1998
DOI: 10.1063/1.477792
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Resonance Raman intensity analysis of a dicyanovinyl-azaadamantane: Mode-specific reorganization energies for charge-transfer and locally-excited states

Abstract: A resonance Raman intensity analysis is performed on the intramolecular charge-transfer molecule 1-aza-adamantane-4-ylidenemalononitrile in acetonitrile solution. We explore the extent to which changes in molecular structure upon charge transfer can be obtained from resonance Raman intensity analysis, and extend the analysis method for charge-transfer excitation to take into account the possible influence of nearby locally excited states. Absolute scattering cross sections are measured at five excitation wavel… Show more

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Cited by 52 publications
(61 citation statements)
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“…We have used ab initio calculations to help choose the appropriate sign of the normal mode displacements. [105][106][107][108][109][110] Table III compares the results of CIS/3-21G*//Becke3P86/3-21G*, and DT͑RPA͒/3-21G*// Becke3P86/3-21G* computations for the normal mode displacements with the absolute value of those determined from resonance Raman intensity analysis of the experimental spectra. There is generally reasonable agreement between the calculated and experimental values for the lower frequency modes ͑below 1000 cm Ϫ1 ͒ associated mainly with the carbon ring and iodine atom as well as the axial v 11 mode at 1190 cm Ϫ1 and the equatorial v 8 mode at 1308 cm Ϫ1 .…”
Section: Resultsmentioning
confidence: 99%
“…We have used ab initio calculations to help choose the appropriate sign of the normal mode displacements. [105][106][107][108][109][110] Table III compares the results of CIS/3-21G*//Becke3P86/3-21G*, and DT͑RPA͒/3-21G*// Becke3P86/3-21G* computations for the normal mode displacements with the absolute value of those determined from resonance Raman intensity analysis of the experimental spectra. There is generally reasonable agreement between the calculated and experimental values for the lower frequency modes ͑below 1000 cm Ϫ1 ͒ associated mainly with the carbon ring and iodine atom as well as the axial v 11 mode at 1190 cm Ϫ1 and the equatorial v 8 mode at 1308 cm Ϫ1 .…”
Section: Resultsmentioning
confidence: 99%
“…(205) and (208); see also Refs. [526,527]. The experimentally determined excitation energies of 3.61 and 4.17 eV, (and a laser wavelength of 388 nm) were assumed in these simulations in order to avoid problems caused by the wrong calculated energy gap between the two states.…”
Section: The Photochemistry Of O-nitrobenzaldehydementioning
confidence: 99%
“…[29][30][31] In order to elucidate the natures of the different electronic transitions we use 457 and 785 nm excitations, which selectively probe the high and low energy absorption bands of the polymers in solution, (see Figure 2b). [29][30][31] In order to elucidate the natures of the different electronic transitions we use 457 and 785 nm excitations, which selectively probe the high and low energy absorption bands of the polymers in solution, (see Figure 2b).…”
Section: Resonant Raman Spectroscopymentioning
confidence: 99%
“…[29][30][31] The different distortions resulting from excitation at different wavelengths can be readily probed using resonant Raman spectroscopy. [29][30][31] The different distortions resulting from excitation at different wavelengths can be readily probed using resonant Raman spectroscopy.…”
Section: Introductionmentioning
confidence: 99%