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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> 11<br />

energy transfer:<br />

∗ A+B→ A + +B –<br />

∗ A+B→ A – +B +<br />

oxidative electron transfer (6)<br />

reductive electron transfer (7)<br />

∗ ∗<br />

A+B→ A+ B energy transfer . (8)<br />

Bimolecular electron- <strong>and</strong> energy-transfer processes are important because<br />

they can be used (1) to quench an electronically excited state, i.e., to prevent<br />

its luminescence <strong>and</strong>/or intramolecular reactivity, <strong>and</strong> (2) to sensitize other<br />

species, for example, to cause chemical changes <strong>of</strong>, or luminescence from,<br />

species that do not absorb light.<br />

Simple kinetic arguments show that only the excited states that live longer<br />

than ca. 10 –9 s may have a chance to be involved in encounters with other solute<br />

molecules. Usually, in the case <strong>of</strong> metal complexes only the lowest excited<br />

state satisfies this requirement. The kinetic aspects <strong>of</strong> energy- <strong>and</strong> electrontransfer<br />

processes are discussed in detail elsewhere [17, 20, 23]. A point that<br />

must be stressed is that an electronically excited state is a species with quite<br />

different properties compared with those <strong>of</strong> the ground-state molecule. In<br />

particular, because <strong>of</strong> its higher energy content, an excited state is both<br />

a stronger reductant <strong>and</strong> a stronger oxidant than the corresponding ground<br />

state. To a first approximation, the redox potentials <strong>of</strong> the excited-state couples<br />

may be calculated from the potentials <strong>of</strong> the ground-state couples <strong>and</strong> the<br />

one-electron potential corresponding to the zero–zero excited-state energy,<br />

E0–0 , as shown by Eqs. 9 <strong>and</strong> 10 [25]:<br />

E � A + / ∗ A � ≈ E � A + /A � – E 0–0<br />

E � ∗ A/A – � ≈ E � A/A –� + E 0–0 . (10)<br />

3.2<br />

Bimolecular Processes Involving Metal Complexes<br />

From an exhaustive monograph that appeared in 1970 [2] <strong>and</strong> a multiauthored<br />

volume <strong>of</strong> 1975 [26], it clearly appears that most <strong>of</strong> the interest was<br />

then focused on lig<strong>and</strong> photosubstitution reactions, photoredox decomposition,<br />

<strong>and</strong> photoisomerization reactions, while bimolecular processes were<br />

barely investigated. This picture, however, changed pr<strong>of</strong>oundly in a few years<br />

following the extensive work carried out by several research groups on the luminescence<br />

<strong>of</strong> coordination compounds [27–29] <strong>and</strong> the discovery that the<br />

lowest excited state <strong>of</strong> a number <strong>of</strong> Cr(III), Ru(II), <strong>and</strong> Os(II) complexes exhibits<br />

a sufficiently long lifetime in fluid solution to be able to participate<br />

as a reactant in bimolecular reactions [25, 30]. A further advantage <strong>of</strong>fered<br />

by Ru(II) <strong>and</strong> Os(II) bipyridine-type complexes is that they can undergo reversible<br />

redox reactions both in the ground <strong>and</strong> excited state, so they were<br />

soon used as reactants <strong>and</strong>, even more interesting, as mediators, in light-<br />

(9)

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