We ulculate the rotatlonnl madnew moments and the correspondmEg\_factors for water and ammoma Our results are g,, = 0.39i,g,,,, ; 0 769 andxiz = 0 345 for water and gXx = g experImental values a.r'eilx = 0 , = 0 69 and gzz = 0 51 for ammonla The 585,g for ammoma yy = 0 742 and gzz = 0 666 for w,% an
Calculation of High Rotation Energies of the Water Molecule Using the Generating Function Model
โ Scribed by V.G. Tyuterev; V.I. Starikov; S.A. Tashkun; S.N. Mikhailenko
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 1015 KB
- Volume
- 170
- Category
- Article
- ISSN
- 0022-2852
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โฆ Synopsis
The previously developed generating function model is applied in this paper to fitting high rotational levels of the water molecule in the domain of rotational quantum numbers where the standard power series expansion of the rotational Hamiltonian has a slow rate of convergence or even diverges. This model typically provides a considerable improvement in the standard deviation of fit with respect both to the conventional polynomial Hamiltonian and to the Pade-type Hamiltonian (with the same or fewer number of adjustable parameters). Ground state rotational levels recovered by Flaud at al. (Mol. Phys. 32, 499-52| (1976)) from flame spectra are fitted with accuracy near that of the experimental values: weighted standard deviation (\chi=1.8) for 422 levels up to (J, k_{a} \leqslant 20) and (x=2.1) for all available levels up to (J \leqslant 35). New ground state data reported by Toth (J.Op. Soc: B 8, 2236-2255 (1991)) are fitted up to (J, K_{a} \leqslant 10) with RMS (=4 \times 10^{-5}) (\mathrm{cm}^{-1}). Tests of extrapolation properties of the generating function model are discussed. In certain cases the accuracy of extrapolation was better than the accuracy of fitting with the standard rotational Hamiltonian. (\quad 1545) Academic Press. inc.
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