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dc.contributor.authorBaba, Masaakien_US
dc.contributor.authorSaitoh, Motohisaen_US
dc.contributor.authorKowaka, Yasuyukien_US
dc.contributor.authorTaguma, Kunioen_US
dc.contributor.authorYoshida, Kazutoen_US
dc.contributor.authorSemba, Yosukeen_US
dc.contributor.authorKasahara, Shunjien_US
dc.contributor.authorYamanaka, Takayaen_US
dc.contributor.authorOhshima, Yasuhiroen_US
dc.contributor.authorHsu, Yen-Chuen_US
dc.contributor.authorLin, Sheng Hsienen_US
dc.date.accessioned2014-12-08T15:23:59Z-
dc.date.available2014-12-08T15:23:59Z-
dc.date.issued1970-01-01en_US
dc.identifier.issn0021-9606en_US
dc.identifier.urihttp://dx.doi.org/224318en_US
dc.identifier.urihttp://hdl.handle.net/11536/16686-
dc.description.abstract"Vibrational level structure in the S-0 (1)A(g) and S-1 B-1(3u) states of pyrene was investigated through analysis of fluorescence excitation spectra and dispersed fluorescence spectra for single vibronic level excitation in a supersonic jet and through referring to the results of ab initio theoretical calculation. The vibrational energies are very similar in the both states. We found broad spectral feature in the dispersed fluorescence spectrum for single vibronic level excitation with an excess energy of 730 cm(-1). This indicates that intramolecular vibrational redistribution efficiently occurs at small amounts of excess energy in the S-1 B-1(3u) state of pyrene. We have also observed a rotationally resolved ultrahigh-resolution spectrum of the 0(0)(0) band. Rotational constants have been determined and it has been shown that the pyrene molecule is planar in both the S-0 and S-1 states, and that its geometrical structure does not change significantly upon electronic excitation. Broadening of rotational lines with the magnetic field by the Zeeman splitting of M-J levels was very small, indicating that intersystem crossing to the triplet state is minimal. The long fluorescence lifetime indicates that internal conversion to the S-0 state is also slow. We conclude that the similarity of pyrene's molecular structure and potential energy curve in its S-0 and S-1 states is the main cause of the slow radiationless transitions."en_US
dc.language.isoen_USen_US
dc.subjectab initio calculationsen_US
dc.subjectexcited statesen_US
dc.subjectfluorescenceen_US
dc.subjectintramolecular mechanicsen_US
dc.subjectnonradiative transitionsen_US
dc.subjectorganic compoundsen_US
dc.subjectpotential energy surfacesen_US
dc.subjectradiative lifetimesen_US
dc.subjectrotational statesen_US
dc.subjectvibrational statesen_US
dc.subjectvibronic statesen_US
dc.subjectZeeman effecten_US
dc.titleVibrational and rotational structure and excited-state dynamics of pyreneen_US
dc.typeArticleen_US
dc.identifier.doi224318en_US
dc.identifier.journalJOURNAL OF CHEMICAL PHYSICSen_US
dc.citation.volume131en_US
dc.citation.issue22en_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:000272803000035-
dc.citation.woscount18-
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