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Photochemistry and Photophysics of Coordination Compounds

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8 V. Balzani et al.<br />

(Fig. 5). For most Cr(III) complexes, e.g., for [Cr(NH3)6] 3+ ,thelowest-energy<br />

transition is metal centered <strong>and</strong> the resulting πM(t2g) 2 σ ∗ M (eg) configuration<br />

gives rise to 4 T2g <strong>and</strong> 4 T1g excited states (Fig. 5). Several other coordination<br />

compounds, including the complexes <strong>of</strong> the lanthanide ions, have an openshell<br />

ground-state configuration <strong>and</strong>, as a consequence, a ground state with<br />

high-multiplicity <strong>and</strong> low-energy intraconfigurational metal-centered excited<br />

states.<br />

Fig. 5 Configurations (a) <strong>and</strong>state(b) diagrams for an octahedral Cr(III) complex. Only<br />

the lower-lying excited states <strong>of</strong> each configuration are shown [20]<br />

In conclusion, metal complexes tend to have more complex <strong>and</strong> specific<br />

Jablonski diagrams than organic molecules. Points to be noticed are: (1) spin<br />

multiplicity other than singlet <strong>and</strong> triplet can occur, but for each electronic<br />

configuration the state with highest multiplicity remains the lowest one;<br />

(2) excited states can exist that belong to the same configuration <strong>of</strong> the ground<br />

state (this implies that the ground state has the highest multiplicity); <strong>and</strong><br />

(3) more than one pair <strong>of</strong> states <strong>of</strong> different multiplicity can arise from a single<br />

electron configuration. In the following, in order to discuss some general<br />

concept <strong>of</strong> molecular photochemistry we will make use <strong>of</strong> a generic Jablonski<br />

diagram based on singlet <strong>and</strong> triplet states.<br />

2.3<br />

Light Absorption <strong>and</strong> Intramolecular Excited-State Decay<br />

Figure 6 shows a schematic energy level diagram for a generic molecule [23].<br />

In principle, transitions between states having the same multiplicity are allowed,<br />

whereas those between states <strong>of</strong> different multiplicity are forbidden.<br />

Therefore, the electronic absorption b<strong>and</strong>s observed in the UV–visible spec-

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