High-resolution absorption lineshapes for the P(3) and P( 6) transitions of the first overtone (v ϭ 2-0) band of HF at 296 K have been measured using a pair of distributed feedback diode lasers operating near 1.31 and 1.34 m, respectively. Spectral line intensities and self-broadening parameters wer
Diode–Laser Measurements of He-, Ar-, and N2-Broadened HF Lineshapes in the First Overtone Band
✍ Scribed by Shang-I Chou; Douglas S. Baer; Ronald K. Hanson
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 112 KB
- Volume
- 196
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
High-resolution lineshapes of the HF P(3) and P( 6) transitions (2-0 band) have been recorded in a 14.9-cm long absorption cell (T ϭ 296 K) using a pair of (InGaAsP)-distributed feedback diode lasers operating near 1.31 and 1.34 m, respectively. The absorption lineshapes were least-squares fit to Voigt, Rautian, and Galatry profiles to determine the collision widths and velocity-changing collision frequencies for the perturbers He, Ar, and N 2 . Motional narrowing was observed for the He-broadened lineshapes over a range of total pressures from 50 to 646 Torr. The Ar-and N 2 -broadened spectra showed a strong narrowing effect for pressures less than 400 Torr. At higher pressures, narrowing parameters could not be reliably determined due to the relatively large Ar-and N 2 -pressure broadening. The collision widths inferred from Voigt-profile fits were systematically less than those determined from Rautian and Galatry fits (up to 25% for the He-broadened P(6) transition). The measured pressure-induced broadening and shift coefficients were compared with other experimental data and full-quantal close-coupling (CC) scattering cross-section calculations. The measured Ar-broadening half-widths were in excellent agreement with calculated values, while the measured shifts were 10 and 20% less than calculated values for the P(3) and P( 6) transitions, respectively. The measured N 2 -broadening and shift coefficients agree reasonably well with values determined from previous experiments.
📜 SIMILAR VOLUMES
Ar-broadening coefficients have been measured for 29 lines of \(\mathrm{HCN}\) in the \(P, Q\), and \(R\) branches of the \(\nu_{2}\) band, using a tunable diode-laser spectrometer. These lines with \(J\) values ranging from 1 to 25 are located in the spectral range \(640-790 \mathrm{~cm}^{-1}\). Th
N 2 -broadening coefficients have been measured for 35 lines of C 2 H 4 in the 7 fundamental transition, using a tunable diode-laser spectrometer. These lines with 3 Յ JЉ Յ 23, 0 Յ K Љ a Յ 4, and 1 Յ K Љ c Յ 22 are located in the spectral range 880 -1024 cm Ϫ1 . The collisional half-widths are obtai
\(\mathrm{N}_{2}\)-broadening coefficients have been measured for 28 lines of \(\mathrm{HCN}\) at \(203 \mathrm{~K}\) in the \(P, Q\). and \(R\) branches of the \(\nu_{2}\) band, using a tunable diode-laser spectrometer. Semiclassical calculations of these collisional broadenings have been performed