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Fluorescence and ultraviolet absorption spectra and structure of coumaran and its ring-puckering potential energy function in the S-1(π,π*) excited state

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dc.contributor.authorYang, Juan-
dc.contributor.authorWagner, Martin-
dc.contributor.authorOkuyama, Katsuhiko-
dc.contributor.authorMorris, Kevin-
dc.contributor.authorArp, Zane-
dc.contributor.authorChoo, Jaebum-
dc.contributor.authorMeinander, Niklas-
dc.contributor.authorKwon, Ohyun-
dc.contributor.authorLaane, Jaan-
dc.date.accessioned2021-06-18T13:42:16Z-
dc.date.available2021-06-18T13:42:16Z-
dc.date.issued2006-07-21-
dc.identifier.issn0021-9606-
dc.identifier.issn1089-7690-
dc.identifier.urihttps://scholarworks.bwise.kr/cau/handle/2019.sw.cau/47025-
dc.description.abstractThe fluorescence excitation (jet cooled), single vibrational level fluorescence, and the ultraviolet absorption spectra of coumaran associated with its S-1(pi,pi(*)) electronic excited state have been recorded and analyzed. The assignment of more than 70 transitions has allowed a detailed energy map of both the S-0 and S-1 states of the ring-puckering (nu(45)) vibration to be determined in the excited states of nine other vibrations, including the ring-flapping (nu(43)) and ring-twisting (nu(44)) vibrations. Despite some interaction with nu(43) and nu(44), a one-dimensional potential energy function for the ring puckering very nicely predicts the experimentally determined energy level spacings. In the S-1(pi,pi(*)) state coumaran is quasiplanar with a barrier to planarity of 34 cm(-1) and with energy minima at puckering angles of +/- 14 degrees. The corresponding ground state (S-0) values are 154 cm(-1) and +/- 25 degrees. As is the case with the related molecules indan, phthalan, and 1,3-benzodioxole, the angle strain in the five-membered ring increases upon the pi ->pi(*) transition within the benzene ring and this increases the rigidity of the attached ring. Theoretical calculations predict the expected increases of the carbon-carbon bond lengths of the benzene ring in S-1, and they predict a barrier of 21 cm(-1) for this state. The bond length increases at the bridgehead carbon-carbon bond upon electron excitation to the S-1(pi,pi(*)) state give rise to angle changes which result in greater angle strain and a nearly planar molecule. (c) 2006 American Institute of Physics.-
dc.language영어-
dc.language.isoENG-
dc.publisherAMER INST PHYSICS-
dc.titleFluorescence and ultraviolet absorption spectra and structure of coumaran and its ring-puckering potential energy function in the S-1(π,π*) excited state-
dc.typeArticle-
dc.identifier.doi10.1063/1.2208616-
dc.identifier.bibliographicCitationJOURNAL OF CHEMICAL PHYSICS, v.125, no.3-
dc.description.isOpenAccessN-
dc.identifier.wosid000239174500015-
dc.identifier.scopusid2-s2.0-33746311495-
dc.citation.number3-
dc.citation.titleJOURNAL OF CHEMICAL PHYSICS-
dc.citation.volume125-
dc.type.docTypeArticle-
dc.publisher.location미국-
dc.subject.keywordPlusSPECTROSCOPIC DETERMINATION-
dc.subject.keywordPlusSURFACE-
dc.subject.keywordPlusVIBRATIONS-
dc.subject.keywordPlusPHTHALAN-
dc.subject.keywordPlusS-0-
dc.relation.journalResearchAreaChemistry-
dc.relation.journalResearchAreaPhysics-
dc.relation.journalWebOfScienceCategoryChemistry, Physical-
dc.relation.journalWebOfScienceCategoryPhysics, Atomic, Molecular & Chemical-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
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