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Photochemistry and Photophysics of Coordination Compounds

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22 V. Balzani et al.<br />

between the emission spectrum <strong>of</strong> the donor <strong>and</strong> the absorption spectrum <strong>of</strong><br />

the acceptor.<br />

The electronic factor H en is a two-electron matrix element involving the<br />

HOMOs <strong>and</strong> LUMOs <strong>of</strong> the energy–donor <strong>and</strong> energy–acceptor components.<br />

By following st<strong>and</strong>ard arguments [20, 23], this factor can be split into two<br />

additive terms, a coulombic term <strong>and</strong> an exchange term. The two terms depend<br />

differently on the parameters <strong>of</strong> the system (spin <strong>of</strong> ground <strong>and</strong> excited<br />

states, donor–acceptor distance, etc.) <strong>and</strong> each <strong>of</strong> them can become predominant<br />

depending on the specific system <strong>and</strong> experimental conditions.<br />

The orbital aspects <strong>of</strong> the two mechanisms are schematically represented in<br />

Fig. 13.<br />

Fig. 13 Pictorial representation <strong>of</strong> the coulombic <strong>and</strong> exchange energy-transfer mechanisms<br />

4.4.1<br />

Coulombic Mechanism<br />

The coulombic (also called resonance, Förster-type [71], or through-space)<br />

mechanism is a long-range mechanism that does not require physical contact<br />

between donor <strong>and</strong> acceptor. It can be shown that the most important<br />

term within the coulombic interaction is the dipole–dipole term, which obeys<br />

the same selection rules as the corresponding electric dipole transitions <strong>of</strong><br />

the two partners ( ∗ A → A<strong>and</strong>B→ ∗ B, Fig. 13). Therefore, coulombic energy<br />

transfer is expected to be efficient in systems in which the radiative transitions<br />

connecting the ground <strong>and</strong> the excited states <strong>of</strong> each partner have high<br />

oscillator strength. The rate constant for the dipole–dipole coulombic energy

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