Abstract:The relativistic solutions of the Klein-Gordon equation comprising an interaction of the generalized inversely quadratic Yukawa potential mixed linearly with the hyperbolic Schiöberg molecular potential is achieved employing the idea of parametric Nikiforov-Uvarov and the Greene-Aldrich approximation scheme. The energy spectra and the corresponding normalized wave functions are derived regarding the hypergeometric function in a closed form for arbitrary
ℓ
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“…Because of their diverse uses, solutions to the relativistic and non-relativistic wave equations have been used in various quantum potential interactions employing various methodologies [22,23]. These approaches include the 1/N shifted expansion procedure [24], the Nikiforov-Uvarov approach [25][26][27], the asymptotic iteration method [28], the factorization method [29,30], the formula technique [31], the supersymmetric approach [32,33], the ansatz methodology [34], the Laplace transform approach [35,36], the functional analysis approach [37,38], the appropriate quantization rule [39], and others [40,41]. For many solvable quantum frameworks, the hypergeometric Nikiforov-Uvarov technique has demonstrated its ability to determine the exact energy levels of bound states [42].…”
The parametric Nikiforov–Uvarov approach and the Greene–Aldrich approximation scheme were used to achieve approximate analytical solutions to the Schrödinger equation, involving an interaction of the modified deformed Hylleraas potential mixed linearly with the improved Frost–Musulin diatomic molecular potential. For each ℓ-state, the energy spectra and normalized wave functions were generated from the hypergeometric function in the closed form. The thermal properties of such a system, including the vibrational partition function, vibrational mean energy, vibrational mean free energy, vibrational specific heat capacity, and vibrational entropy, were then calculated for the selected diatomic molecules using their experimental spectroscopic parameters. Furthermore, the peculiar conditions of this potential were evaluated, and their energy eigenvalues were calculated for the purpose of comparison. The acquired results were found to be in reasonable agreement with those reported in the literature.
“…Because of their diverse uses, solutions to the relativistic and non-relativistic wave equations have been used in various quantum potential interactions employing various methodologies [22,23]. These approaches include the 1/N shifted expansion procedure [24], the Nikiforov-Uvarov approach [25][26][27], the asymptotic iteration method [28], the factorization method [29,30], the formula technique [31], the supersymmetric approach [32,33], the ansatz methodology [34], the Laplace transform approach [35,36], the functional analysis approach [37,38], the appropriate quantization rule [39], and others [40,41]. For many solvable quantum frameworks, the hypergeometric Nikiforov-Uvarov technique has demonstrated its ability to determine the exact energy levels of bound states [42].…”
The parametric Nikiforov–Uvarov approach and the Greene–Aldrich approximation scheme were used to achieve approximate analytical solutions to the Schrödinger equation, involving an interaction of the modified deformed Hylleraas potential mixed linearly with the improved Frost–Musulin diatomic molecular potential. For each ℓ-state, the energy spectra and normalized wave functions were generated from the hypergeometric function in the closed form. The thermal properties of such a system, including the vibrational partition function, vibrational mean energy, vibrational mean free energy, vibrational specific heat capacity, and vibrational entropy, were then calculated for the selected diatomic molecules using their experimental spectroscopic parameters. Furthermore, the peculiar conditions of this potential were evaluated, and their energy eigenvalues were calculated for the purpose of comparison. The acquired results were found to be in reasonable agreement with those reported in the literature.
“…In particular, we can further analyze and discuss the problems related to the hydrogen atom through the relationship between the spatial harmonic oscillator and the hydrogen atom. In recent years, using the double wave function method, asymptotic iteration method, the Fourier transform method, and so on, some researchers study the problem of the onedimensional or isotropous quantum harmonic oscillator, in which significant results have been obtained [1][2][3][4][5][6][7][8][9][10][11][12][13][14]. In this paper, by the method of separating variables, the steady-state Schrodinger equation of a potential well of an infinite elliptic parabola is solved, and quantum properties of the harmonic oscillator in the potential well of an infinite elliptic parabola are analyzed and studied.…”
The harmonic oscillator is an important and typical physical model in quantum mechanics and quantum optics. It is very important and widely used and has been confirmed by the development and application of science and technology. The harmonic oscillator in the elliptic paraboloid potential is studied and effects of the elliptic oblateness on the harmonic oscillator in the elliptic paraboloid potential are revealed. The energy of the harmonic oscillator in the elliptical paraboloid potential is quantized, which is described by two quantum numbers n, and m. Generally speaking, the maximum value of the probability density peak decreases as the extremum number of the probability density increases. However, this reduction is with oscillations and fluctuations, which shows even a maximum structure for the smaller quantum number. For the elliptic paraboloid potential, the spatial distribution of the probability density on different cutting surfaces is various. The flatter the ellipse is, the greater the probability density of the ellipse center, and the smaller the extreme of the edge peak of the probability density will be.
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