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1: 23.9 Laurent and Other Power Series
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c 2 = 1 20 ⁒ g 2 ⁑ ,
β–ΊExplicit coefficients c n in terms of c 2 and c 3 are given up to c 19 in Abramowitz and Stegun (1964, p. 636). … β–ΊAlso, Abramowitz and Stegun (1964, (18.5.25)) supplies the first 22 terms in the reverted form of (23.9.2) as 1 / ⁑ ( z ) 0 . …
2: 5.11 Asymptotic Expansions
β–ΊWrench (1968) gives exact values of g k up to g 20 . …For explicit formulas for g k in terms of Stirling numbers see Nemes (2013a), and for asymptotic expansions of g k as k see Boyd (1994) and Nemes (2015a). …
3: Bibliography G
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  • W. Gautschi (1994) Algorithm 726: ORTHPOL — a package of routines for generating orthogonal polynomials and Gauss-type quadrature rules. ACM Trans. Math. Software 20 (1), pp. 21–62.
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  • A. Gil, J. Segura, and N. M. Temme (2014) Algorithm 939: computation of the Marcum Q-function. ACM Trans. Math. Softw. 40 (3), pp. 20:1–20:21.
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  • H. W. Gould (1972) Explicit formulas for Bernoulli numbers. Amer. Math. Monthly 79, pp. 44–51.
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  • Ya. I. GranovskiΔ­, I. M. Lutzenko, and A. S. Zhedanov (1992) Mutual integrability, quadratic algebras, and dynamical symmetry. Ann. Phys. 217 (1), pp. 1–20.
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  • C. H. Greene, U. Fano, and G. Strinati (1979) General form of the quantum-defect theory. Phys. Rev. A 19 (4), pp. 1485–1509.
  • 4: 18.39 Applications in the Physical Sciences
    β–ΊHere are three examples of solutions for (18.39.8) for explicit choices of V ⁒ ( x ) and with the ψ n ⁒ ( x ) corresponding to the discrete spectrum. … β–ΊThe orthonormal stationary states and corresponding eigenvalues are then of the formβ–ΊExplicit normalization is given for the second, third, and fourth of these, paragraphs c) and d), below. … β–Ίthus recapitulating, for Z = 1 , line 11 of Table 18.8.1, now shown with explicit normalization for the measure d r . … β–ΊThese, taken together with the infinite sets of bound states for each l , form complete sets. …