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11: Bibliography R
  • M. Rahman (1981) A non-negative representation of the linearization coefficients of the product of Jacobi polynomials. Canad. J. Math. 33 (4), pp. 915–928.
  • J. Raynal (1979) On the definition and properties of generalized 6 - j  symbols. J. Math. Phys. 20 (12), pp. 2398–2415.
  • W. H. Reid (1995) Integral representations for products of Airy functions. Z. Angew. Math. Phys. 46 (2), pp. 159–170.
  • W. H. Reid (1997a) Integral representations for products of Airy functions. II. Cubic products. Z. Angew. Math. Phys. 48 (4), pp. 646–655.
  • W. H. Reid (1997b) Integral representations for products of Airy functions. III. Quartic products. Z. Angew. Math. Phys. 48 (4), pp. 656–664.
  • 12: Bibliography B
  • G. Backenstoss (1970) Pionic atoms. Annual Review of Nuclear and Particle Science 20, pp. 467–508.
  • Á. Baricz and T. K. Pogány (2013) Integral representations and summations of the modified Struve function. Acta Math. Hungar. 141 (3), pp. 254–281.
  • K. L. Bell and N. S. Scott (1980) Coulomb functions (negative energies). Comput. Phys. Comm. 20 (3), pp. 447–458.
  • W. G. Bickley (1935) Some solutions of the problem of forced convection. Philos. Mag. Series 7 20, pp. 322–343.
  • P. L. Butzer and M. Hauss (1992) Riemann zeta function: Rapidly converging series and integral representations. Appl. Math. Lett. 5 (2), pp. 83–88.
  • 13: Bibliography G
  • A. Gil, J. Segura, and N. M. Temme (2004c) Integral representations for computing real parabolic cylinder functions. Numer. Math. 98 (1), pp. 105–134.
  • 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.
  • H. W. Gould (1960) Stirling number representation problems. Proc. Amer. Math. Soc. 11 (3), pp. 447–451.
  • K. I. Gross and R. A. Kunze (1976) Bessel functions and representation theory. I. J. Functional Analysis 22 (2), pp. 73–105.
  • E. Grosswald (1985) Representations of Integers as Sums of Squares. Springer-Verlag, New York.
  • 14: Bibliography P
  • R. B. Paris and S. Cang (1997) An asymptotic representation for ζ ( 1 2 + i t ) . Methods Appl. Anal. 4 (4), pp. 449–470.
  • J. Patera and P. Winternitz (1973) A new basis for the representation of the rotation group. Lamé and Heun polynomials. J. Mathematical Phys. 14 (8), pp. 1130–1139.
  • B. Pichon (1989) Numerical calculation of the generalized Fermi-Dirac integrals. Comput. Phys. Comm. 55 (2), pp. 127–136.
  • R. Piessens (1982) Automatic computation of Bessel function integrals. Comput. Phys. Comm. 25 (3), pp. 289–295.
  • W. H. Press and S. A. Teukolsky (1990) Elliptic integrals. Computers in Physics 4 (1), pp. 92–96.
  • 15: 11.6 Asymptotic Expansions
    11.6.3 0 z 𝐊 0 ( t ) d t 2 π ( ln ( 2 z ) + γ ) 2 π k = 1 ( 1 ) k + 1 ( 2 k ) ! ( 2 k 1 ) ! ( k ! ) 2 ( 2 z ) 2 k , | ph z | π δ ,
    11.6.4 0 z 𝐌 0 ( t ) d t + 2 π ( ln ( 2 z ) + γ ) 2 π k = 1 ( 2 k ) ! ( 2 k 1 ) ! ( k ! ) 2 ( 2 z ) 2 k , | ph z | 1 2 π δ ,
    c 3 ( λ ) = 20 λ 6 4 λ 4 ,
    These and higher coefficients c k ( λ ) can be computed via the representations in Nemes (2015b). …
    16: 14.30 Spherical and Spheroidal Harmonics
    Explicit Representation
    14.30.8 0 2 π 0 π Y l 1 , m 1 ( θ , ϕ ) ¯ Y l 2 , m 2 ( θ , ϕ ) sin θ d θ d ϕ = δ l 1 , l 2 δ m 1 , m 2 .
    See also (34.3.22), and for further related integrals see Askey et al. (1986). … For a series representation of the product of two Dirac deltas in terms of products of spherical harmonics see §1.17(iii). …