11.01.2013 Views

Photochemistry and Photophysics of Coordination Compounds

Photochemistry and Photophysics of Coordination Compounds

Photochemistry and Photophysics of Coordination Compounds

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!