Imaging Proton Transfer and Dihalide Formation Pathways in Reactions of F(-) + CH3I

dc.bibliographicCitation.firstPage4711eng
dc.bibliographicCitation.issue27eng
dc.bibliographicCitation.lastPage4719eng
dc.bibliographicCitation.volume120eng
dc.contributor.authorCarrascosa, Eduardo
dc.contributor.authorMichaelsen, Tim
dc.contributor.authorStei, Martin
dc.contributor.authorBastian, Björn
dc.contributor.authorMeyer, Jennifer
dc.contributor.authorMikosch, Jochen
dc.contributor.authorWester, Roland
dc.date.accessioned2022-05-18T06:18:18Z
dc.date.available2022-05-18T06:18:18Z
dc.date.issued2016
dc.description.abstractIon–molecule reactions of the type X– + CH3Y are commonly assumed to produce Y– through bimolecular nucleophilic substitution (SN2). Beyond this reaction, additional reaction products have been observed throughout the last decades and have been ascribed to different entrance channel geometries differing from the commonly assumed collinear approach. We have performed a crossed beam velocity map imaging experiment on the F– + CH3I reaction at different relative collision energies between 0.4 and 2.9 eV. We find three additional channels competing with nucleophilic substitution at high energies. Experimental branching ratios and angle- and energy differential cross sections are presented for each product channel. The proton transfer product CH2I– is the main reaction channel, which competes with nucleophilic substitution up to 2.9 eV relative collision energy. At this level, the second additional channel, the formation of IF– via halogen abstraction, becomes more efficient. In addition, we present the first evidence for an [FHI]− product ion. This [FHI]− product ion is present only for a narrow range of collision energies, indicating possible dissociation at high energies. All three products show a similar trend with respect to their velocity- and scattering angle distributions, with isotropic scattering and forward scattering of the product ions occurring at low and high energies, respectively. Reactions leading to all three reaction channels present a considerable amount of energy partitioning in product internal excitation. The internally excited fraction shows a collision energy dependence only for CH2I–. A similar trend is observed for the isoelectronic OH– + CH3I system. The comparison of our experimental data at 1.55 eV collision energy with a recent theoretical calculation for the same system shows a slightly higher fraction of internal excitation than predicted, which is, however, compatible within the experimental accuracy.eng
dc.description.versionpublishedVersioneng
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/8995
dc.identifier.urihttps://doi.org/10.34657/8033
dc.language.isoengeng
dc.publisherWashington, DC : American Chemical Societyeng
dc.relation.doihttps://doi.org/10.1021/acs.jpca.5b11181
dc.relation.essn1520-5215
dc.relation.ispartofseriesJournal of Physical Chemistry A 120 (2016), Nr. 27eng
dc.rights.licenseCC BY 4.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/eng
dc.subjectForward scatteringeng
dc.subjectIonseng
dc.subjectProton transfereng
dc.subjectAdditional reactionseng
dc.subjectCollision-energy dependenceeng
dc.subjectDifferential cross sectioneng
dc.subjectIon-molecule reactioneng
dc.subjectIsotropic scatteringeng
dc.subjectNucleophilic substitutionseng
dc.subjectScattering angle distributioneng
dc.subjectTheoretical calculationseng
dc.subjectNuclear reactionseng
dc.subject.ddc530eng
dc.titleImaging Proton Transfer and Dihalide Formation Pathways in Reactions of F(-) + CH3Ieng
dc.typearticleeng
dc.typeTexteng
dcterms.bibliographicCitation.journalTitleThe journal of physical chemistry. Aeng
tib.accessRightsopenAccesseng
wgl.contributorMBIeng
wgl.subjectPhysikeng
wgl.typeZeitschriftenartikeleng
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