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Volumn 102, Issue 39, 1998, Pages 7712-7722

Two valence bond state model for molecular nonlinear optical properties. Nonequilibrium solvation formulation

Author keywords

[No Author keywords available]

Indexed keywords

CALCULATIONS; ELECTRONIC STRUCTURE; FREE ENERGY; GROUND STATE; MATHEMATICAL MODELS; OPTICAL PROPERTIES; SOLVENTS; SURFACES;

EID: 0032164495     PISSN: 10895639     EISSN: None     Source Type: Journal    
DOI: 10.1021/jp981916j     Document Type: Article
Times cited : (57)

References (78)
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    • note
    • 7.8 (though this could be related to delocalized character of the charges within the donor and acceptor groups).
  • 46
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    • note
    • Since nuclear positions do not change in Franck-Condon transitions, entropies remain unchanged so that free energy differences are the same as energy differences.
  • 48
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    • note
    • This is an oversimplification; see ref 18 and the discussion around eq 2.20.
  • 49
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    • The two-level expression of (hyper)polarizabilities are easily derived using the quantum-perturbed expressions given in: Ward, J. F. Rev. Mod. Phys. 1965. 37, 1.
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    • 34 in terms of a molecule in a constant external electric field of infinite wavelength, such that the dipole moment can be used to characterize the molecule. On the other hand, a point dipole description of the solute molecule in interaction with polarization fields in the solvent is not expected to be very accurate for solutes the size of the push-pull polyenes and is avoided in the present treatment.
  • 53
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    • note
    • 0 holds that the two conditions coincide. Note also that when the mirror condition holds MIX becomes proportional to BLA. See also ref 18 for a related discussion.
  • 54
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    • note
    • It was assumed in ref 8 that the neutral state carries no dipole moment, but this is a detail irrelevant for the main point made in the text.
  • 55
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    • note
    • eq = -1: an equilibrium solvation based relation such as eq 2.26 will predict no solvent effect, whereas the nonequilibrium solvation based eq 2.25 predicts a solvent influence on the diabatic gap (see also Figure 1).
  • 56
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    • note
    • 11
  • 58
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    • note
    • F, is always the same, independent of what the composition of the ground adiabatic state might be: in a Franck-Condon transition between two VB states, the solvent electronic polarization adjusts instantly.
  • 59
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    • note
    • e.g can be developed.
  • 61
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    • note
    • 45 unfortunately, for most of the molecules solubility requirements for the various polarizability measurements rule this out.
  • 62
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    • note
    • s = t to a very good approximation.
  • 63
    • 85034277350 scopus 로고    scopus 로고
    • note
    • max: 546 (cyclohexane); 556 (dioxane); 556 (diethyl oxide); 569 (ethyl acetate); 572 (tetrahydrofurane); 584 (dichloromethane); 578 (acetone); 581 (acetonitrile); 591 (DMF); 598 (DMSO).
  • 64
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    • note
    • N = 17.3 D from Table I, this gives ΔQ = 0.40e. (See also ref 28.)
  • 65
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    • Muller, J.; Fort. A.; Barzoukas, M.; Alain, V.; Blanchard-Desce, M. Work in progress
    • Muller, J.; Fort. A.; Barzoukas, M.; Alain, V.; Blanchard-Desce, M. Work in progress.
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    • As noted in refs 44, 47, 52, and 57, refinements can be made within the basic two VB state description presented herein.
  • 69
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    • As an illustration for an environment somewhat more complex than simple solutions, one could consider the environment of an electrolyte solution (van der Zwan. G.; Hynes, J. T. Chem. Phys. 1991 152, 169). in which dissolved ions contribute to the "solvation" ingredients.
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  • 72
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    • note
    • el is the characteristic frequency of the solvent electronic polarization, which can be approximated by the solvent electronic absorption energy. The Born-Oppenheimer limit for the solvent electronic polarization is given by ρ → 0. For the molecules and solvents considered here ρ < 2/3. See Appendix C of ref 56 for the relevant equations.
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    • Bianco, R.; Juanos i Timoneda, J.; Hynes, J. T. J. Phys. Chem. 1994, 98, 12103. Bianco, R.; Hynes, J. T. J. Chem. Phys. 1995, 102, 7864, 7885.
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    • note
    • This assumes that vibrational relaxation is rapid compared to solvation dynamics proper, which is not guaranteed. In addition, the excited-state charge distribution will evolve from that reached in the Franck-Condon transition to that appropriate to equilibrium; such a feature is not included in standard descriptions, which assume, e.g., a fixed dipole moment in the excited state. This feature is incorporated in the present description.
  • 77
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    • note
    • Such experiments could also indicate if other geometrical coordinates (e.g. cis-trans isomerization) are necessary beyond the BLA coordinate.
  • 78
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    • Plaza, P.; Martin, M.; Laage, D.; Barbosa, E.; Alain, V.; Blanchard-Desce, M. Work in progress
    • Plaza, P.; Martin, M.; Laage, D.; Barbosa, E.; Alain, V.; Blanchard-Desce, M. Work in progress.


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