Photochemistry and Photophysics of Coordination Compounds
Photochemistry and Photophysics of Coordination Compounds
Photochemistry and Photophysics of Coordination Compounds
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94 N. Armaroli et al.<br />
tionalized derivative. The combined effect <strong>of</strong> these two factors (kinetic <strong>and</strong><br />
thermodynamic) can explain the different <strong>and</strong> unexpected trend in photoprocesses<br />
<strong>of</strong> multicomponent arrays containing Cu(I)-phenanthrolines linked to<br />
methan<strong>of</strong>ullerenes vs. bismethan<strong>of</strong>ullerenes, which has been found in a variety<br />
<strong>of</strong> molecular architectures such as dendrimers [38], rotaxanes [98] <strong>and</strong><br />
s<strong>and</strong>wich-type dyads [110].<br />
Exhaustive review articles presenting photophysical investigations on<br />
fullerene- <strong>and</strong> porphyrin-type arrays built-up around [Cu(NN)2] + centers<br />
have been published recently <strong>and</strong> we suggest the reader refers to these papers<br />
for a comprehensive <strong>and</strong> updated overview on this topic [15, 25, 111, 112].<br />
2.6<br />
Bimolecular Quenching Processes<br />
Excited state electrochemical potentials can be obtained from the ground<br />
state monoelectronic electrochemical potentials <strong>and</strong> the spectroscopic energy<br />
(E ◦◦ in eV units, to be considered divided by a unitary charge) related to the<br />
involved transition, according to Eqs 2 <strong>and</strong> 3 [6]:<br />
E(A + / ∗ A)=E(A + /A)–E ◦◦<br />
E( ∗ A/A – )=E(A/A – )+E ◦◦<br />
Hence the variation <strong>of</strong> the electron-donating or accepting capability <strong>of</strong> a given<br />
molecule A, upon light excitation, can be easily assessed. In Eqs 2 <strong>and</strong> 3: ∗ A<br />
denotes the lowest-lying electronically excited state <strong>of</strong> A <strong>and</strong> its spectroscopic<br />
energy (E ◦◦ ) can be estimated from the onset <strong>of</strong> emission spectra [6].<br />
Oxidation from Cu(I) to Cu(II) is easily accomplished <strong>and</strong> the MLCT<br />
excited states <strong>of</strong> Cu(I)-bisphenanthrolines are, therefore, potent reductants.<br />
For example [Cu(3)2] + is a more powerful reductant than the very popular<br />
photosensitizer [Ru(bpy)3] 2+ (A + /A = – 1.11 <strong>and</strong> – 0.85 V, respectively)<br />
owing to its more favorable ground state 2+/+ potential (+ 0.69 vs. + 1.27 V),<br />
that largely compensates the lower content <strong>of</strong> excited state energy (1.80 vs.<br />
2.12 eV) [15]. By contrast reduction <strong>of</strong> Cu(I)-bisphenanthrolines is strongly<br />
disfavored <strong>and</strong> they are mild excited state oxidants; accordingly, only a few examples<br />
<strong>of</strong> reductive quenching <strong>of</strong> [Cu(NN)2] + complexes are reported in the<br />
literature, with ferrocenes as donors [113, 114].<br />
Oxidative quenching <strong>of</strong> [Cu(NN)2] + ’s by Co(III) <strong>and</strong> Cr(III) complexes as<br />
well as nitroaromatic compounds <strong>and</strong> viologens has been reported <strong>and</strong> comprehensively<br />
reviewed [115]. Some attempts to sensitize wide b<strong>and</strong>-gap semiconductors<br />
with Cu(I) complexes were also carried out [115] but so far they<br />
do not seem to be competitive in terms <strong>of</strong> stability <strong>and</strong> efficiency with those<br />
based on Ru(II) complexes [12]. Energy transfer quenching to molecules<br />
possessing low-lying triplets such as anthracene has been demonstrated via<br />
transient absorption spectroscopy [116, 117], whereas oxygen quenching,<br />
(2)<br />
(3)