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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 161<br />

chromophore <strong>and</strong> interconversion between the initially prepared S3 state<br />

<strong>and</strong> the low-lying S1 level within the pyrenyl subunits have also been evidenced.<br />

The rate constant <strong>of</strong> the energy transfer from the pyrenyl groups<br />

to the Ru/Os excited state manifold is in good agreement with the Förster<br />

mechanism when the relaxed S1 pyrene state is taken into account. Energy<br />

transfer from the nonrelaxed state most likely involves folded conformations<br />

in which the pyrenyl subunits are strongly interacting with inner subunits <strong>of</strong><br />

the tetranuclear core. Such interactions were also suggested by the groundstate<br />

absorption spectrum <strong>of</strong> the compound [272].<br />

Because octahedral metal complexes can exist in two chiral forms, Λ <strong>and</strong><br />

∆, it could be expected that the photophysical properties <strong>of</strong> dendrimers<br />

containing metal complexes as branching centers could be different for the<br />

various isomers (the situation can be even more complicated in the case <strong>of</strong><br />

geometrical isomers). However, the investigation <strong>of</strong> optically pure isomers <strong>of</strong><br />

dinuclear <strong>and</strong> dendritic-shaped tetranuclear species (37 is the general structural<br />

formula <strong>of</strong> the tetranuclear systems: optical geometry is not evidenced)<br />

has shown that stereochemical isomerism does not cause any sizeable difference,<br />

at least for the studied compounds [194].<br />

In 37 the emissive state, which involves the peripheral Ru(II) centers, does<br />

not have a sizeable absorption counterpart, since it is a special type <strong>of</strong> chargeseparated<br />

state, with the formal “hole” localized on a peripheral Ru(II) center<br />

<strong>and</strong> the “electron” localized on an orbital mainly centered on the pyrazine<br />

moiety <strong>of</strong> the bridging lig<strong>and</strong>: the absorption related to such a state has negligible<br />

oscillator strength, due to the poor overlap <strong>of</strong> the orbitals involved

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