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Photochemistry and Photophysics of Coordination Compounds

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16 V. Balzani et al.<br />

Fig. 9 Schematic representation <strong>of</strong> excimer <strong>and</strong> exciplex formation in a supramolecular<br />

system<br />

Compared with the “monomer” emission, the emission <strong>of</strong> an excimer or exciplex<br />

is always displaced to lower energy (longer wavelengths) <strong>and</strong> usually<br />

corresponds to a broad <strong>and</strong> rather weak b<strong>and</strong>.<br />

Excimers are usually obtained when an excited state <strong>of</strong> an aromatic<br />

molecule interacts with the ground state <strong>of</strong> a molecule <strong>of</strong> the same type. For<br />

example, between the excited <strong>and</strong> ground states <strong>of</strong> anthracene units. Exciplexes<br />

are obtained when an electron donor (acceptor) excited state interacts<br />

with an electron acceptor (donor) ground-state molecule; for example, between<br />

excited states <strong>of</strong> aromatic molecules (electron acceptors) <strong>and</strong> amines<br />

(electron donors). Excited states <strong>of</strong> coordination compounds are seldom involved<br />

in excimers or exciplexes, since their components (metal <strong>and</strong> lig<strong>and</strong>s)<br />

have already used their electron donor or acceptor properties in forming<br />

the complex. Furthermore, the three-dimensional structure <strong>of</strong> coordination<br />

compounds usually prevents strong electronic interaction with other species.<br />

However, for some square planar complexes excimer emission has long been<br />

reported [54] <strong>and</strong> can indeed be found for some families <strong>of</strong> Au <strong>and</strong> Pt complexes,<br />

as discussed in other chapters <strong>of</strong> this volume.<br />

The working mechanisms <strong>of</strong> a number <strong>of</strong> biological <strong>and</strong> artificial molecular<br />

devices <strong>and</strong> machines are based on photoinduced electron- <strong>and</strong> energytransfer<br />

processes [20, 48, 55]. Since these processes have to compete with<br />

the intrinsic decays <strong>of</strong> the relevant excited states, a key problem is that <strong>of</strong><br />

maximizing their rates. It is therefore appropriate to summarize some basic<br />

principles <strong>of</strong> electron- <strong>and</strong> energy-transfer kinetics. [56].<br />

4.3<br />

Electron Transfer<br />

4.3.1<br />

Marcus Theory<br />

Electron-transfer processes involving excited-state <strong>and</strong>/or ground-state molecules<br />

can be dealt with in the frame <strong>of</strong> the Marcus theory [57] <strong>and</strong> <strong>of</strong> the

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