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Photochemistry and Photophysics of Coordination Compounds

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54 N.A.P. Kane-Maguire<br />

reaction sequence shown in Scheme 1. In this scheme, the long-lived <strong>and</strong><br />

short-lived Cr(III) species are labeled CrL <strong>and</strong> CrS, respectively, while kET<br />

<strong>and</strong> k–ET are the corresponding rate constants for forward <strong>and</strong> reverse energy<br />

transfer. Likewise, the terms kL <strong>and</strong> kS are the reciprocals <strong>of</strong> the lifetimes <strong>of</strong><br />

CrL <strong>and</strong> CrS, respectively, in the absence <strong>of</strong> energy transfer. Emission quenching<br />

<strong>of</strong> CrL <strong>and</strong> CrS couldthenbefollowedbyanalyzingthedecaypr<strong>of</strong>ile<br />

following pulsed excitation according to the mathematical formulation developed<br />

by Maharaj <strong>and</strong> Winnik [95].<br />

For the trans-dicyano <strong>and</strong> trans-diammine systems, energy transfer rate<br />

constants at 20 ◦ C(µ = 1.0) were determined to be kET ≫ 7 × 10 6 M –1 s –1<br />

<strong>and</strong> 9.7 × 10 6 M –1 s –1 , respectively. However, for trans-[Cr(tet a)F2] + no<br />

energy transfer was observed, which implied that the rate constant was<br />

≪ 3 × 10 5 M –1 s –1 . Analysis <strong>of</strong> these results using Marcus theory lead to<br />

the important conclusion that electronic effects play a significant role in<br />

determining the rates <strong>of</strong> energy transfer self-exchange for these series <strong>of</strong><br />

complexes.<br />

7<br />

Photoredox Behavior <strong>of</strong> [Cr(diimine)3] 3+ Systems<br />

Arguably, the seminal report by Gafney <strong>and</strong> Adamson in 1972 [96] that the<br />

3 MLCT excited state <strong>of</strong> [Ru(bpy)3] 2+ (where bpy is 2,2 ′ -bipyridine) could<br />

function as an electron transfer agent was the catalytic event that led to the<br />

extraordinary growth <strong>of</strong> transition metal photochemistry <strong>and</strong> photophysics<br />

over the last three decades [94, 97–99]. Today, the polypyridyl compounds<br />

<strong>of</strong> Ru(II) still hold a favored status, due to a coalescence <strong>of</strong> desirable properties<br />

including an intense, relatively long-lived luminescence signature, <strong>and</strong><br />

a remarkable thermal robustness in a range <strong>of</strong> oxidation states.<br />

The analogous polypyridyl complexes <strong>of</strong> Cr(III) are the next most investigated<br />

[M(diimine)3] n+ systems. A few years after the Gafney <strong>and</strong> Adamson<br />

article appeared, Bolletta et al. presented the first evidence that the lig<strong>and</strong>field<br />

2 Eg excited state <strong>of</strong> [Cr(bpy)3] 3+ was a strong one-electron photooxidant<br />

[100]. This involvement <strong>of</strong> polypyridyl Cr(III) species in direct bimolecular<br />

electron transfer reactions <strong>of</strong> the generic type represented in Eq. 1 has<br />

since been thoroughly documented for numerous substrates, Q [101–106]:<br />

( 2 Eg)Cr 3+ +Q→ Cr 2+ +Q + . (1)<br />

Importantly, [Cr(diimine)3] 3+ complexes are more powerful photooxidants<br />

than their [Ru(diimine)3] 2+ analogs. The oxidizing power <strong>of</strong> the Cr(III) 2 Eg<br />

excited state can be assessed from the value <strong>of</strong> the 2 Eg excited state reduction<br />

potential, E o ( ∗ Cr 3+ /Cr 2+ ). It has been shown [102, 103] that this latter quantity<br />

can be reliably estimated from the difference between the 2 Eg → 4 A2g

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