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representations as sums of powers

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21: 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.
  • 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.
  • RISC Combinatorics Group (website) Research Institute for Symbolic Computation, Hagenberg im Mühlkreis, Austria.
  • 22: 32.8 Rational Solutions
    where the Q n ( z ) are monic polynomials (coefficient of highest power of z is 1 ) satisfying …
    32.8.8 m = 0 p m ( z ) λ m = exp ( z λ 4 3 λ 3 ) .
    For determinantal representations see Kajiwara and Masuda (1999). … For determinantal representations see Kajiwara and Ohta (1998) and Noumi and Yamada (1999). … For determinantal representations see Masuda et al. (2002). …
    23: Errata
    For some classical polynomials we give some positive sums and discriminants. …
  • Section 16.11(i)

    A sentence indicating that explicit representations for the coefficients c k are given in Volkmer (2023) was inserted just below (16.11.5).

  • Additions

    Equations: (3.3.3_1), (3.3.3_2), (5.15.9) (suggested by Calvin Khor on 2021-09-04), (8.15.2), Pochhammer symbol representation in (10.17.1) for a k ( ν ) coefficient, Pochhammer symbol representation in (11.9.4) for a k ( μ , ν ) coefficient, and (12.14.4_5).

  • Equation (11.11.1)

    Pochhammer symbol representations for the functions F k ( ν ) and G k ( ν ) were inserted.

  • Subsections 2.3(ii), 2.3(iv), 2.3(vi)

    Clarifications regarding t -powers and asymptotics were added, along with extra citations.

  • 24: 11.10 Anger–Weber Functions
    §11.10(i) Definitions
    §11.10(iii) Maclaurin Series
    §11.10(x) Integrals and Sums
    For collections of integral representations and integrals see Erdélyi et al. (1954a, §§4.19 and 5.17), Marichev (1983, pp. 194–195 and 214–215), Oberhettinger (1972, p. 128), Oberhettinger (1974, §§1.12 and 2.7), Oberhettinger (1990, pp. 105 and 189–190), Prudnikov et al. (1990, §§1.5 and 2.8), Prudnikov et al. (1992a, §3.18), Prudnikov et al. (1992b, §3.18), and Zanovello (1977). For sums see Hansen (1975, pp. 456–457) and Prudnikov et al. (1990, §§6.4.2–6.4.3).
    25: 16.8 Differential Equations
    16.8.4 z q 𝐷 q + 1 w + j = 1 q z j 1 ( α j z + β j ) 𝐷 j w + α 0 w = 0 , p q ,
    16.8.5 z q ( 1 z ) 𝐷 q + 1 w + j = 1 q z j 1 ( α j z + β j ) 𝐷 j w + α 0 w = 0 , p = q + 1 ,
    For other values of the b j , series solutions in powers of z (possibly involving also ln z ) can be constructed via a limiting process; compare §2.7(i) in the case of second-order differential equations. …
    16.8.9 ( k = 1 q + 1 Γ ( a k ) / k = 1 q Γ ( b k ) ) F q q + 1 ( a 1 , , a q + 1 b 1 , , b q ; z ) = j = 1 q + 1 ( z 0 z ) a j n = 0 Γ ( a j + n ) n ! ( k = 1 k j q + 1 Γ ( a k a j n ) / k = 1 q Γ ( b k a j n ) ) F q q + 1 ( a 1 a j n , , a q + 1 a j n b 1 a j n , , b q a j n ; z 0 ) ( z z 0 ) n .
    In this reference it is also explained that in general when q > 1 no simple representations in terms of generalized hypergeometric functions are available for the fundamental solutions near z = 1 . …
    26: 30.11 Radial Spheroidal Wave Functions
    30.11.3 S n m ( j ) ( z , γ ) = ( 1 z 2 ) 1 2 m A n m ( γ 2 ) 2 k m n a n , k m ( γ 2 ) ψ n + 2 k ( j ) ( γ z ) .
    30.11.4 A n ± m ( γ 2 ) = 2 k m n ( 1 ) k a n , k ± m ( γ 2 ) ( 0 ) .
    For asymptotic expansions in negative powers of z see Meixner and Schäfke (1954, p. 293). …
    §30.11(vi) Integral Representations