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1: 33.23 Methods of Computation
The power-series expansions of §§33.6 and 33.19 converge for all finite values of the radii ρ and r , respectively, and may be used to compute the regular and irregular solutions. … Thus the regular solutions can be computed from the power-series expansions (§§33.6, 33.19) for small values of the radii and then integrated in the direction of increasing values of the radii. … This implies decreasing for the regular solutions and increasing for the irregular solutions of §§33.2(iii) and 33.14(iii). …
2: 33.2 Definitions and Basic Properties
§33.2(i) Coulomb Wave Equation
§33.2(ii) Regular Solution F ( η , ρ )
§33.2(iii) Irregular Solutions G ( η , ρ ) , H ± ( η , ρ )
As in the case of F ( η , ρ ) , the solutions H ± ( η , ρ ) and G ( η , ρ ) are analytic functions of ρ when 0 < ρ < . …
3: 33.14 Definitions and Basic Properties
§33.14(i) Coulomb Wave Equation
§33.14(ii) Regular Solution f ( ϵ , ; r )
4: 33.20 Expansions for Small | ϵ |
§33.20(ii) Power-Series in ϵ for the Regular Solution
5: 1.13 Differential Equations
A regular Sturm-Liouville system will only have solutions for certain (real) values of λ , these are eigenvalues. …
6: 16.21 Differential Equation
16.21.1 ( ( 1 ) p m n z ( ϑ a 1 + 1 ) ( ϑ a p + 1 ) ( ϑ b 1 ) ( ϑ b q ) ) w = 0 ,
With the classification of §16.8(i), when p < q the only singularities of (16.21.1) are a regular singularity at z = 0 and an irregular singularity at z = . When p = q the only singularities of (16.21.1) are regular singularities at z = 0 , ( 1 ) p m n , and . A fundamental set of solutions of (16.21.1) is given by …
7: 2.6 Distributional Methods
§2.6(iv) Regularization
However, in the theory of generalized functions (distributions), there is a method, known as “regularization”, by which these integrals can be interpreted in a meaningful manner. …For rigorous derivations of these results and also order estimates for δ n ( x ) , see Wong (1979) and Wong (1989, Chapter 6).
8: 33.22 Particle Scattering and Atomic and Molecular Spectra
For scattering problems, the interior solution is then matched to a linear combination of a pair of Coulomb functions, F ( η , ρ ) and G ( η , ρ ) , or f ( ϵ , ; r ) and h ( ϵ , ; r ) , to determine the scattering S -matrix and also the correct normalization of the interior wave solutions; see Bloch et al. (1951). …
9: 14.2 Differential Equations
§14.2(i) Legendre’s Equation
§14.2(ii) Associated Legendre Equation
§14.2(iii) Numerically Satisfactory Solutions
Equation (14.2.2) has regular singularities at x = 1 , 1 , and , with exponent pairs { 1 2 μ , 1 2 μ } , { 1 2 μ , 1 2 μ } , and { ν + 1 , ν } , respectively; compare §2.7(i). … Hence they comprise a numerically satisfactory pair of solutions2.7(iv)) of (14.2.2) in the interval 1 < x < 1 . …
10: Bibliography B
  • W. G. C. Boyd and T. M. Dunster (1986) Uniform asymptotic solutions of a class of second-order linear differential equations having a turning point and a regular singularity, with an application to Legendre functions. SIAM J. Math. Anal. 17 (2), pp. 422–450.