Using recently published potential energy surfaces, rovibrational energy levels are computed for the ground electronic states of H O and NO , using three-2 2 Ε½ . dimensional discrete variable representation DVR algorithms. Calculations are presented for H O to demonstrate the accuracy of these algor
On the Spectroscopically Determined Potential Energy Surfaces for the Electronic Ground States of NO2and H2O
β Scribed by Jeremy H. Schryber; Oleg L. Polyansky; Per Jensen; Jonathan Tennyson
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 256 KB
- Volume
- 185
- Category
- Article
- ISSN
- 0022-2852
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β¦ Synopsis
Previous spectroscopically determined potentials for both H 2 16 O and NO 2 are discussed. It is shown that a recent H 2 16 O potential energy surface due to D. Xie and G. Yan (1996. Chem. Phys. Lett. 248, 409), which was determined by fits to vibrational term values alone and was claimed to be more accurate than other published spectroscopically determined potentials for this system, actually gives unacceptably poor results for rotationally excited water. Reasons for this failure are discussed and the dangers of relying on vibrational term values alone are emphasized. Previous spectroscopic potentials for ground state NO 2 are all found to have problems with unphysical minima (''holes''). Starting from the potential energy surface for the ground (X Λ2A 1 ) electronic state of NO 2 constructed by S. A. Tashkun and P. Jensen (1994. J. Mol. Spectrosc. 165, 173) using the approximate MORBID approach a suitable starting point for fits using an exact kinetic energy operator approach was constructed. Least-squares fits to 17 potential parameters gives a potential which reproduces 173 vibrational term values with a standard deviation of only 2.8 cm 01 in the lowenergy region (Γ΅10 000 cm 01 ). For many even levels below, and all levels above, approximately 10 000 cm 01 the first excited electronic state (A Λ2B 2 ) perturbs the vibrational energy levels of the ground state. We were unable to fit these levels. Tests show that the resulting effective potential surface has no problems with unphysical holes and gives a reasonable representation of the rotational structure of the low-lying vibrational states of NO 2 . α§ 1997 Academic Press
II. PREVIOUS POTENTIALS
Xie and Yan (XY) (6), and Partridge and Schwenke (7).
There are several reasons for attempting to create an accu-(a) H 2 O
Recently Xie and Yan (6) presented a new spectroscopi-
π SIMILAR VOLUMES
At the correlation-consistent polarized-valence quadruple-zeta complete active space self-consistent field second-order configuration interaction level of ab initio theory (cc-pVQZ CASSCF-SOCI), we calculated 129 points on the ground electronic state potential energy surface of the water dication H(
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
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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