Relaxation of NH(a1?, v=1) in Collisions with H(2S): An Experimental and Theoretical Study

dc.contributor.authorDefazio, P.
dc.contributor.authorPetrongolo, C.
dc.contributor.authorMcBane, G. C.
dc.contributor.authorAdam, L.
dc.contributor.authorHack, W.
dc.contributor.authorAkpinar, S.
dc.contributor.authorSchinke, R.
dc.date.accessioned2026-08-12T17:30:23Z
dc.date.issued2009
dc.departmentFırat Üniversitesi
dc.description.abstractCollisions of electronically and vibrationally excited NH(a(1)Delta, v = 1) with H atoms were investigated by experimental, quantum mechanical (QM) wavepacket, and quasiclassical trajectory (QCT) methods. The NH(a(1)Delta, v = 1) total loss rate constant, corresponding to the sum of the NH vibrational relaxation, N(D-2)+H-2 formation, and electronic quenching to NH(X-3 Sigma(-)), was measured at room temperature, Most of the calculations were performed within the Born-Oppenheimer approximation, neglecting electronic quenching due to Renner-Teller Coupling because QCT calculations showed that for the loss of NH(a(1)Delta, v = 1) the contribution of quenching is negligible. The QM Study included Coriolis couplings, and the QCT study counted only trajectories ending close to a vibrational quantum level of the product diatom. The collisions are dominated by long-lived intermediate complexes, and QM probabilities and cross sections thus exhibit pronounced resonances. QM and QCT cross sections and rate coefficients of the various processes are in very good agreement. The measured rate constant is (9.1 +/- 3.3) x 10(-11) cm(3) s(-1), compared with (14.4 +/- 0.5) x 10(-11) and (15.6 +/- 1.6) x 10(-11) cm(3) s(-1), as obtained from QM and QCT calculations, respectively. The reason for the theoretical overestimation is unknown.
dc.description.sponsorshipMIUR and IPCF-CNR of Pisa; Max-Planck-Institut fur Dynamik und Selbstorganisation
dc.description.sponsorshipThis work was supported by MIUR and IPCF-CNR of Pisa and by the Max-Planck-Institut fur Dynamik und Selbstorganisation.
dc.identifier.doi10.1021/jp903839p
dc.identifier.endpage14464
dc.identifier.issn1089-5639
dc.identifier.issue52
dc.identifier.orcid0000-0002-9655-7641
dc.identifier.orcid0000-0002-2790-3467
dc.identifier.pmid19569615
dc.identifier.scopus2-s2.0-73949150066
dc.identifier.scopusqualityQ2
dc.identifier.startpage14458
dc.identifier.urihttps://doi.org/10.1021/jp903839p
dc.identifier.urihttps://hdl.handle.net/11508/56074
dc.identifier.volume113
dc.identifier.wosWOS:000273263700036
dc.identifier.wosqualityQ2
dc.indekslendigikaynakWeb of Science
dc.indekslendigikaynakScopus
dc.indekslendigikaynakPubMed
dc.language.isoen
dc.publisherAmer Chemical Soc
dc.relation.ispartofJournal of Physical Chemistry A
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.snmzKA_WoS_20260511
dc.subjectPotential-Energy Surface
dc.subjectReal Wave-Packets
dc.subjectN(D-2)+H-2 Reaction
dc.subjectAngular-Momentum
dc.subjectNh2
dc.subjectTransitions
dc.subjectAtoms
dc.subjectH-2
dc.subjectPhotolysis
dc.subjectMolecules
dc.titleRelaxation of NH(a1?, v=1) in Collisions with H(2S): An Experimental and Theoretical Study
dc.typeArticle

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