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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> 9<br />

Fig. 6 Schematic energy level diagram for a generic molecule<br />

trum <strong>of</strong> such a generic molecule would display b<strong>and</strong>s corresponding to the<br />

S0 → Sn transitions <strong>of</strong> the diagram. For metal complexes, which usually are<br />

highly symmetric species, symmetry selection rules can also play a role in determining<br />

the intensity <strong>of</strong> the absorption b<strong>and</strong>s. Furthermore, the presence <strong>of</strong><br />

a heavy atom (namely, the metal) relaxes the spin-conservation rule.<br />

The excited states are unstable species that decay not only by intramolecular<br />

chemical reactions (e.g., dissociation, isomerization) but also (actually,<br />

more <strong>of</strong>ten) by intramolecular radiative <strong>and</strong> nonradiative deactivations.<br />

When a species is excited to upper spin-allowed excited states, it usually<br />

undergoes a fast <strong>and</strong> 100% efficient radiationless deactivation (internal conversion,<br />

ic) to the lowest spin-allowed excited (S1 in Fig. 6). Setting aside the<br />

intramolecular photochemical processes, such an excited state undergoes deactivation<br />

via three competing first-order processes: nonradiative decay to the<br />

ground state (internal conversion, rate constant kic); radiative decay to the<br />

ground state (fluorescence, kfl); <strong>and</strong> intersystem crossing (isc) to the lowest<br />

triplet state T1 (kisc). In its turn, T1 can undergo deactivation via nonradiative<br />

(intersystem crossing, k ′ isc ) or radiative (phosphorescence, kph) decayto<br />

the ground state S0. When the species contains heavy atoms, as in the case<br />

<strong>of</strong> metal complexes, the formally forbidden intersystem crossing <strong>and</strong> phosphorescence<br />

processes become faster. The lifetime (τ) <strong>of</strong> an excited state, i.e.,<br />

the time needed to reduce the excited-state concentration by 2.718, is given

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