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Topics in Current Chemistry

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Electronic Spectroscopy and Photoreactivity of Transition Metal Complexes 121<br />

fer, Sigma-Bond-to-Ligand-Charge-Transfer, Intra-Ligand, Ligand-to-Metal-<br />

Charge-Transfer). The presence of electronic states of different nature, localisation,<br />

dynamics and reactivity <strong>in</strong> a limited doma<strong>in</strong> of energy gives to this<br />

class of molecules unconventional photophysical and photochemical properties<br />

and expla<strong>in</strong>s the versatility and the richness of their photochemistry [1,<br />

2]. Moreover these specific properties responsible for the occurrence under<br />

irradiation of fundamental physico-chemical processes such as electron/energy<br />

transfer, bonds break<strong>in</strong>g or formation, isomerisation, radicals formation,<br />

lum<strong>in</strong>escence can be tailored chemically and more recently controlled<br />

by shaped laser pulses [3]. Two contrasted behaviours can be considered: after<br />

irradiation the molecular system can either be trapped <strong>in</strong> long-lived excited<br />

states of well def<strong>in</strong>ed structure lead<strong>in</strong>g to beautiful resolved absorption/emission<br />

spectroscopy or land on repulsive potential energy surfaces<br />

<strong>in</strong>duc<strong>in</strong>g extremely fast ligand dissociation <strong>in</strong> femtosecond time-scale. The<br />

bipyrid<strong>in</strong>e substituted complexes <strong>in</strong>tensively studied over the last 30 years<br />

are representative of the first category [4] whereas transition metal carbonyls<br />

illustrate the second behaviour [5, 6]. Most of the time bound and repulsive<br />

electronic excited states coexist <strong>in</strong> a limited doma<strong>in</strong> of energy and<br />

may <strong>in</strong>terfere <strong>in</strong> the Franck-Condon region generat<strong>in</strong>g structureless absorption<br />

spectra. The <strong>in</strong>teraction between various electronic states <strong>in</strong> different<br />

regions of the potential energy surfaces leads to critical geometrical structures<br />

such as saddle po<strong>in</strong>ts, conical <strong>in</strong>tersections or local m<strong>in</strong>ima. Consequently<br />

the observed response to the light of the molecular system is entirely<br />

governed by the sequence of many concurrent elementary processes. The<br />

development of short time resolved spectroscopy [7] (picoseconds–femtoseconds<br />

time-scale) <strong>in</strong> different doma<strong>in</strong>s (resonance Raman, FT-Infra-<br />

Red, FT-Electron Paramagnetic Resonance, emission, absorption UV/visible)<br />

has contributed to a better understand<strong>in</strong>g of excited states structures<br />

and processes that are very fast even at low temperature. However several<br />

fundamental questions still rema<strong>in</strong> to be solved. One important aspect is the<br />

differentiation between i) chemically active electronic states lead<strong>in</strong>g to<br />

bonds break<strong>in</strong>g or formation, isomerisation, radicals production and ii)<br />

long-lived excited states <strong>in</strong>volved <strong>in</strong> the photophysics or subsequent secondary<br />

processes such as electron/energy transfer. The photo-<strong>in</strong>duced reactivity<br />

<strong>in</strong> transition metal complexes is characterized by the occurrence of several<br />

schemes of fragmentation orig<strong>in</strong>ated <strong>in</strong> complicated mechanisms. These<br />

mechanisms <strong>in</strong>volve different electronic states and various reaction paths<br />

and elementary processes such as direct/<strong>in</strong>direct dissociation, <strong>in</strong>ternal conversion<br />

or <strong>in</strong>tersystem cross<strong>in</strong>g. The simulation of the dynamics follow<strong>in</strong>g<br />

the photon absorption is not an easy task and two different situations have<br />

to be considered: i) ultra-fast direct dissociation from the absorb<strong>in</strong>g state itself<br />

(adiabatic process); ii) <strong>in</strong>direct dissociation via <strong>in</strong>ternal conversion or<br />

<strong>in</strong>tersystem cross<strong>in</strong>g (non-adiabatic process). A third case, not contemplated

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