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1998-TG-10.jpg 114.6Kb JPEG image Thumbnail of $1+1^{\prime}$ TWO-COLOR PHOTOIONIZATION SPECTROSCOPY OF ACETYLENE

dc.creator Tang, Shuenn-Jiun en_US
dc.creator Lin, Jim Jr-Min en_US
dc.creator Ni, Kenny en_US
dc.creator Hsu, Yen-Chu en_US
dc.date.accessioned 2006-06-15T19:08:51Z
dc.date.available 2006-06-15T19:08:51Z
dc.date.issued 1998 en_US
dc.identifier 1998-TG-10 en_US
dc.identifier.uri http://hdl.handle.net/1811/19077
dc.description Author Institution: Institute of Atomic and Molecular Sciences, Academia Sinica, P.O. Box 23-166, Taipei, Taiwan, R.O.C. and Department of Chemistry, National Taiwan University en_US
dc.description.abstract $1+1^{\prime}$ two-color photoionization spectrum of $C_{2}H_{2}$ via a single rovibrational level of $\tilde{A}^{1} A_{u}$ as the intermediate was recorded under nearly field-free condition in the range of $91900-92700 cm^{-1}$. If the first color was frequency-tuned to excite a single rotational level $(J^{\prime} = 1 - 4, e$ parity) of $V_{4}K_{1}$ of the $\tilde{A}^{1} A_{u}$ state, sharp autoionizing spectral lines with the line width of $\Delta \nu =0.13-0.20 cm^{-1}$ were obtained except that where near the ionization threshold, extensive diffuseness $(\Delta \nu = 2.1 - 4.1 cm^{-1})$ was observed. The prominent autoionizing features have been assigned as two Rydberg series converging to the vibronic state $(K^{+} =0^{-}, V^{+}_{4} =1)$ of $C_{2}H^{+}_{2}(\tilde{X}^{2}\Pi_{u})$. However, if a single rotational level $(J^{\prime} = 2 - 4, e$ parity) of $V_{4}K_{2}$ of the $\tilde{A}$ state was chosen as the doorway state, no autoionizing Rydberg series was possibly assigned. The interchannel coupling between the vibrationally autoionizing state and the ZEKE state explains the vibronic effect of the ion core on the intensity and spectral line shape of the PFI-ZEKE spectrum of acetylene near the ionization threshold. en_US
dc.format.extent 117369 bytes
dc.format.mimetype image/jpeg
dc.language.iso English en_US
dc.type article en_US