The photophysical properties of the chromophore−quencher complexes, fac-[(4,4‘-R2bpy)ReI(CO)3(LA)]
n
+
(4,4‘-R2bpy = 4,4‘-R2-2,2‘-bipyridine, R = Me or
t
Bu, and LA = the quinone acceptor ligands, benz[g]isoquinoline-5,10-dione (BIQD), 2-oxy-1,4-naphthoquinone anion (ONQ-), 1/2 2,6-dihydroxyanthraquinone
dianion (AFA2-), or the pyridinium acceptor, 1-methyl-6-oxyquinoline (OQD)) in 1,2-dichloroethane are
described. Following ReI → 4,4‘-R2bpy metal-to-ligand charge transfer (MLCT) excitation, intramolecular
electron transfer leads to the transients, fac-[(4,4‘-R2bpy)ReII(CO)3(LA•-)]
n+. They have been characterized
by emission spectral fitting and transient absorption measurements and, for LA = OQD, by transient infrared
measurements. As shown by analysis of excited-state emission, there is weak-to-moderate electronic coupling
between the electron donor and acceptor sites in the transients with H
DA varying from 153 cm-1 for the
BIQD complex to 3.9 cm-1 for the OQD complex. The transients are redox-separated (RS) states with the
electronic configurations dπ5πLA* for BIQD or σ(Re−O)1πLA*1 for ONQ-, AFA
-, and OQD. They are
weak emitters and return to the ground state largely by nonradiative decay which occurs by back electron
transfer (k
ET). Reasonable agreement has been reached between k
ET and values calculated from kinetic
parameters derived by emission spectral fitting and excited-state decay. The RS states for the AFA2- and
OQD complexes are remarkably long-lived (τ = 4 μs for LA = AFA2- in DCE at 296 K and 16 μs for LA
= OQD in DCE at 296 K) due to orbital and spin restrictions on back electron transfer.