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21: 3.8 Nonlinear Equations
For the computation of zeros of Bessel functions, Coulomb functions, and conical functions as eigenvalues of finite parts of infinite tridiagonal matrices, see Grad and Zakrajšek (1973), Ikebe (1975), Ikebe et al. (1991), Ball (2000), and Gil et al. (2007a, pp. 205–213). … Initial approximations to the zeros can often be found from asymptotic or other approximations to f ( z ) , or by application of the phase principle or Rouché’s theorem; see §1.10(iv). …
3.8.15 p ( x ) = ( x 1 ) ( x 2 ) ( x 20 )
Consider x = 20 and j = 19 . We have p ( 20 ) = 19 ! and a 19 = 1 + 2 + + 20 = 210 . …
22: 33.22 Particle Scattering and Atomic and Molecular Spectra
§33.22(i) Schrödinger Equation
§33.22(iv) Klein–Gordon and Dirac Equations
§33.22(vi) Solutions Inside the Turning Point
23: Bibliography N
  • D. Naylor (1989) On an integral transform involving a class of Mathieu functions. SIAM J. Math. Anal. 20 (6), pp. 1500–1513.
  • W. J. Nellis and B. C. Carlson (1966) Reduction and evaluation of elliptic integrals. Math. Comp. 20 (94), pp. 223–231.
  • T. D. Newton (1952) Coulomb Functions for Large Values of the Parameter η . Technical report Atomic Energy of Canada Limited, Chalk River, Ontario.
  • E. W. Ng and M. Geller (1969) A table of integrals of the error functions. J. Res. Nat. Bur. Standards Sect B. 73B, pp. 1–20.
  • C. J. Noble (2004) Evaluation of negative energy Coulomb (Whittaker) functions. Comput. Phys. Comm. 159 (1), pp. 55–62.
  • 24: 33.8 Continued Fractions
    §33.8 Continued Fractions
    If we denote u = F / F and p + i q = H + / H + , then …
    F = u F ,
    G = q 1 ( u p ) F ,
    G = q 1 ( u p p 2 q 2 ) F .
    25: 33.16 Connection Formulas
    §33.16(i) F and G in Terms of f and h
    §33.16(ii) f and h in Terms of F and G when ϵ > 0
    §33.16(iii) f and h in Terms of W κ , μ ( z ) when ϵ < 0
    §33.16(iv) s and c in Terms of F and G when ϵ > 0
    §33.16(v) s and c in Terms of W κ , μ ( z ) when ϵ < 0
    26: 33 Coulomb Functions
    Chapter 33 Coulomb Functions
    27: 5.20 Physical Applications
    Rutherford Scattering
    In nonrelativistic quantum mechanics, collisions between two charged particles are described with the aid of the Coulomb phase shift ph Γ ( + 1 + i η ) ; see (33.2.10) and Clark (1979). …
    28: 8 Incomplete Gamma and Related
    Functions
    29: 28 Mathieu Functions and Hill’s Equation
    30: 33.20 Expansions for Small | ϵ |
    §33.20(i) Case ϵ = 0
    §33.20(ii) Power-Series in ϵ for the Regular Solution
    §33.20(iii) Asymptotic Expansion for the Irregular Solution
    §33.20(iv) Uniform Asymptotic Expansions
    For a comprehensive collection of asymptotic expansions that cover f ( ϵ , ; r ) and h ( ϵ , ; r ) as ϵ 0 ± and are uniform in r , including unbounded values, see Curtis (1964a, §7). …