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Pseudospectral method of solution of the Schrodinger equation for the Kratzer and pseudoharmonic potentials with nonclassical polynomials and applications to realistic diatom potentials

机译:Kratzer和伪谐波潜力的Schrodinger方程求解伪谱法,用非分化多项式和应用于现实硅藻电位

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The pseudoharmonic and Kratzer potentials have been extensively employed by numerous workers to model the vibrational states of diatomic molecules. These potentials belong to SUperSYmmetric (SUSY) quantum mechanics and the eigenvalues of the Schrodinger equation are known. The energy eigenvalues of the Schrodinger equation for the pseudoharmonic and Kratzer potentials have been determined with different numerical methods as a benchmark of the numerical schemes. We employ a pseudospectral method based on a quadrature grid defined with a nonclassical polynomial basis set. This basis set is defined orthogonal with respect to the square of ground state wavefunction as the weight function. A discrete matrix representation of the Hamiltonian of dimension N is constructed and vibrational energies are calculated with the numerical diagonalization of this matrix. This pseudospectral method is employed to calculate the vibrational energy levels of H-2, CO and NO modelled with the pseudoharmonic and Kratzer potentials in comparison with the more realistic Morse potential. The vibrational energy eigenstates for H-2 with a realistic quantum mechanical potential and an approximate Morse potential are also calculated. The oversimplified pseudoharmonic and Kratzer potentials are useful for benchmarking numerical methods. However, they represent potential energy curves that can deviate drastically from more exact potentials such as the Morse potential.
机译:众多工人的伪谐波和Kratzer潜力已被广泛使用,以模拟抗原硅分子的振动状态。这些电位属于超对称(SASY)量子力学,并且已知施罗德格方程的特征值是已知的。已经用不同的数值方法确定了伪谐波和Kratzer电位的Schrodinger方程的能量特征值,以不同的数值方法作为数值方案的基准。我们采用基于具有非分类多项式基础集定义的正交网格的伪谱方法。这种基础组与作为权重函数的地面挥发性的正方形定义正交。构造尺寸N的哈密尔顿的离散矩阵表示,并用该矩阵的数值对角计算计算振动能量。该假谱法用于计算H-2,CO,与伪谐波和Kratzer电位建模的振动能量水平相比,与更现实的摩尔斯潜力相比。还计算了具有现实量子力学电位的H-2的振动能量特征,以及近似摩尔斯潜力。过度简化的伪臂和Kratzer电位对于基准测试数值方法非常有用。然而,它们代表潜在的能量曲线,可以从更具精确的潜力(例如Morse潜力)均匀地偏离。

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