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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>: Ruthenium 185<br />

nected rings is obtained (66). Heating regenerates the starting catenane. The<br />

process can be repeated at will, since both the reactions (coordination <strong>and</strong><br />

decoordination) are quantitative. It can be noted that in this system the photosubstitution<br />

process, usually considered as an undesired property for Ru(II)<br />

complexes, is instead used to perform the desired function. More recently,<br />

light-induced motion on a rotaxane system has also been obtained by using<br />

the same strategy [361].<br />

6<br />

Ruthenium Complexes <strong>and</strong> Biological Systems<br />

The effects <strong>of</strong> the interaction <strong>of</strong> photoactive ruthenium complexes with biological<br />

structures have been extensively studied. Because <strong>of</strong> the outst<strong>and</strong>ing<br />

excited-state properties <strong>of</strong> Ru(II) polypyridine complexes, these systems<br />

have been employed as probes <strong>of</strong> biological sites, as well as photocleavage<br />

agents <strong>and</strong>, in recent times, as inhibitors <strong>of</strong> biological functions [362–369].<br />

Among the species used as luminescent probes, one <strong>of</strong> the most studied compounds<br />

in the last 15 years is 67 [200–204, 362–379]. This complex is very<br />

weakly emissive in aqueous solution, but becomes strongly emitting in the<br />

presence <strong>of</strong> DNA, giving rise to the so-called light-switch effect [200, 201].<br />

The reason for such a behavior lies in the electronic properties <strong>of</strong> this specific<br />

chromophore <strong>and</strong> in the intercalation ability <strong>of</strong> the dipyrido[3,2-a:2 ′ ,3 ′ -<br />

c]phenazine (dppz) lig<strong>and</strong>. In this species, there are several triplet excited<br />

states quite close in energy: (1) a MLCT state directly populated by light excitation,<br />

in which the excited electron resides in the LUMO+1 centered on<br />

the “bpy-like” portion <strong>of</strong> dppz lig<strong>and</strong>; (2) a MLCT state in which the excited<br />

electron is located in the LUMO centered on the “phenazine-like” portion <strong>of</strong><br />

the dppz lig<strong>and</strong>; <strong>and</strong> (3) a lig<strong>and</strong>-centered (dppz-based) excited state. This<br />

compound represents another example <strong>of</strong> interplay between multiple MLCT<br />

states, discussed in more detail in Sect. 4.4. The energy gap <strong>and</strong> order <strong>of</strong> the<br />

three low-lying excited states mentioned above, as well as their dynamics,<br />

can be modulated by various parameters, including solvent dielectrics, protic<br />

ability <strong>of</strong> the solvent, <strong>and</strong> hydrophobic interactions. In a simplified schema-

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