisenberg magnets, and compounds characterized by a singlet–triplet model . The magnetic moment is not localized in an atomic orbital, as in transition-metal magnets, and not localized in a specific part of a molecule, as in organic radicals, but is delocalized across a whole BEDT-TTF molecule.…”