1992
DOI: 10.1016/0022-4073(92)90008-r
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Quantitative photoabsorption and fluorescence spectroscopy of benzene, naphthalene, and some derivatives at 106–295 nm

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Cited by 72 publications
(62 citation statements)
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“…21 Burrow et al 22 determined the vertical electron affinities and characterized the temporary anion states of a series of hydrocarbons including benzene, using electron transmission spectroscopy, while a review of all these resonance studies was provided by Allan. 23 Most experimental studies into excitation of the 1 B 1u and 1 E 1u electronic states have employed either photoabsorption or dipole (e,e ) techniques, [24][25][26][27][28] in order to determine their respective optical oscillator strengths (OOSs). Agreement between the various OOS measurements for the 1 E 1u state is typically very good to the ±5% level, however, for the 1 B 1u state there is a serious disagreement between the results of Feng et al 24 , and Suto et al 25 on the one hand, and those of Philis et al, 26 Pantos et al 27 and Hammond and Price, 28 on the other.…”
Section: Introductionmentioning
confidence: 99%
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“…21 Burrow et al 22 determined the vertical electron affinities and characterized the temporary anion states of a series of hydrocarbons including benzene, using electron transmission spectroscopy, while a review of all these resonance studies was provided by Allan. 23 Most experimental studies into excitation of the 1 B 1u and 1 E 1u electronic states have employed either photoabsorption or dipole (e,e ) techniques, [24][25][26][27][28] in order to determine their respective optical oscillator strengths (OOSs). Agreement between the various OOS measurements for the 1 E 1u state is typically very good to the ±5% level, however, for the 1 B 1u state there is a serious disagreement between the results of Feng et al 24 , and Suto et al 25 on the one hand, and those of Philis et al, 26 Pantos et al 27 and Hammond and Price, 28 on the other.…”
Section: Introductionmentioning
confidence: 99%
“…23 Most experimental studies into excitation of the 1 B 1u and 1 E 1u electronic states have employed either photoabsorption or dipole (e,e ) techniques, [24][25][26][27][28] in order to determine their respective optical oscillator strengths (OOSs). Agreement between the various OOS measurements for the 1 E 1u state is typically very good to the ±5% level, however, for the 1 B 1u state there is a serious disagreement between the results of Feng et al 24 , and Suto et al 25 on the one hand, and those of Philis et al, 26 Pantos et al 27 and Hammond and Price, 28 on the other. Finally, we note the total ionization cross section results from measurements due to Schram et al 29 From a theoretical perspective, elastic electron scattering from C 6 H 6 , at energies up to about 40 eV, using single-center expansion methods at the static exchange level, were reported by Gianturco and Lucchese.…”
Section: Introductionmentioning
confidence: 99%
“…Of course, matrix isolation spectroscopy provided important measurements, even up to the deep UV. Unfortunately, few were studied in the gas phase around the bump region, most spectra being published in 1992 using synchrotron light sources (Joblin et al 1992;Suto et al 1992). Since that time, nearly no new spectra were published and moreover no cold ones.…”
Section: From the Visible To The 217 Nm Bump Region Absorption Of Thementioning
confidence: 99%
“…The existence of fast relaxation channels in highly excited states of neutral PAHs remains to be explored, only one study seems to be available Suto et al (1992). The strength of the coupling in radicals or superhydrogenated PAHs is still unknown.…”
Section: Nonradiative Transitions In Pahs: Present Statusmentioning
confidence: 99%
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