“…The origin of the unexpected long lifetime of the charge-separated pyr •– –Zr IV –O–Co III state is most likely crossing to a spin-forbidden state. , Our earlier study of TiOMn centers explored spin crossover in binuclear units; we proposed that the transient d 1 metal center was the most likely site of the spin crossover because it is the conserved feature of a variety of different metal combinations with long-lifetime MMCT states . In ZrOCo–pyr, there is no obvious barrier that would require the electron to remain at the zirconium center to undergo spin crossover before reducing the pyridine; as the spin–orbit coupling of cobalt is higher than that of pyridine, spin crossover at cobalt is considered more likely. − Cobalt is known to undergo spin crossover on the ultrafast time scale in a variety of oxidation states, geometries, and phases, ,− including in our previous works with organometallic systems. , In particular, this phenomenon has been characterized in great detail in photoinduced magnetization due to metal-to-metal charge transfer states in Prussian blue analogues. ,− As in those analogues, Co III is commonly found in an octahedral configuration, taking on a tetrahedral geometry when required by ligand steric constraints, as in the tungsten oxide matrices discussed earlier or with ligands like benzene dithiolates. , Tetrahedral cobalt centers are most frequently high-spin but display a low-spin ground state with strong-field norbornyl or phosphanido ligands. , Based on this information, we propose that the long lifetime of the pyr •– –Zr IV –O–Co III state is the result of spin crossover from the original optically formed quartet state to a doublet state. Our tetrahedral Co III forms in the high-spin state ( S = 1) alongside Zr III ( S = 1/2).…”