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Photochemistry and Photophysics of Coordination Compounds

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20 V. Balzani et al.<br />

where H el <strong>and</strong> FC el are the electronic coupling <strong>and</strong> the Franck–Condon density<br />

<strong>of</strong> states, respectively.<br />

In the absence <strong>of</strong> any intervening medium (through-space mechanism),<br />

the electronic factor decreases exponentially with increasing distance:<br />

H el = H el �<br />

(0) exp – βel<br />

2<br />

� �<br />

rAB – r0<br />

�<br />

, (26)<br />

where rAB is the donor–acceptor distance, H el (0) is the interaction at the “contact”<br />

distance r0,<strong>and</strong>β el is an appropriate attenuation parameter.<br />

For donor–acceptor components separated by vacuum, β el is estimated to<br />

be in the range 2–5 ˚A –1 . When donor <strong>and</strong> acceptor are separated by “matter”<br />

(e.g., a bridge L), the electronic coupling can be mediated by mixing <strong>of</strong><br />

the initial <strong>and</strong> final states <strong>of</strong> the system with virtual, high-energy electrontransfer<br />

states involving the intervening medium (superexchange mechanism)<br />

[60, 61].<br />

The FC el term <strong>of</strong> Eq. 25 is a thermally averaged Franck–Condon factor connecting<br />

the initial <strong>and</strong> final states. In the high temperature limit (hν

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