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A precise solution of the rotation bending Schrödinger equation for a triatomic molecule with application to the water molecule
In this paper we report the results of improving the non-rigid bender formulation of the rotation-vibration Hamiltonian of a triatomic molecule [see A. R. Hoy and P. R. Bunker, J. Mol. Spectrosc., 52, 439 (1974)]. This improved Hamiltonian can be diagonalized as before by a combination of numerical...
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Published in: | Journal of molecular spectroscopy 1979, Vol.74 (1), p.1-8 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In this paper we report the results of improving the non-rigid bender formulation of the rotation-vibration Hamiltonian of a triatomic molecule [see A. R. Hoy and P. R. Bunker,
J. Mol. Spectrosc.,
52, 439 (1974)]. This improved Hamiltonian can be diagonalized as before by a combination of numerical integration and matrix diagonalization and it yields rotation-bending energies to high values of the rotational quantum numbers. We have calculated all the rotational energy levels up to
J = 10 for the (
v
1,
v
2,
v
3) states (0, 0, 0) and (0, 1, 0) for both H
2O and D
2O. By least squares fitting to the observations varying seven parameters we have refined the equilibrium structure and force field of the water molecule and have obtained a fit to the 375 experimental energies used with a root mean square deviation of 0.05 cm
−1. The equilibrium bond angle and bond length are determined to be 104.48° and 0.9578 Å respectively. We have also calculated these energy levels using the
ab initio equilibrium geometry and force constants of Rosenberg, Ermler and Shavitt [
J. Chem. Phys.,
65, 4072 (1976)] and this is then the first complete
ab initio calculation of rotation-vibration energy levels of high
J in a polyatomic molecule to this precision. the rms fit of these
ab initio energies to the experimental energies for the H
2O molecule is 2.65 cm
−1. |
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ISSN: | 0022-2852 1096-083X |
DOI: | 10.1016/0022-2852(79)90019-5 |