1989
DOI: 10.1016/0301-0104(89)87173-3
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An investigation of the excited state dynamics of cyclohexadiene in a supersonic jet

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Cited by 9 publications
(6 citation statements)
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“…The low symmetry of the system allows the doubly excited configuration to mix and contribute to this state, unlike in CHD14 (the V 5 state). While no evidence of this state is seen in the gas phase spectra, a transition has been reported 41 near 6.3 eV in the liquid phase. As Rydberg transitions do not appear in solution, the most likely assignment for this transition is to a valence state.…”
Section: Theoretical Results and Discussionmentioning
confidence: 94%
See 1 more Smart Citation
“…The low symmetry of the system allows the doubly excited configuration to mix and contribute to this state, unlike in CHD14 (the V 5 state). While no evidence of this state is seen in the gas phase spectra, a transition has been reported 41 near 6.3 eV in the liquid phase. As Rydberg transitions do not appear in solution, the most likely assignment for this transition is to a valence state.…”
Section: Theoretical Results and Discussionmentioning
confidence: 94%
“…Two ab initio studies of the excited states of CHD13 have been reported. One, a MRCI calculation by Share et al, placed the intense transition to the first valence 1 B state (at the ground state geometry) at much higher energies than the weak transition to the lowest valence excited 1 A state placed the B vertically excited state below the A state.…”
Section: Introductionmentioning
confidence: 99%
“…89,90 Earlier studies erroneously predicted S 2 to be the bright B state. 91,92 This may have led to the hypothesis that a S 2 -S 1 transition is involved in the excited state decay of Pro. 28 For Pro, TDDFT and CC2 calculations predict the first excited state to be the bright (1B-like) state (Table 2).…”
Section: Resultsmentioning
confidence: 99%
“…The peak probe beam intensity in the focal plane was about 2ϫ10 13 W cm Ϫ2 . Whereas with low-intensity ionization ͑i.e., at 267 nm͒ the mass spectra of CHD and HT are almost indistinguishable, 22 they show a rather different fragmentation pattern when ionized by an intense-laser field: HT produces a strong H ϩ signal, while CHD gives practically no hydrogen ion. The TOF-spectrum of the H ϩ signal has a characteristic doublet shape indicating that it is due to Coulomb explosion of a doubly charged parent ion.…”
mentioning
confidence: 94%