Using high-resolution Fourier transform spectra of monoisotopic \(\mathrm{H}_{2}{ }^{80} \mathrm{Se}\) recorded in the 1.8 and \(1.55-\mu \mathrm{m}\) regions. an extensive analysis of the \(2 \nu_{1}+\nu_{2}, \nu_{1}+\nu_{2}+\nu_{3}, 3 \nu_{1}, 2 \nu_{1}+\nu_{3}\), and \(\nu_{1}+\) \(2 v_{3}\) band
The ν1+ν3 and the ν1+ν2+ν41+ν5−1 Combination Bands of 13C2H2. Linestrengths, Broadening Parameters, and Pressure Shifts
✍ Scribed by Mitsuhiro Kusaba; Jes Henningsen
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 259 KB
- Volume
- 209
- Category
- Article
- ISSN
- 0022-2852
No coin nor oath required. For personal study only.
✦ Synopsis
The ν 1 + ν 3 and the ν 1 + ν 2 + ν 1 4 + ν -1 5 combination bands of 13 C 2 H 2 at 6521.9 and 6535.1 cm -1 , respectively, are studied with diode laser spectroscopy. Line center wavelengths have been determined with 0.00012-nm standard uncertainty up to J = 40 for ν 1 + ν 3 and up to J = 25 for ν 1 + ν 2 + ν 1 4 + ν -1 5 . Linestrengths are modeled with a Herman-Wallis expansion
Collision broadening parameters are extracted from Voigt fits to the line profiles and can be modeled for both bands by the analytical expression γ = 5.221 -0.0839 |m| + 1.46 exp(-0.45 |m|) MHz/mbar, indicating independence of vibrational state. Collisional narrowing is studied on selected lines and the model dependence of linestrengths and broadening parameters is determined. Pressure shifts are studied in ν 1 + ν 3 , and a characteristic difference in the shifts for the P-branch and the R-branch is explained in terms of a simple ad hoc assumption about the level shifts. These bands have a potential for providing wavelength standards for optical fiber communication.
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