The potential energy surface for the electronic ground state of CO 2 is refined by means of a two-step variational procedure using the exact rovibrational Hamiltonian in the bond length-bond angle coordinates. In the refinement, the observed rovibrational energy levels for J = 0-4 below 16,000 cm -1
A Refined Potential Energy Surface for the Electronic Ground State of the Water Molecule
β Scribed by P. Jensen; S.A. Tashkun; V.G. Tyuterev
- Publisher
- Elsevier Science
- Year
- 1994
- Tongue
- English
- Weight
- 949 KB
- Volume
- 168
- Category
- Article
- ISSN
- 0022-2852
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β¦ Synopsis
We report here an optimization of the parameters in an analytical representation of the potential energy function for the electronic ground state of the water molecule on the basis of experimental data. The calculations are carried out with the MORBID (Morse Oscillator Rigid Bender Internal Dynamics) computer program (P. Jensen. J. Mol. Spectrosc. 128, 478-501, 1988; J. Chem. Soc. Faraday. Trans. 2 84, 1315-1340, 1988; in "Methods in Computational Molecular Physics," S. Wilson and G. H. F. Diercksen, Eds., Plenum Press, New York, 1992 ). In the least-squares fitting, we adjusted 28 parameters ( and constrained one parameter to its ab initio value) to fit a total of 2383 rotation-vibration energy spacings involving rotational spacings with (J \leqslant 10) in 120 vibrational states of the 10 isotopomers (\mathrm{H}{2}{ }^{16} \mathrm{O}, \mathrm{D}{2}{ }^{16} \mathrm{O}, \mathrm{T}{2}{ }^{16} \mathrm{O}, \mathrm{HD}^{16} \mathrm{O}, \mathrm{HT}^{16} \mathrm{O}, \mathrm{H}{2}{ }^{17} \mathrm{O}, \mathrm{HD}^{17} \mathrm{O}, \mathrm{H}{2}{ }^{18} \mathrm{O}, \mathrm{D}{2}{ }^{18} \mathrm{O}), and (H{ }^{18} \mathrm{O}). The root-mean-square deviation of this fitting was (0.36 \mathrm{~cm}^{-1}). The potential energy function obtained in the present work represents an improvement of the function determined previously (P. Jensen, J. Mol. Spectrosc. 133, 438-460, 1989) on the basis of input data involving (J \leqslant 2) for six isotopomers of water. In the new fitting reported here, we obtain the equilibrium bond length of the water molecule as (r_{i 2}=0.957848) ( 16 ) (\AA) and the equilibrium bond angle as (\alpha_{c}=104.5424(46)^{\circ}) (one standard error in units of the last digit given in parentheses). We consider this to be the most accurate equilibrium geometry currently available for water. (Γ§ 1994 Academic Press. Inc.
π SIMILAR VOLUMES
We report here the determination of a new potential energy surface for the electronic ground state of the H 2 Te molecule by fitting to an extensive set of very recent experimental spectroscopic data (see J.-M. Flaud, P. Arcas, H. Bu Β¨rger, O. Polanz, and L. Halonen, J. Mol. Spectrosc. 183, 310-335
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