In order to determine the complete \(r_{s}\) structure of methyl cyanate, the microwave spectra of \({ }^{13} \mathrm{CH}_{3} \mathrm{OCN}, \mathrm{CH}_{3}{ }^{18} \mathrm{OCN}, \mathrm{CH}_{3} \mathrm{O}^{13} \mathrm{CN}\), sym- \(\mathrm{CH}_{2} \mathrm{DOCN}\), and asym- \(\mathrm{CH}_{2} \mathrm
Microwave Spectrum of the SD+3Ion: Molecular Structure
β Scribed by Mitsunori Araki; Hiroyuki Ozeki; Shuji Saito
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 85 KB
- Volume
- 192
- Category
- Article
- ISSN
- 0022-2852
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β¦ Synopsis
The J Ο 1-0 to 4 -3 spectral lines of SD 3 Ο© were measured in the 152-610 GHz region using a source-modulated microwave spectrometer. The SD 3 Ο© ion was generated in a free space absorption cell by a hollow-cathode discharge in a gas mixture of D 2 S and D 2 . The rotational constant B 0 and the centrifugal distortion constants D J and D JK were determined from the measured frequencies. A vibration-rotation analysis was carried out and the r z structures of SH 3 Ο© and SD 3 Ο© were derived from their zero point averaged rotational constants, expressed as SH 3 Ο© : r z Ο 1.36512( 22) Γ and z Ο 94.098(26)Β°, and SD 3 Ο© : r z Ο 1.36086( 16) Γ and z Ο 94.1211(195)Β°, where the difference between z (HSH) and z (DSD) was assumed to be the same as that between z (HPH) of PH 3 and z (DPD) of PD 3 . From the shift between the r z structures of SH 3 Ο© and SD 3 Ο© , the r e structure of SH 3 Ο© was estimated to be r e Ο 1.35001(113) Γ , e Ο 94.181(135)Β°.
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