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MPI photoelectron spectroscopy of <i>u</i> <i>n</i> <i>g</i> <i>e</i> <i>r</i> <i>a</i> <i>d</i> <i>e</i> excited states of acetylene: Intermediate state mixing and ion state selection
63
Citations
48
References
1987
Year
Localized Excited StateEngineeringAbsorption SpectroscopyMpi Photoelectron SpectroscopyChemistryElectronic Excited StateIonization SpectroscopyElectron SpectroscopySharp BandsPhotophysical PropertyPhotochemistryPhysicsAtomic PhysicsPhysical ChemistryPhoton ResonantQuantum ChemistryExcited State PropertyNatural SciencesSpectroscopyApplied PhysicsIntermediate State MixingIon State Selection
Three photon resonant, four photon (3+1) ionization spectroscopy and photoelectron spectroscopy have been used to study the ungerade excited states of acetylene in the energy range from 74 500 to 90 000 cm−1. Sharp bands from the nR (π3u nsσg) and 1Φu (π3u ndδg) Rydberg series dominate the MPI spectrum. A large number of Rydberg and valence states which are prominent in VUV absorption spectra are absent or weak in MPI studies. These weak bands are only observable under high power conditions, which suggests that nonradiative decay is rapid enough to depopulate these states before ionization occurs. The photoelectron results provide further insight into the nature of the excited states. Ionization through the sharp bands occurs via Δν=0 Franck–Condon transitions, resulting in ions in a single vibrational state. Ionization through bands which are mixed results in complicated ion vibrational distributions including excitation of both cis and trans bends.
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