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dc.contributor.authorChen, Ting-Yuen_US
dc.contributor.authorLee, Yuan-Pernen_US
dc.date.accessioned2020-10-05T02:01:59Z-
dc.date.available2020-10-05T02:01:59Z-
dc.date.issued2020-08-21en_US
dc.identifier.issn1463-9076en_US
dc.identifier.urihttp://dx.doi.org/10.1039/d0cp01940ben_US
dc.identifier.urihttp://hdl.handle.net/11536/155409-
dc.description.abstractThe reaction CH2I + O(2)has been widely employed recently for the production of the simplest Criegee intermediate CH2OO in laboratories, but the detailed dynamics of this reaction have been little explored. Infrared emission of several products of this reaction, initiated on irradiation of CH(2)I(2)and O-2(similar to 8 Torr) in a flowing mixture at 308 or 248 nm, was recorded with a step-scan Fourier-transform spectrometer; possible routes of formation were identified according to the observed vibrational distribution of products and published theoretical potential-energy schemes. Upon irradiation at 308 nm, Boltzmann distributions of CO (v <= 5,J <= 19) with an average vibrational energy of 32 +/- 3 kJ mol(-1)and OH (v <= 3,J <= 5.5) with an average vibrational energy of 29 +/- 4 kJ mol(-1)were observed and assigned to the decomposition of HCOOH* to form CO + H2O and OH + HCO, respectively. The broadband emission of CO(2)was simulated with two vibrational distributions of average energies (91 +/- 4) and (147 +/- 8) kJ mol(-1)and assigned to be produced from the decomposition of HCOOH* and methylene bis(oxy), respectively. Upon irradiation of samples at 248 nm, the emission of OH and CO(2)showed similar distributions with slightly greater energies, but the distribution of CO (v <= 11,J <= 19) became bimodal with average vibrational energies of (23 +/- 4) and (107 +/- 29) kJ mol(-1), and branching (56 +/- 5) : (44 +/- 5). The additional large-vcomponent is assigned to be produced from a secondary reaction HCO + O(2)to form CO + HO2; HCO is a coproduct of OH. The branching between CO and OH is (50 +/- 5) : (50 +/- 5) at 308 nm and (64 +/- 5) : (36 +/- 4) at 248 nm, consistent with the mechanism according to which an additional channel to produce CO opens at 248 nm. Highly internally excited H2CO was also observed. With O(2)at 16 Torr, the extrapolated nascent internal distributions are similar to those with O(2)at 8 Torr except for a slight quenching effect.en_US
dc.language.isoen_USen_US
dc.titleDynamics of the reaction CH2I + O(2)probedviainfrared emission of CO, CO2, OH and H2COen_US
dc.typeArticleen_US
dc.identifier.doi10.1039/d0cp01940ben_US
dc.identifier.journalPHYSICAL CHEMISTRY CHEMICAL PHYSICSen_US
dc.citation.volume22en_US
dc.citation.issue31en_US
dc.citation.spage17540en_US
dc.citation.epage17553en_US
dc.contributor.department交大名義發表zh_TW
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.departmentNational Chiao Tung Universityen_US
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.contributor.departmentInstitute of Molecular scienceen_US
dc.identifier.wosnumberWOS:000560847500007en_US
dc.citation.woscount0en_US
Appears in Collections:Articles