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dc.contributor.authorSemba, Yosukeen_US
dc.contributor.authorYoshida, Kazutoen_US
dc.contributor.authorKasahara, Shunjien_US
dc.contributor.authorNi, Chi-Kungen_US
dc.contributor.authorHsu, Yen-Chuen_US
dc.contributor.authorLin, Sheng Hsienen_US
dc.contributor.authorOhshima, Yasuhiroen_US
dc.contributor.authorBaba, Masaakien_US
dc.date.accessioned2019-04-02T06:00:10Z-
dc.date.available2019-04-02T06:00:10Z-
dc.date.issued2009-07-14en_US
dc.identifier.issn0021-9606en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.3168394en_US
dc.identifier.urihttp://hdl.handle.net/11536/149806-
dc.description.abstractWe have observed rotationally resolved ultrahigh-resolution fluorescence excitation spectra of the 0(0)(0) (a-type) and 0(0)(0)+467 cm(-1) (b-type) bands of the S-2 (1)A(1)<- S-0 (1)A(1) transition of jet-cooled azulene. The observed linewidth is 0.0017 cm(-1), which corresponds to the lifetime of 3.1 ns in the S-2 state. Zeeman splitting of rotational lines is very small so that intersystem crossing to the triplet state is considered to be very slow. Inertial defect is very small and the molecule is considered to be planar in the S-0 and S-2 states (C-2 upsilon symmetry). Rotational constants of the S-2 state are almost identical to those of the S-0 state, indicating that geometrical structure is similar in both electronic states. In this case, internal conversion (IC) by vibronic coupling is thought to be inactive. Therefore, the main radiationless transition process in the S-2 (1)A(1) state of azulene was identified to be IC to the S-1 B-1(2) state. However, this S-2 -> S-1 IC is still slower than that of conventional polycyclic aromatic hydrocarbons. We consider it to be due to the shallower potential energy curve in the S-1 B-1(2) state, which is also responsible for the extraordinarily fast S-1 -> S-0 IC in the isolated azulene molecule. (C) 2009 American Institute of Physics. [DOI: 10.1063/1.3168394]en_US
dc.language.isoen_USen_US
dc.titleRotationally resolved ultrahigh-resolution laser spectroscopy of the S-2 (1)A(1)<- S-0 (1)A(1) transition of azuleneen_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.3168394en_US
dc.identifier.journalJOURNAL OF CHEMICAL PHYSICSen_US
dc.citation.volume131en_US
dc.contributor.department應用化學系zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.identifier.wosnumberWOS:000267983100026en_US
dc.citation.woscount5en_US
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