“…A Cu H complex with D 3 symmetry, such as [Cu(phen)a] 2+, has an 2E electronic ground state and is susceptible to Jahn-Teller distoi'tion (Jotham & Kettle, 1971). If one of the phen groups is replaced by a chelating OXO-group, the resulting symmetry is C2 and the electronic degeneracy is lifted: the 2E term splits into a 2.4 ground state and a 2B excited state (Procter, Clifford, Counihan, Fitzgerald, Serf, Simmons, Tyagi & Hathaway (1982); (3) Simmons, Alcock, ; (4) this work; (5) ; (6) Walsh, Walsh, Murphy & Hathaway (1981); (7) ; (8) Simmons, Clearfield, Fitzgerald, Tyagi & Hathaway (1983); (9) Fitzgerald & Hathaway (1981); (10) Hathaway (1983); (I 1) Escobar & Wittke (1983); (12) Fereday, Hodgson, Tyagi & Hathaway (1981);Nakai (1980 Hathaway, Billing, Dudley & Nicholls, 1969 (Bersuker, 1975;Burdett, 1980). Thus, an isolated [Cu(phen or bpy)2(OXO)] + cation is unsusceptible to distortion unless a vibronic coupling of the 2A and 2B electronic states occurs, in which case static C2 symmetry cannot be retained.…”