Differential Cross Sections for the H + D2 → HD(v′ = 3, j′ = 4-10) + D Reaction above the Conical Intersection

dc.bibliographicCitation.firstPage12036
dc.bibliographicCitation.issue50
dc.bibliographicCitation.journalTitleThe journal of physical chemistry : A, Molecules, spectroscopy, kinetics, environment & general theoryeng
dc.bibliographicCitation.lastPage12042
dc.bibliographicCitation.volume119
dc.contributor.authorGao, Hong
dc.contributor.authorSneha, Mahima
dc.contributor.authorBouakline, Foudhil
dc.contributor.authorAlthorpe, Stuart C.
dc.contributor.authorZare, Richard N.
dc.date.accessioned2022-07-04T06:20:43Z
dc.date.available2022-07-04T06:20:43Z
dc.date.issued2015
dc.description.abstractWe report rovibrationally selected differential cross sections (DCSs) of the benchmark reaction H + D2 → HD(v′ = 3, j′ = 4–10) + D at a collision energy of 3.26 eV, which exceeds the conical intersection of the H3 potential energy surface at 2.74 eV. We use the PHOTOLOC technique in which a fluorine excimer laser at 157.64 nm photodissociates hydrogen bromide (HBr) molecules to generate fast H atoms and the HD product is detected in a state-specific manner by resonance-enhanced multiphoton ionization. Fully converged quantum wave packet calculations were performed for this reaction at this high collision energy without inclusion of the geometric phase (GP) effect, which takes into account coupling to the first excited state of the H3 potential energy surface. Multimodal structures can be observed in most of the DCSs up to j′ = 10, which is predicted by theory and also well-reproduced by experiment. The theoretically calculated DCSs are in good overall agreement with the experimental measurements, which indicates that the GP effect is not large enough that its existence can be verified experimentally at this collision energy.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/9488
dc.identifier.urihttps://doi.org/10.34657/8526
dc.language.isoengeng
dc.publisherWashington, DC : Soc.
dc.relation.doihttps://doi.org/10.1021/acs.jpca.5b04573
dc.relation.essn1520-5215
dc.rights.licenseACS AuthorChoice
dc.rights.urihttps://pubs.acs.org/page/policy/authorchoice_termsofuse.html
dc.subject.ddc530
dc.subject.otherAtom laserseng
dc.subject.otherExcimer laserseng
dc.subject.otherMolecular physicseng
dc.subject.otherPhotoionizationeng
dc.subject.otherPotential energyeng
dc.subject.otherPotential energy surfaceseng
dc.subject.otherQuantum chemistryeng
dc.subject.otherQuantum theoryeng
dc.subject.otherCollision energieseng
dc.subject.otherConical intersectioneng
dc.subject.otherDifferential cross sectioneng
dc.subject.otherFirst excited stateeng
dc.subject.otherHydrogen bromideeng
dc.subject.otherMultimodal structureeng
dc.subject.otherQuantum wave packetseng
dc.subject.otherResonance-enhanced multiphoton ionizationeng
dc.subject.otherExcited stateseng
dc.titleDifferential Cross Sections for the H + D2 → HD(v′ = 3, j′ = 4-10) + D Reaction above the Conical Intersectioneng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorMBIger
wgl.subjectPhysikger
wgl.subjectChemieger
wgl.typeZeitschriftenartikelger
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