1997
DOI: 10.1021/jp962817d
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Rotational−Vibrational Levels of Diatomic Molecules Represented by the Tietz−Hua Rotating Oscillator

Abstract: Analytical expressions for the rotational-vibrational energy levels of diatomic molecules represented by the Tietz-Hua rotating oscillator are derived using the Hamilton-Jacoby theory and the Bohr-Sommerfeld quantization rule. In molecules with moderate and large values of rotational and vibrational quantum numbers, the levels are in much better agreement with the results of numerical calculations than the energies obtained from the common model of the rotating Morse oscillator.

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Cited by 79 publications
(67 citation statements)
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“…2 In terms of the wave functions for diatomic molecules, one can calculate the transition dipole matrix elements. [3][4][5] Some authors have investigated analytical solutions of the Schrödinger equation with typical diatomic molecule potential models, such as the Morse potential, 6 Deng−Fan potential, 7-10 Rosen−Morse potential, 11,12 Manning−Rosen potential, [13][14][15][16][17] Wei potential, 18 and Schiöberg potential. 19 In 1932, Rosen and Morse 20 proposed a potential energy function for polyatomic molecules: (1) U RM (r) ϭ B tanh (r/d) Ϫ C sech 2 (r/d)…”
Section: Introductionmentioning
confidence: 99%
“…2 In terms of the wave functions for diatomic molecules, one can calculate the transition dipole matrix elements. [3][4][5] Some authors have investigated analytical solutions of the Schrödinger equation with typical diatomic molecule potential models, such as the Morse potential, 6 Deng−Fan potential, 7-10 Rosen−Morse potential, 11,12 Manning−Rosen potential, [13][14][15][16][17] Wei potential, 18 and Schiöberg potential. 19 In 1932, Rosen and Morse 20 proposed a potential energy function for polyatomic molecules: (1) U RM (r) ϭ B tanh (r/d) Ϫ C sech 2 (r/d)…”
Section: Introductionmentioning
confidence: 99%
“…In Table 1 Spectroscopic constants for some diatomic molecules in the ground electronic state [28,29]: Re is the molecular bond length, ωe the vibrational frequency, the relative atomic mass, D the dissociation energy, ˇ the Morse constant, Be the rotational constant and ωexe the anharmonicity constant. order to achieve this objective we shall suppose that the cross section j l ijkl is a function of the diameters of the colliding molecules, which depend on the rotational and vibrational states (j, i) of the molecules.…”
Section: Molecular Diametersmentioning
confidence: 99%
“…First we calculate the size of these molecules for different excited states according to the model proposed in Refs. [24,28]. Then we evaluate the contribution of rotational states to the size of the oscillator.…”
Section: Introductionmentioning
confidence: 99%
“…In the present work, the spectroscopic parameters for three diatomic molecules (LiH, H 2 , HF) are summarized in table1 [15,16,17], dissociation energy is obtained using (eq.4) compared with another energy. and potential energy curves for two functions began with Varshni potential function for ground 1 Σ + state (eq.…”
Section: Resultsmentioning
confidence: 99%