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11: Bibliography M
  • R. S. Maier (2005) On reducing the Heun equation to the hypergeometric equation. J. Differential Equations 213 (1), pp. 171–203.
  • H. Majima, K. Matsumoto, and N. Takayama (2000) Quadratic relations for confluent hypergeometric functions. Tohoku Math. J. (2) 52 (4), pp. 489–513.
  • M. Mazzocco (2001b) Picard and Chazy solutions to the Painlevé VI equation. Math. Ann. 321 (1), pp. 157–195.
  • K. S. Miller and B. Ross (1993) An Introduction to the Fractional Calculus and Fractional Differential Equations. A Wiley-Interscience Publication, John Wiley & Sons, Inc., New York.
  • S. C. Milne (1985c) A new symmetry related to SU ( n ) for classical basic hypergeometric series. Adv. in Math. 57 (1), pp. 71–90.
  • 12: Errata
  • Additions

    Section: 15.9(v) Complete Elliptic Integrals. Equations: (11.11.9_5), (11.11.13_5), Intermediate equality in (15.4.27) which relates to F ( a , a ; a + 1 ; 1 2 ) , (15.4.34), (19.5.4_1), (19.5.4_2) and (19.5.4_3).

  • Equation (35.7.3)

    Originally the matrix in the argument of the Gaussian hypergeometric function of matrix argument F 1 2 was written with round brackets. This matrix has been rewritten with square brackets to be consistent with the rest of the DLMF.

  • Equations (10.22.37), (10.22.38), (14.17.6)–(14.17.9)

    The Kronecker delta symbols have been moved furthest to the right, as is common convention for orthogonality relations.

  • Equation (9.7.2)

    Following a suggestion from James McTavish on 2017-04-06, the recurrence relation u k = ( 6 k - 5 ) ( 6 k - 3 ) ( 6 k - 1 ) ( 2 k - 1 ) 216 k u k - 1 was added to Equation (9.7.2).

  • Chapter 25 Zeta and Related Functions

    A number of additions and changes have been made to the metadata to reflect new and changed references as well as to how some equations have been derived.

