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dc.contributor.authorMandal, Bikramaditya
dc.contributor.authorCroft, James F. E.
dc.contributor.authorGarcía Jambrina, Pablo 
dc.contributor.authorGuo, Hua
dc.contributor.authorAoíz Moleres, Francisco Javier
dc.contributor.authorBalakrishnan, Naduvalath
dc.date.accessioned2025-07-07T08:04:55Z
dc.date.available2025-07-07T08:04:55Z
dc.date.issued2024
dc.identifier.citationPhys. Chem. Chem. Phys., 2024,26, 18368-18381es_ES
dc.identifier.issn1463-9076
dc.identifier.urihttp://hdl.handle.net/10366/166348
dc.description.abstract[EN]We report full-dimensional quantum calculations of stereodynamic control of HD(v = 1, j = 2) + D2 collisions that has been probed experimentally by Perreault et al. using the Stark-induced adiabatic Raman passage (SARP) technique. Computations were performed on two highly accurate full-dimensional H4 potential energy surfaces. It is found that for both potential surfaces, rotational quenching of HD from Image ID:d4cp01737d-t1.gif with concurrent rotational excitation of D2 from Image ID:d4cp01737d-t2.gif is the dominant transition with cross sections four times larger than that of elastically scattered D2Image ID:d4cp01737d-t3.gif for the same quenching transition in HD. This process was not considered in the original analysis of the SARP experiments that probed ΔjHD = −2 transitions in HD(vHD = 1, jHD = 2) + D2 collisions. Cross sections are characterized by an l = 3 resonance for ortho-D2(jD2 = 0) collisions, while both l = 1 and l = 3 resonances are observed for the para-D2(jD2 = 1) partner. While our results are in excellent agreement with prior measurements of elastic and inelastic differential cross sections, the agreement is less satisfactory with the SARP experiments, in particular for the Image ID:d4cp01737d-t4.gif transition for which the theoretical calculations indicate that D2 rotational excitation channel is the dominant inelastic process.es_ES
dc.format.mimetypeapplication/pdf
dc.language.isoenges_ES
dc.publisherRoyal Society of Chemistryes_ES
dc.rightsAttribution-NonCommercial 3.0 Unported*
dc.rights.urihttp://creativecommons.org/licenses/by-nc/3.0/*
dc.subjectReaction dynamicses_ES
dc.subjectComputational chemistryes_ES
dc.subjectStereodynamicses_ES
dc.titleStereodynamical control of cold HD + D2 collisionses_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.relation.publishversionhttps://doi.org/10.1039/D4CP01737Des_ES
dc.identifier.doi10.1039/D4CP01737D
dc.relation.projectIDPID2021-122839NB- I00es_ES
dc.relation.projectIDPID2020-113147GA-I00es_ES
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses_ES
dc.identifier.essn1463-9084
dc.journal.titlePhysical Chemistry Chemical Physicses_ES
dc.volume.number26es_ES
dc.issue.number26es_ES
dc.page.initial18368es_ES
dc.page.final18381es_ES
dc.type.hasVersioninfo:eu-repo/semantics/publishedVersiones_ES


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