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The High-Resolution Fourier Transform Spectrum of Dideuterated Methane CH2D2in the Region between 1900 and 2400 cm−1

✍ Scribed by Oleg N. Ulenikov; Eizi Hirota; Mitsuru Akiyama; S. Alanko; M. Koivusaari; R. Anttila; G. Guelachvili; R.N. Tolchenov


Publisher
Elsevier Science
Year
1996
Tongue
English
Weight
569 KB
Volume
180
Category
Article
ISSN
0022-2852

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✦ Synopsis


The infrared spectrum of doubly deuterated methane CH 2 D 2 has been recorded in the region from 1900 to 2400 cm 01 at almost Doppler-limited resolution by using two high-resolution Fourier transform spectrometers. The vibrational bands observed include 2n 4 , n 4 / n 7 , 2n 7 , n 2 , n 8 , n 4 / n 9 , and n 7 / n 9 , which were analyzed by taking into account Coriolis and Fermi interactions among them and also those with n 4 / n 5 , n 3 / n 7 , and n 5 / n 7 . Most of the centrifugal distortion constants were constrained to appropriate values, while the vibrational term value and three rotational constants in each of the seven excited states were adjusted along with Coriolis and Fermi interaction parameters by the leastsquares analysis of the observed spectrum. The vibration-rotation interaction constants a s thus determined for the n 2 and n 8 states were combined with those of other fundamental states already published to calculate the equilibrium C-H distance.


📜 SIMILAR VOLUMES


High Resolution Fourier Transform Spectr
✍ O.N. Ulenikov; G.A. Onopenko; M. Koivusaari; S. Alanko; R. Anttila 📂 Article 📅 1996 🏛 Elsevier Science 🌐 English ⚖ 721 KB

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The high-resolution Fourier transform spectrum of the D 2 O molecule were recorded and analyzed in the region near 0.97 µm (10 200-10 440 cm -1 ) where the bands of the v = 4 (v = v 1 + v 2 /2 + v 3 ) polyad are located. Transitions belonging to the strongest band of the polyad, 3ν 1 + ν 3 , are ass

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✍ Sheng-gui He; O.N. Ulenikov; G.A. Onopenko; E.S. Bekhtereva; Xiang-huai Wang; Sh 📂 Article 📅 2000 🏛 Elsevier Science 🌐 English ⚖ 220 KB

The high-resolution Fourier transform spectrum of the D 2 O molecule was recorded in the 3200 -4200 cm Ϫ1 region, where the bands of the second triad of interacting vibrational states are located. As a result of the theoretical analysis, both the rotational-vibrational structure of the (011) vibrati