  • 13: 13.29 Methods of Computation
    §13.29(ii) Differential Equations
    A comprehensive and powerful approach is to integrate the differential equations (13.2.1) and (13.14.1) by direct numerical methods. … The recurrence relations in §§13.3(i) and 13.15(i) can be used to compute the confluent hypergeometric functions in an efficient way. … normalizing relationnormalizing relation
    14: Bibliography B
  • G. Blanch and D. S. Clemm (1962) Tables Relating to the Radial Mathieu Functions. Vol. 1: Functions of the First Kind. U.S. Government Printing Office, Washington, D.C..
  • G. Blanch and D. S. Clemm (1965) Tables Relating to the Radial Mathieu Functions. Vol. 2: Functions of the Second Kind. U.S. Government Printing Office, Washington, D.C..
  • S. Bochner (1952) Bessel functions and modular relations of higher type and hyperbolic differential equations. Comm. Sém. Math. Univ. Lund [Medd. Lunds Univ. Mat. Sem.] 1952 (Tome Supplementaire), pp. 12–20.
  • W. G. C. Boyd and T. M. Dunster (1986) Uniform asymptotic solutions of a class of second-order linear differential equations having a turning point and a regular singularity, with an application to Legendre functions. SIAM J. Math. Anal. 17 (2), pp. 422–450.
  • J. C. Butcher (2003) Numerical Methods for Ordinary Differential Equations. John Wiley & Sons Ltd., Chichester.
  • 15: 33.23 Methods of Computation
    §33.23(i) Methods for the Confluent Hypergeometric Functions
    §33.23(iii) Integration of Defining Differential Equations
    §33.23(iv) Recurrence Relations
    In a similar manner to §33.23(iii) the recurrence relations of §§33.4 or 33.17 can be used for a range of values of the integer , provided that the recurrence is carried out in a stable direction (§3.6). … Noble (2004) obtains double-precision accuracy for W - η , μ ( 2 ρ ) for a wide range of parameters using a combination of recurrence techniques, power-series expansions, and numerical quadrature; compare (33.2.7). …
    16: 33.2 Definitions and Basic Properties
    §33.2(i) Coulomb Wave Equation
    This differential equation has a regular singularity at ρ = 0 with indices + 1 and - , and an irregular singularity of rank 1 at ρ = (§§2.7(i), 2.7(ii)). … The function F ( η , ρ ) is recessive (§2.7(iii)) at ρ = 0 , and is defined by …where M κ , μ ( z ) and M ( a , b , z ) are defined in §§13.14(i) and 13.2(i), and … The functions H ± ( η , ρ ) are defined by …
    17: 17.13 Integrals
    §17.13 Integrals
    17.13.1 - c d ( - q x / c ; q ) ( q x / d ; q ) ( - a x / c ; q ) ( b x / d ; q ) d q x = ( 1 - q ) ( q ; q ) ( a b ; q ) c d ( - c / d ; q ) ( - d / c ; q ) ( a ; q ) ( b ; q ) ( c + d ) ( - b c / d ; q ) ( - a d / c ; q ) ,
    Ramanujan’s Integrals
    17.13.3 0 t α - 1 ( - t q α + β ; q ) ( - t ; q ) d t = Γ ( α ) Γ ( 1 - α ) Γ q ( β ) Γ q ( 1 - α ) Γ q ( α + β ) ,
    Askey (1980) conjectured extensions of the foregoing integrals that are closely related to Macdonald (1982). …
    18: 14.19 Toroidal (or Ring) Functions
    This form of the differential equation arises when Laplace’s equation is transformed into toroidal coordinates ( η , θ , ϕ ) , which are related to Cartesian coordinates ( x , y , z ) by …
    §14.19(ii) Hypergeometric Representations
    With F as in §14.3 and ξ > 0 ,
    14.19.2 P ν - 1 2 μ ( cosh ξ ) = Γ ( 1 2 - μ ) π 1 / 2 ( 1 - e - 2 ξ ) μ e ( ν + ( 1 / 2 ) ) ξ F ( 1 2 - μ , 1 2 + ν - μ ; 1 - 2 μ ; 1 - e - 2 ξ ) , μ 1 2 , 3 2 , 5 2 , .
    19: 28.8 Asymptotic Expansions for Large q
    Barrett (1981) supplies asymptotic approximations for numerically satisfactory pairs of solutions of both Mathieu’s equation (28.2.1) and the modified Mathieu equation (28.20.1). …It is stated that corresponding uniform approximations can be obtained for other solutions, including the eigensolutions, of the differential equations by application of the results, but these approximations are not included. … Dunster (1994a) supplies uniform asymptotic approximations for numerically satisfactory pairs of solutions of Mathieu’s equation (28.2.1). … The approximations are expressed in terms of Whittaker functions W κ , μ ( z ) and M κ , μ ( z ) with μ = 1 4 ; compare §2.8(vi). … For related results see Langer (1934) and Sharples (1967, 1971). …
    20: Bibliography S
  • R. B. Shirts (1993b) Algorithm 721: MTIEU1 and MTIEU2: Two subroutines to compute eigenvalues and solutions to Mathieu’s differential equation for noninteger and integer order. ACM Trans. Math. Software 19 (3), pp. 391–406.
  • S. Yu. Slavyanov and N. A. Veshev (1997) Structure of avoided crossings for eigenvalues related to equations of Heun’s class. J. Phys. A 30 (2), pp. 673–687.
  • F. C. Smith (1939b) Relations among the fundamental solutions of the generalized hypergeometric equation when p = q + 1 . II. Logarithmic cases. Bull. Amer. Math. Soc. 45 (12), pp. 927–935.
  • C. Snow (1952) Hypergeometric and Legendre Functions with Applications to Integral Equations of Potential Theory. National Bureau of Standards Applied Mathematics Series, No. 19, U. S. Government Printing Office, Washington, D.C..
  • B. I. Suleĭmanov (1987) The relation between asymptotic properties of the second Painlevé equation in different directions towards infinity. Differ. Uravn. 23 (5), pp. 834–842 (Russian).