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dc.contributor.authorSmith, Mica C.en_US
dc.contributor.authorTing, Wei-Lunen_US
dc.contributor.authorChang, Chun-Hungen_US
dc.contributor.authorTakahashi, Kaitoen_US
dc.contributor.authorBoering, Kristie A.en_US
dc.contributor.authorLin, Jim Jr-Minen_US
dc.date.accessioned2014-12-08T15:36:42Z-
dc.date.available2014-12-08T15:36:42Z-
dc.date.issued2014-08-21en_US
dc.identifier.issn0021-9606en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.4892582en_US
dc.identifier.urihttp://hdl.handle.net/11536/25057-
dc.description.abstractThe UV spectrum of CH3CHOO was measured by transient absorption in a flow cell at 295 K. The absolute absorption cross sections of CH3CHOO were measured by laser depletion in a molecular beam to be (1.06 +/- 0.09) x 10(-17) cm(2) molecule-1 at 308 nm and (9.7 +/- 0.6) x 10(-18) cm(2) molecule-1 at 352 nm. After scaling the UV spectrum of CH3CHOO to the absolute cross section at 308 nm, the peak UV cross section is (1.27 +/- 0.11) x 10(-)1(7) cm(2) molecule-1 at 328 nm. Compared to the simplest Criegee intermediate CH2OO, the UV absorption band of CH3CHOO is similar in intensity but blue shifted by 14 nm, resulting in a 20% slower photolysis rate estimated for CH3CHOO in the atmosphere. (C) 2014 AIP Publishing LLC.en_US
dc.language.isoen_USen_US
dc.titleUV absorption spectrum of the C2 Criegee intermediate CH3CHOOen_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.4892582en_US
dc.identifier.journalJOURNAL OF CHEMICAL PHYSICSen_US
dc.citation.volume141en_US
dc.citation.issue7en_US
dc.citation.epageen_US
dc.contributor.department應用化學系zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.identifier.wosnumberWOS:000340714600016-
dc.citation.woscount4-
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