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Photochemistry and Photophysics of Coordination Compounds

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<strong>Photochemistry</strong> <strong>and</strong> <strong>Photophysics</strong> <strong>of</strong> <strong>Coordination</strong> <strong>Compounds</strong>: Chromium 41<br />

total phosphorescence quenching is accompanied by significant but less than<br />

total reaction quenching. Definitively establishing the precise role <strong>of</strong> the<br />

doublet level in this quenched reaction component has proven an elusive<br />

goal, with competing options including direct 2 Eg reaction, 2 Eg tunneling to<br />

a ground state intermediate (GSI) surface, or “delayed” quartet excited state<br />

reaction via thermally activated 2 Eg → 4 T2g back-intersystem crossing, BISC<br />

(Fig. 2).<br />

This debate has been exhaustively discussed elsewhere [4, 6, 23, 24], <strong>and</strong><br />

will not be a focus <strong>of</strong> this review. From the outset, it was appreciated that<br />

the 4 T2g level <strong>of</strong> (t2g) 2 (eg) 1 orbital parentage was an attractive c<strong>and</strong>idate for<br />

substitution chemistry, based on the occupation <strong>of</strong> an eg orbital which is σ ∗<br />

antibonding with respect to the metal–lig<strong>and</strong> (M – L) bond. At present, the<br />

most widely employed theoretical model for rationalizing Cr(III) photosubstitution<br />

behavior, assuming quartet reactivity, is the semi-empirical symmetry<br />

restricted angular overlap model (AOM) developed by Vanquickenborne<br />

<strong>and</strong> Ceulemans [25–27]. For mixed lig<strong>and</strong> systems it has had considerable<br />

success in predicting relative lig<strong>and</strong> labilities based on identifying the plane<br />

<strong>of</strong> labilization <strong>and</strong> assuming that the lig<strong>and</strong> with the smallest excited state<br />

M – L bond strength is preferentially substituted. A further strength <strong>of</strong> the<br />

model is the rationalization it provides for the stereochemical change that<br />

is a common feature <strong>of</strong> Cr(III) photochemistry (in contrast to their corresponding<br />

thermal behavior), especially for cases <strong>of</strong> axial lig<strong>and</strong> loss in mixed<br />

lig<strong>and</strong> systems <strong>of</strong> D4h or C4v symmetry [4, 28]. A more recent ab initio study<br />

<strong>of</strong> the photochemistry <strong>of</strong> Cr(III) ammine systems yielded results in good<br />

agreement with the earlier AOM calculations [29]. Tris-polypyridyl Cr(III)<br />

complexes may prove to be an exception to this apparent preference for quartet<br />

excited state reactivity. Early quenching studies on [Cr(phen)3] 3+ (where<br />

phen = 1,10-phenanthroline) revealed up to 95% reaction quenching in the<br />

presence <strong>of</strong> doublet quenchers such as I – <strong>and</strong> NCS – [30, 31], <strong>and</strong> the data from<br />

subsequent <strong>and</strong> more detailed investigations were most readily interpreted in<br />

terms <strong>of</strong> a direct doublet excited state reaction pathway [32–34].<br />

The remaining sections <strong>of</strong> this chapter are devoted to a discussion <strong>of</strong> developments<br />

since December 1998 in a range <strong>of</strong> different focus areas <strong>of</strong> Cr(III)<br />

photochemistry <strong>and</strong> photophysics. For convenience, the state term symbols<br />

for Oh symmetry shown in Fig. 2 are usually employed during these discussions.<br />

3<br />

Ultrafast Dynamics <strong>of</strong> Cr(III) Lig<strong>and</strong> Field Excited States<br />

Ultrafast time-resolved absorption spectroscopy constitutes one <strong>of</strong> the most<br />

exciting <strong>and</strong> promising new frontiers in transition metal photochemistry <strong>and</strong><br />

photophysics. The term ultrafast is applied to photoprocesses that occur on

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