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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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11.1 Theoretical treatment <strong>of</strong> solvent effects 661<br />

Table 11.1.3. INDO/S SCRF CI calculated and experimental spectroscopic transition<br />

energies <strong>of</strong> some dyes in different solvents 27<br />

Molecule Solvent νcalc, cm -1<br />

(Scheme 23)<br />

(Scheme 24)<br />

(Scheme 25)<br />

Gas phase<br />

Cyclohexane<br />

Water<br />

Gas phase<br />

n-Hexane<br />

Water<br />

Gas phase<br />

Chlor<strong>of</strong>orm<br />

Water<br />

Scheme 23 Scheme 24<br />

Scheme 25<br />

29,700<br />

26,300<br />

22,500<br />

36,900<br />

34,800<br />

31,100<br />

20,200<br />

21,800<br />

24,600<br />

νexp, cm -1<br />

-<br />

27,400<br />

23,300<br />

-<br />

30,200<br />

26,100<br />

-<br />

19,600<br />

22,100<br />

The INDO/S SCRF CI method has been also successfully applied for the prediction <strong>of</strong><br />

the solvatochromic shifts in various nitro-substituted porphyrins. 32<br />

The SCRF methodology has been employed also for the prediction <strong>of</strong> the<br />

solvatochromic shifts on emission spectra. 33,34 A satisfactory agreement was obtained between<br />

the calculated and experimental fluorescence energies <strong>of</strong><br />

p-N,N-dimethylaminobenzonitrile in different solvents. Finally, the solvent-induced shifts<br />

in the vibrational spectra <strong>of</strong> molecules have been also calculated using the SCRF theory. 35<br />

The SCRF approach has been also implemented for the treatment <strong>of</strong> solute-continuum<br />

solvent systems at the ab initio Hartree-Fock level <strong>of</strong> theory. 36,37 In addition, a general SCRF<br />

(GSCRF) approach has been proposed to account for the interaction <strong>of</strong> the solvent reaction<br />

field with the arbitrary charge distribution <strong>of</strong> the solute molecule. According to this theory,<br />

38,39 the effective Hamiltonian <strong>of</strong> the solute in the solvent has the following form<br />

⎣ ⎦<br />

H� H� 0 0<br />

= + drΩ r V r + dr′ G r,r′ Ω r′<br />

[11.1.71]<br />

∫<br />

() () ∫ ( ) ( )<br />

s s s m s<br />

where Ω s ( r) is the solute charge density operator given by<br />

() r =− ( r − r) + ∑Z<br />

( r −R<br />

)<br />

Ωs i a a<br />

i<br />

a<br />

∑δ δ [11.1.72]

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