Intramolecular electron transfer between Co II (SQ) and Co III (Cat) species has been investigated for the series of complexes Co(py 2 X)(3,6-DBQ) 2, where 3,6-DBQ are semiquinonate and catecholate forms of 3,6-di- tert -butyl-1,2-benzoquinone and py 2 X is bis(pyridine) ether and its heteroatomic analogs with X = S, Se, and Te. Transition temperature for Co(III)/Co(II) redox isomerism decreases in steps of approximately 30 K in toluene solution and in steps of 80 K in the solid state for the complexes with X = S, Se, Te. This appears to be primarily associated with an entropy increase that results from low-energy shifts in vibrational modes with increasing heteroatomic mass. Complexes containing py 2 O have been isolated at room temperature in two charge distributions, Co II (py 2 O)(3,6-DBSQ) 2 and Co III (py 2 O)(3,6-DBSQ)(3,6-DBCat). Crystallographic characterization on both forms of the complex [Co II (py 2 O)(3,6-DBSQ) 2, monoclinic, P 2 1 / c, a = 11.0280(2) Å, b = 30.2750(9) Å, c = 12.1120(2) Å, β = 113.490(2)°, V = 3708.7(1) Å 3, Z = 4, R = 0.056; Co III (py 2 O)(3,6-DBSQ)(3,6-DBCat), monoclinic, P 2 1 / n, a = 9.882(3) Å, b = 20.915(5) Å, c = 17.579(4) Å, β = 91.57(2)°, V = 3632(2) Å 3, Z = 4, R = 0.054] has shown that the py 2 O ligand adopts a planar structure for the Co(II) isomer that shifts to a folded, nonplanar structure with the smaller Co(III) ion. This structural change is responsible for hysteresis in the Co(III) → Co(II) and Co(II) → Co(III) electron transfer steps in the solid state. Optically induced shifts in charge distribution have been investigated using a low-energy polychromatic light source.
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Jung et al. (1997) studied this question.
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