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Topics in Current Chemistry

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Electronic Spectroscopy and Photoreactivity of Transition Metal Complexes 133<br />

proaches but cases where current exchange-correlation functionals dramatically<br />

fail are known to exist [94, 95].<br />

The calculated dipole transition moments are very sensitive to the quality<br />

of the calculation, namely the basis sets and the functional used [96]. Obviously<br />

they rely on the hypothesis that DFT excited states are well def<strong>in</strong>ed, an<br />

assumption which is not always true as expla<strong>in</strong>ed above. Some functionals<br />

have been found to be more sensitive to the basis set quality than others.<br />

2.5<br />

Potential Energy Surfaces<br />

In pr<strong>in</strong>ciple photochemical mechanisms are described by reaction paths on<br />

ground and excited states PES which can be determ<strong>in</strong>ed accord<strong>in</strong>g to the<br />

procedures developed for chemical reactivity. The new problem <strong>in</strong> photo-<strong>in</strong>duced<br />

mechanisms is the complicated landscape of the PES characterized by<br />

the presence of a variety of critical geometries such as m<strong>in</strong>ima, transition<br />

states, high-order saddle po<strong>in</strong>ts, avoided cross<strong>in</strong>gs, conical <strong>in</strong>tersections result<strong>in</strong>g<br />

from non-adiabatic <strong>in</strong>teractions between N-Dimensional PES. For a<br />

given atomic basis set the computational method used to solve the electronic<br />

problem has to be flexible enough to characterize correctly different regions<br />

of the molecular PES at the same level of accuracy. An <strong>in</strong>adequate wave<br />

function would result <strong>in</strong> a biased description of the different regions and<br />

such computed PES would not reproduce the exact BO potentials.<br />

One of the most significant advances made <strong>in</strong> applied quantum chemistry<br />

<strong>in</strong> the past 20 years is the development of computationally workable<br />

schemes based on the analytical energy derivatives able to determ<strong>in</strong>e stationary<br />

po<strong>in</strong>ts, transition states, high-order saddle po<strong>in</strong>ts and conical <strong>in</strong>tersections<br />

on multidimensional PES [8]. The determ<strong>in</strong>ation of equilibrium geometries,<br />

transition states and reaction paths on ground state potentials has<br />

become almost a rout<strong>in</strong>e at many levels of calculation (SCF, MP2, DFT, MC-<br />

SCF, CCSD, CI) for molecular systems of chemical <strong>in</strong>terest [97, 98]. The<br />

availability of reliable and efficient analytic energy gradient procedures (first<br />

and second derivative) for the search of various critical po<strong>in</strong>ts on several <strong>in</strong>teract<strong>in</strong>g<br />

complex surfaces at high correlated level (CASSCF, CCSD(T) and<br />

its extension EOM-CCSD, MR-CI) will have a significant impact <strong>in</strong> the theoretical<br />

study of transition metal photo-reactivity. Indeed, although reaction<br />

paths are uniquely def<strong>in</strong>ed <strong>in</strong> any coord<strong>in</strong>ate system they cannot be determ<strong>in</strong>ed<br />

unambiguously without the knowledge of reference po<strong>in</strong>ts on the PES<br />

from which the analytical energy derivation procedure may start. Unfortunately<br />

the derivative formulation for highly correlated wave functions is very<br />

complex and if analytical first derivatives are available for the standard<br />

methods second derivatives calculations are even more complicated.<br />

Density functional methods are competitive with the above traditional<br />

wave functions methods for numerous applications among them the compu-

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