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Photodissociative production of O(1<i>S</i>) from N2O and S(1<i>S</i>) from OCS in rare gas matrices
11
Citations
24
References
1980
Year
EngineeringRare Gas MatrixExcitation Energy TransferRare Gas MatricesChemistryElectronic Excited StatePhotoelectrochemistryPhosphorescence ImagingPhotocatalysisPhotophysical PropertyPhysicsPhotochemistryMechanistic PhotochemistryAtomic PhysicsPhysical ChemistryPhotodissociation Energy ThresholdsQuantum ChemistryParticular Rydberg StatePhotodissociative ProductionExcited State PropertyNatural SciencesSpectroscopyApplied Physics
Photoluminescence excitation spectra of Ar:N2O (1%), Ar:OCS (1%), and Kr:OCS (1%) were obtained in the region 180–104 nm, using UV synchrotron radiation at SSRL. Photodissociation energy thresholds in the matrix were found to be: 8.06 eV for N2O→N2(X 1Σ+)+0(1S) and 7.17 eV for OCS→CO (X 1Σ+)+S(1S). Our results show several effects due to interactions between the matrix and the triatomic molecule: (1) differential blue shifts of the 1Π←1Σ+ and 1Σ+←1Σ+ transitions, (2) a greatly enhanced predissociation rate from 1Π to 1Σ+, (3) matrix dependent energy shifts of a particular Rydberg state, (4) nonradiative energy transfer between the matrix and the triatomic, involving either self-trapped excitons and a Foster–Dexter mechanism or free excitons and a harpooning mechanism. To our knowledge, this is the first observation of the free exciton–harpooning mechanism in a rare gas matrix.
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