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Lamé spheroconal harmonics in atoms and molecules

机译:原子和分子中的Lamé球锥谐波

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Spheroconal harmonics are the natural basis for the description of asymmetric-molecule rotations (Kramers and Ittmann, Zeitschrift für Physik, 1929, 53, 553; Pi?a, J Mol Str 1999, 493, 159) and also an alternative to the familiar spherical harmonics as the angular part of the Schr?dringer equation eigenfunctions for central potentials (Kalnins et al. SIAM J Appl Math 1976, 30, 360).We have dealt with their properties and matrix evaluation in connection with the rotations of asymmetric molecules (Ley-Koo and Méndez-Fragoso, Rev Mex Fís 2008, 54, 162) and the construction of a generating function for the complete wave functions of the Hydrogen atom (Ley-Koo and Góngora, Int J Quantum Chem 2009, 109, 790). For these cases, the spheroconal harmonics are products of Lamé polynomials Δ~A_(n1)(X1)Δ~B_(n2)(X2) in the respective angular coordinates X1, X2, with n1 + n2 = l, the angular momentum label. More recently during the investigations of the Hydrogen atom (Méndez-Fragoso and Ley-Koo, Int J Quantum Chem. In press) and the rotations of asymmetric molecules (Méndez-Fragoso and Ley-Koo, to be submitted), confined in elliptical cones associated with the spheroconal coordinates in which the respective Schr?dinger equations are separable, we have recognized the need to use and to construct quasi-periodic Lamé functions. In fact, the new boundary conditions require that the angular momentum label becomes noninteger l → λ, and the respective Lamé functions become infinite series. This contribution contains details about the evaluation of the polynomial and quasi-periodic Lamé functions, and their applications in the free particle confined by an elliptical cone with a spherical cap and the harmonic oscillator confined by an elliptical cone.
机译:球面谐波是描述不对称分子旋转的自然基础(Kramers和Ittmann,ZeitschriftfürPhysik,1929,53,553; Pi?a,J Mol Str 1999,493,159),也是熟悉的球面谐波的替代方法谐波作为中心势的Schr?dringer方程本征函数的角部分(Kalnins等人,SIAM J Appl Math 1976,30,360)。我们已经处理了它们的性质以及与不对称分子旋转有关的矩阵评估(Ley -Koo andMéndez-Fragoso,Rev MexFís2008,54,162)和氢原子完整波函数的生成函数的构造(Ley-Koo和Góngora,Int J Quantum Chem 2009,109,790)。对于这些情况,球锥谐波是各自角坐标X1,X2中的Lamé多项式Δ〜A_(n1)(X1)Δ〜B_(n2)(X2)的乘积,其中n1 + n2 = l(角动量标签) 。最近,在研究氢原子(Méndez-Fragoso和Ley-Koo,Int J Quantum Chem。印刷中)和不对称分子的旋转(Méndez-Fragoso和Ley-Koo,待提交)时,它们局限于椭圆锥与球形球形坐标相关联,在球形球形坐标中各个薛定equation方程是可分离的,我们已经认识到需要使用和构造准周期Lamé函数。实际上,新的边界条件要求角动量标记变为非整数l→λ,并且各个Lamé函数变为无穷级数。该贡献包含有关多项式和准周期Lamé函数求值的详细信息,以及它们在由带球形帽的椭圆锥约束的自由粒子和由椭圆锥约束的谐振子中的应用。

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