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The unimolecular reaction of <i>t</i>-BuNO on singlet and triplet surfaces: Spectroscopy, real-time rate measurements, and NO energy distributions
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Citations
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References
1986
Year
EngineeringLaser ApplicationsChemistryElectronic Excited StateLaser ExcitationOptical SpectroscopyPhotophysical PropertyUnimolecular ReactionPhysicsPhotochemistryMechanistic PhotochemistryPhysical ChemistryQuantum ChemistryTriplet SurfacesExcited State PropertyLaser PhotochemistryNatural SciencesSpectroscopyReal-time Rate MeasurementsDissociation ProceedsReal Time
The predissociation of jet-cooled (CH3)3CNO (t-BuNO) following laser excitation in the à 1A″←X̃ 1A′ system has been studied in both the energy (frequency) and time domains. Unlike the smaller nitroso compounds whose predissociation has been already examined, unimolecular reaction is the rate determining step for predissociation near threshold. Consequently, it has been possible to separately measure radiationless transition rates and unimolecular reaction rates in real time. Dissociation on both the ground state (S0) and the first triplet state (T1) has been identified. At threshold, dissociation proceeds only on S0, with lifetimes &gt;3.5 μs, but for E°≥650 cm−1, fast (&lt;10 ns) predissociation via T1 becomes progressively the dominant dissociative route. Nascent NO photofragments have been characterized in detail using one-photon LIF. The rotational and spin-orbit distributions of NO following dissociation on S0 are statistical, depending only on E°. The NO derived from dissociation on the T1 surface is not at all statistical, consistent with a sizable (∼650 cm−1) exit channel barrier on this surface. Most notably, the [NO(2Π3/2)]/[NO(2Π1/2)] ratios are much smaller, and rotational distributions are colder than predicted by a statistical model. In order that some of the predissociating vibrational states could be assigned, the 1A″←1A′ spectrum of t-BuNO has been analyzed and the electronic origin assigned as 13 911 cm−1. The ground state dissociation energy, D0, is found to be 13 930±30 cm−1, i.e., 39.8±0.1 kcal mol−1.
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