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dc.contributor.authorHuang, Chong-Kaien_US
dc.contributor.authorXu, Zhen-Fengen_US
dc.contributor.authorNakajima, Masakazuen_US
dc.contributor.authorNguyen, Hue M. T.en_US
dc.contributor.authorLin, M. C.en_US
dc.contributor.authorTsuchiya, Sojien_US
dc.contributor.authorLee, Yuan-Pernen_US
dc.date.accessioned2014-12-08T15:28:35Z-
dc.date.available2014-12-08T15:28:35Z-
dc.date.issued2012-10-28en_US
dc.identifier.issn0021-9606en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.4759619en_US
dc.identifier.urihttp://hdl.handle.net/11536/20681-
dc.description.abstractWe investigated the reactivity of O(D-1) towards two types of hydrogen atoms in CH3OH. The reaction was initiated on irradiation of a flowing mixture of O-3 and CD3OH or CH3OD at 248 nm. Relative vibration-rotational populations of OH and OD (1 <= nu <= 4) states were determined from their infrared emission recorded with a step-scan time-resolved Fourier-transform spectrometer. In O(D-1) + CD3OH, the rotational distribution of OD is nearly Boltzmann, whereas that of OH is bimodal; the product ratio [OH]/[OD] is 1.56 +/- 0.36. In O(D-1) + CH3OD, the rotational distribution of OH is nearly Boltzmann, whereas that of OD is bimodal; the product ratio [OH]/[OD] is 0.59 +/- 0.14. Quantum-chemical calculations of the potential energy and microcanonical rate coefficients of various channels indicate that the abstraction channels are unimportant and O(D-1) inserts into the C-H and O-H bonds of CH3OH to form HOCH2OH and CH3OOH, respectively. The observed three channels of OH are consistent with those produced via decomposition of the newly formed OH or the original OH moiety in HOCH2OH or decomposition of CH3OOH. The former decomposition channel of HOCH2OH produces vibrationally more excited OH because of incomplete intramolecular vibrational relaxation, and decomposition of CH3COOH produces OH with greater rotational excitation, likely due to a large torque angle during dissociation. The predicted [OH]/[OD] ratios are 1.31 and 0.61 for O(D-1) + CD3OH and CH3OD, respectively, at collision energy of 26 kJ mol(-1), in satisfactory agreement with the experimental results. These predicted product ratios vary weakly with collision energy. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4759619]en_US
dc.language.isoen_USen_US
dc.titleDynamics of the reactions of O(D-1) with CD3OH and CH3OD studied with time-resolved Fourier-transform IR spectroscopyen_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.4759619en_US
dc.identifier.journalJOURNAL OF CHEMICAL PHYSICSen_US
dc.citation.volume137en_US
dc.citation.issue16en_US
dc.citation.epageen_US
dc.contributor.department應用化學系zh_TW
dc.contributor.department應用化學系分子科學碩博班zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.contributor.departmentInstitute of Molecular scienceen_US
dc.identifier.wosnumberWOS:000310853800023-
dc.citation.woscount3-
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