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in terms of Bessel functions of variable order

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11: 10.17 Asymptotic Expansions for Large Argument
§10.17 Asymptotic Expansions for Large Argument
§10.17(iii) Error Bounds for Real Argument and Order
If these expansions are terminated when k = 1 , then the remainder term is bounded in absolute value by the first neglected term, provided that max ( ν 1 2 , 1 ) . … For higher re-expansions of the remainder terms see Olde Daalhuis and Olver (1995a) and Olde Daalhuis (1995, 1996).
12: 18.15 Asymptotic Approximations
The latter expansions are in terms of Bessel functions, and are uniform in complex z -domains not containing neighborhoods of 1. … These expansions are in terms of Bessel functions and modified Bessel functions, respectively. …
In Terms of Elementary Functions
In Terms of Bessel Functions
In Terms of Airy Functions
13: 10.41 Asymptotic Expansions for Large Order
§10.41 Asymptotic Expansions for Large Order
§10.41(ii) Uniform Expansions for Real Variable
14: 13.9 Zeros
When a < 0 and b > 0 let ϕ r , r = 1 , 2 , 3 , , be the positive zeros of M ( a , b , x ) arranged in increasing order of magnitude, and let j b 1 , r be the r th positive zero of the Bessel function J b 1 ( x ) 10.21(i)). … … For fixed a and z in the function M ( a , b , z ) has only a finite number of b -zeros. …
15: 10.22 Integrals
Orthogonality
Orthogonality
See also §1.17(ii) for an integral representation of the Dirac delta in terms of a product of Bessel functions. … Additional infinite integrals over the product of three Bessel functions (including modified Bessel functions) are given in Gervois and Navelet (1984, 1985a, 1985b, 1986a, 1986b). … For collections of integrals of the functions J ν ( z ) , Y ν ( z ) , H ν ( 1 ) ( z ) , and H ν ( 2 ) ( z ) , including integrals with respect to the order, see Andrews et al. (1999, pp. 216–225), Apelblat (1983, §12), Erdélyi et al. (1953b, §§7.7.1–7.7.7 and 7.14–7.14.2), Erdélyi et al. (1954a, b), Gradshteyn and Ryzhik (2000, §§5.5 and 6.5–6.7), Gröbner and Hofreiter (1950, pp. 196–204), Luke (1962), Magnus et al. (1966, §3.8), Marichev (1983, pp. 191–216), Oberhettinger (1974, §§1.10 and 2.7), Oberhettinger (1990, §§1.13–1.16 and 2.13–2.16), Oberhettinger and Badii (1973, §§1.14 and 2.12), Okui (1974, 1975), Prudnikov et al. (1986b, §§1.8–1.10, 2.12–2.14, 3.2.4–3.2.7, 3.3.2, and 3.4.1), Prudnikov et al. (1992a, §§3.12–3.14), Prudnikov et al. (1992b, §§3.12–3.14), Watson (1944, Chapters 5, 12, 13, and 14), and Wheelon (1968).
16: Bibliography T
  • N. M. Temme (1990b) Uniform asymptotic expansions of a class of integrals in terms of modified Bessel functions, with application to confluent hypergeometric functions. SIAM J. Math. Anal. 21 (1), pp. 241–261.
  • N. M. Temme (1994c) Steepest descent paths for integrals defining the modified Bessel functions of imaginary order. Methods Appl. Anal. 1 (1), pp. 14–24.
  • I. J. Thompson and A. R. Barnett (1986) Coulomb and Bessel functions of complex arguments and order. J. Comput. Phys. 64 (2), pp. 490–509.
  • I. J. Thompson and A. R. Barnett (1987) Modified Bessel functions I ν ( z ) and K ν ( z ) of real order and complex argument, to selected accuracy. Comput. Phys. Comm. 47 (2-3), pp. 245–257.
  • I. J. Thompson (2004) Erratum to “COULCC: A continued-fraction algorithm for Coulomb functions of complex order with complex arguments”. Comput. Phys. Comm. 159 (3), pp. 241–242.
  • 17: 11.10 Anger–Weber Functions
    §11.10 Anger–Weber Functions
    The Anger and Weber functions satisfy the inhomogeneous Bessel differential equation …
    §11.10(vi) Relations to Other Functions
    §11.10(viii) Expansions in Series of Products of Bessel Functions
    where the prime on the second summation symbols means that the first term is to be halved. …
    18: 18.39 Applications in the Physical Sciences
    The functions ϕ n are expressed in terms of Romanovski–Bessel polynomials, or Laguerre polynomials by (18.34.7_1). …
    a) Spherical Radial Coulomb Wave Functions Expressed in terms of Laguerre OP’s
    d) Radial Coulomb Wave Functions Expressed in Terms of the Associated Coulomb–Laguerre OP’s
    Discretized and Continuum Expansions of Scattering Eigenfunctions in terms of Pollaczek Polynomials: J-matrix Theory
    The fact that non- L 2 continuum scattering eigenstates may be expressed in terms or (infinite) sums of L 2 functions allows a reformulation of scattering theory in atomic physics wherein no non- L 2 functions need appear. …
    19: Bibliography W
  • A. D. Wheelon (1968) Tables of Summable Series and Integrals Involving Bessel Functions. Holden-Day, San Francisco, CA.
  • M. E. Wojcicki (1961) Algorithm 44: Bessel functions computed recursively. Comm. ACM 4 (4), pp. 177–178.
  • R. Wong and T. Lang (1991) On the points of inflection of Bessel functions of positive order. II. Canad. J. Math. 43 (3), pp. 628–651.
  • R. Wong and Y.-Q. Zhao (2003) Estimates for the error term in a uniform asymptotic expansion of the Jacobi polynomials. Anal. Appl. (Singap.) 1 (2), pp. 213–241.
  • E. M. Wright (1940b) The generalized Bessel function of order greater than one. Quart. J. Math., Oxford Ser. 11, pp. 36–48.
  • 20: 10.74 Methods of Computation
    In the case of the spherical Bessel functions the explicit formulas given in §§10.49(i) and 10.49(ii) are terminating cases of the asymptotic expansions given in §§10.17(i) and 10.40(i) for the Bessel functions and modified Bessel functions. … If values of the Bessel functions J ν ( z ) , Y ν ( z ) , or the other functions treated in this chapter, are needed for integer-spaced ranges of values of the order ν , then a simple and powerful procedure is provided by recurrence relations typified by the first of (10.6.1). …
    Fourier–Bessel Expansion
    §10.74(viii) Functions of Imaginary Order
    For the computation of the functions I ~ ν ( x ) and K ~ ν ( x ) defined by (10.45.2) see Temme (1994c) and Gil et al. (2002d, 2003a, 2004b).