ROVIBRATIONAL HAMILTONIAN FOR TRIATOMIC MOLECULE IN RADAV'S COORDINATES

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1991

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Ohio State University

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{Makarewicz}1 has shown that the rovibrational Hamiltonian of a symmetrical triatomic molecule takes a simple form when expressed in terms of Radau’s coordinates r1,r2 and 0, very similar to the two valence and bond angle coordinates. This Hamiltonian can be further simplified if the two coordinates r1 and r2 are frozen. Taking then a simple model potential function, the eigenvalues of this simplified Hamiltonian can be determined exactly for each K value.2 In this paper a trial rovibrational Hamiltonian for triatomic molecules has been derived starting from the one proposed by Makarewicz.2 However, ΔK>0 matrix elements arising from the rotational Hamiltonian were treated rigorously and phenomenological distortion-like parameters were introduced. The Hamiltonian thereby obtained can account for the rotational levels up to J=15 of $ H_{2}O$ in its ground vibrational state3 with an R.M.S. deviation of 4.9 ×10−3cm−1, using 30 parameters. In the first excited vibrational state v2=1 of the same molecule,4 the rotational levels up to J = 9 are reproduced with an R.M.S. deviation of 1.4×10−3cm−1, using 22 parameters. These results will be discussed and we hope to be able to achieve a better understanding of the four-fold clustering.

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1J. Makarewicz, J. Phys. B: At. Mol. Phys. 21, 1803-1819 (1988). 2J. Makarewicz, J. Phys. B: At. Mol. Phys. 21, 3633-3651 (1988). 3J.-M. Flaud, C. Camy-Peyret and J. P. Maillard, Mol. Phys. 32, 499-521 (1976). 4C. Camy-Peyret, J.-N. Flaud, J. P. Maillard and G. Guelachvili, Mol. Phys. 33, 1641-1650 (1977).""


Author Institution: Laboratoire de Physique Mol{'e}culaire et Atmosph{'e}rique, Tour 13, Universit{'e} Pierre et Marie Curie et CNRS

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