1987
DOI: 10.1016/0009-2614(87)80148-3
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ICN photodissociation at 193 nm; CN(B2Σ) rotational distributions and fluorescence polarization

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Cited by 5 publications
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“…The ultraviolet photolysis of ICN is an extensively studied process which has been used to explore nuclear dynamics in electronically excited states and bimolecular reactions of the photofragment CN radical. The dissociation of the I–CN bond in isolated, gas-phase ICN molecules has been directly observed on the femtosecond time scale, and computational and experimental studies characterized the dissociative electronic potentials and the resulting quantum-state specific I and CN energy distributions. The ultraviolet absorption of gaseous ICN peaks at wavelengths around 250 nm, with the broad absorption band structure composed of excitations from the linear 1 Σ + 0 ground state to excited states of 1 Π 1 , 3 Π 0+ and 3 Π 1 symmetry. The 3 Π 0+ state correlates asymptotically with CN (X 2 Σ + ) radicals and spin–orbit excited I*­( 2 P 1/2 ) atoms, but a conical intersection with the 1 Π 1 state provides a nonadiabatic pathway to the lower-lying CN (X 2 Σ + ) + I­( 2 P 3/2 ) asymptote .…”
Section: Introductionmentioning
confidence: 99%
“…The ultraviolet photolysis of ICN is an extensively studied process which has been used to explore nuclear dynamics in electronically excited states and bimolecular reactions of the photofragment CN radical. The dissociation of the I–CN bond in isolated, gas-phase ICN molecules has been directly observed on the femtosecond time scale, and computational and experimental studies characterized the dissociative electronic potentials and the resulting quantum-state specific I and CN energy distributions. The ultraviolet absorption of gaseous ICN peaks at wavelengths around 250 nm, with the broad absorption band structure composed of excitations from the linear 1 Σ + 0 ground state to excited states of 1 Π 1 , 3 Π 0+ and 3 Π 1 symmetry. The 3 Π 0+ state correlates asymptotically with CN (X 2 Σ + ) radicals and spin–orbit excited I*­( 2 P 1/2 ) atoms, but a conical intersection with the 1 Π 1 state provides a nonadiabatic pathway to the lower-lying CN (X 2 Σ + ) + I­( 2 P 3/2 ) asymptote .…”
Section: Introductionmentioning
confidence: 99%