A continuously tunable single-frequency color-center laser spectrometer has been used to rovibrationally analyze the static gas-phase spectrum of the ~1 (C-H stretching) vibration in HCN---H35Cl providing molecular parameters: VI = 3309.0286(3) cm-l , B1 = 2007.37(36) MHz and Dj = 3.51(13) X 10m3 MH
Rovibrational Spectroscopy of C35Cl4
โ Scribed by S.L. Xu; R.S. Mcdowell; S.W. Sharpe; B.J. Krohn
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 576 KB
- Volume
- 173
- Category
- Article
- ISSN
- 0022-2852
No coin nor oath required. For personal study only.
โฆ Synopsis
High-resolution rotationally resolved infrared spectra of the spherical-top rotor (\mathrm{C}^{35} \mathrm{Cl}{4}) (in samples of natural isotopic composition ) were obtained both in static cells by FTIR spectroscopy ( (\nu{4}, \nu_{1}) (\left.+\nu_{4}\right)) and in a supersonically cooled expansion with tunable diode lasers ( (\nu_{3}) ). For the (\nu_{3}) fundamental at (799 \mathrm{~cm}^{-1}), quantum assignments were made for individual transitions from (P(20)) to (R(24)), and the partially resolved (Q) branch was matched with synthesized spectra. The bands (\nu_{4}) ( 316 (\left.\mathrm{cm}^{-1}\right)) and (v_{1}+v_{4}\left(774 \mathrm{~cm}^{-1}\right)) exhibit much reduced manifold splitting. and scalar fits were made to the (R(24)-R(70)) and (P(38)-R(56)) frequencies. respectively. The (\nu_{3} /\left(\nu_{1}+\nu_{4}\right)) Fermi dyad yields Coriolis constants (\zeta_{3}=0.621) and (\zeta_{4}^{\prime}=-0.145) that satisfy the harmonic sum rule, but are perturbed by the Fermi resonance and are inconsistent with intramolecular force fields previously reported based on isotope shifts in matrix spectra. The true bending-mode Coriolis constant (\zeta_{4}) (=-0.414), obtained from analysis of the isolated and unperturbed (v_{4}) band, agrees well with the isotope shifts. (\mathrm{CCl}{4}) and other tetrahedral (X Y{4}) molecules are shown to vibrate according to a simple vector-displacement normal-mode model for which (\zeta_{3} \approx 4 /\left[3\left(m_{X} / m_{Y}\right)+4\right]).
(c) 1995 Academic Press. Inc.
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