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Reviews in Computational Chemistry Volume 18

Reviews in Computational Chemistry Volume 18

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192 Charge-Transfer Reactions <strong>in</strong> Condensed Phases<br />

below). The former route connects the spectral moments to ET activation<br />

parameters (Table 1). The latter is applied to extract off-diagonal matrix elements,<br />

most often the ET matrix element and the transition dipole. Band shape<br />

analysis of optical spectra has been successfully used <strong>in</strong> ET research for many<br />

years, and our present knowledge about mechanisms and energetics of ET orig<strong>in</strong>ates<br />

largely from spectroscopic measurements. 16 The understand<strong>in</strong>g of electronic<br />

and solvent effects on the ET k<strong>in</strong>etics has been recently supplemented<br />

by extensive <strong>in</strong>formation about the <strong>in</strong>tramolecular, vibronic envelope from<br />

resonance Raman spectroscopy. 86<br />

The fast growth of the field of ET research and, especially, the design of<br />

new bridge-coupled donor–acceptor pairs imposes new demands on the theory<br />

of optical spectra. Several major challenges are currently faced by the field.<br />

They may be summarized as follows: (1) The presently exist<strong>in</strong>g band-shape<br />

analysis has been created for ET transitions. 17 It has not anticipated strong<br />

electronic coupl<strong>in</strong>g and thus fails when applied to transitions with high magnitudes<br />

of the ET matrix element. 87 (2) The model is limited to two states only.<br />

Mix<strong>in</strong>g to higher excited states, result<strong>in</strong>g <strong>in</strong> <strong>in</strong>tensity borrow<strong>in</strong>g, is commonly<br />

neglected. Extension to more then two states is especially important for photo<strong>in</strong>duced<br />

CT where a CT state is formed from and is strongly coupled to a<br />

locally exited state of either donor or acceptor unit. 17,88 (3) There are <strong>in</strong>dications<br />

<strong>in</strong> the literature that the common assumption of complete decoupl<strong>in</strong>g<br />

between the <strong>in</strong>tramolecular vibrational modes and solvent thermal motions<br />

may fail for some systems. 89,90 Understand<strong>in</strong>g the orig<strong>in</strong> of and full account<br />

for these effects should be <strong>in</strong>corporated <strong>in</strong>to new models of optical bands.<br />

The challenges outl<strong>in</strong>ed above still await a solution. In this section, we<br />

show how some of the theoretical limitations employed <strong>in</strong> traditional formulations<br />

of the band shape analysis can be lifted. We discuss two extensions of<br />

the present-day band shape analysis. First, the two-state model of CT transitions<br />

is applied to build the Franck–Condon optical envelopes. Second, the<br />

restriction of only two electronic states is lifted with<strong>in</strong> the band shape analysis<br />

of polarizable chromophores that takes higher ly<strong>in</strong>g excited states <strong>in</strong>to account<br />

through the solute dipolar polarizability. F<strong>in</strong>ally, we show how a hybrid model<br />

<strong>in</strong>corporat<strong>in</strong>g the electronic delocalization and chromophore’s polarizability<br />

effects can be successfully applied to the calculation of steady-state optical<br />

band shapes of the optical dye coumar<strong>in</strong> 153 (C153). We first start with a general<br />

theory and outl<strong>in</strong>e the connection between optical <strong>in</strong>tensities and the ET<br />

matrix element and transition dipole.<br />

Optical Franck–Condon Factors<br />

Absorption of light by molecules, result<strong>in</strong>g <strong>in</strong> electronic excitations, is<br />

caused by the <strong>in</strong>teraction of the bound molecular electrons with the electric<br />

field of the radiation. In the dipolar approximation, the <strong>in</strong>teraction of the<br />

dipole operator of the solute ^m0 with the time-dependent electric field EðtÞ

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