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11: Bibliography
  • G. E. Andrews (1966a) On basic hypergeometric series, mock theta functions, and partitions. II. Quart. J. Math. Oxford Ser. (2) 17, pp. 132–143.
  • G. E. Andrews (1972) Summations and transformations for basic Appell series. J. London Math. Soc. (2) 4, pp. 618–622.
  • G. E. Andrews (1974) Applications of basic hypergeometric functions. SIAM Rev. 16 (4), pp. 441–484.
  • R. Askey and J. Wilson (1985) Some basic hypergeometric orthogonal polynomials that generalize Jacobi polynomials. Mem. Amer. Math. Soc. 54 (319), pp. iv+55.
  • R. Askey (1980) Some basic hypergeometric extensions of integrals of Selberg and Andrews. SIAM J. Math. Anal. 11 (6), pp. 938–951.
  • 12: Bibliography G
  • F. Gao and V. J. W. Guo (2013) Contiguous relations and summation and transformation formulae for basic hypergeometric series. J. Difference Equ. Appl. 19 (12), pp. 2029–2042.
  • L. Gårding (1947) The solution of Cauchy’s problem for two totally hyperbolic linear differential equations by means of Riesz integrals. Ann. of Math. (2) 48 (4), pp. 785–826.
  • G. Gasper and M. Rahman (1990) Basic Hypergeometric Series. Encyclopedia of Mathematics and its Applications, Vol. 35, Cambridge University Press, Cambridge.
  • G. Gasper and M. Rahman (2004) Basic Hypergeometric Series. Second edition, Encyclopedia of Mathematics and its Applications, Vol. 96, Cambridge University Press, Cambridge.
  • R. A. Gustafson (1987) Multilateral summation theorems for ordinary and basic hypergeometric series in U ( n ) . SIAM J. Math. Anal. 18 (6), pp. 1576–1596.
  • 13: 29.3 Definitions and Basic Properties
    §29.3 Definitions and Basic Properties
    For each pair of values of ν and k there are four infinite unbounded sets of real eigenvalues h for which equation (29.2.1) has even or odd solutions with periods 2 K or 4 K . … If ν is a nonnegative integer and 2 p ν , then the continued fraction on the right-hand side of (29.3.10) terminates, and (29.3.10) has only the solutions (29.3.9) with 2 m ν . If ν is a nonnegative integer and 2 p > ν , then (29.3.10) has only the solutions (29.3.9) with 2 m > ν . …
    14: 28.20 Definitions and Basic Properties
    §28.20 Definitions and Basic Properties
    §28.20(ii) Solutions Ce ν , Se ν , Me ν , Fe n , Ge n
    §28.20(iii) Solutions M ν ( j )
    It follows that (28.20.1) has independent and unique solutions M ν ( 3 ) ( z , h ) , M ν ( 4 ) ( z , h ) such that …
    §28.20(v) Solutions Ie n , Io n , Ke n , Ko n
    15: 27.13 Functions
    The basic problem is that of expressing a given positive integer n as a sum of integers from some prescribed set S whose members are primes, squares, cubes, or other special integers. … Every even integer n > 4 is the sum of two odd primes. In this case, S ( n ) is the number of solutions of the equation n = p + q , where p and q are odd primes. … has nonnegative integer solutions for all n 1 . …Similarly, G ( k ) denotes the smallest m for which (27.13.1) has nonnegative integer solutions for all sufficiently large n . … For a given integer k 2 the function r k ( n ) is defined as the number of solutions of the equation …
    16: Bibliography K
  • K. Kajiwara and Y. Ohta (1996) Determinant structure of the rational solutions for the Painlevé II equation. J. Math. Phys. 37 (9), pp. 4693–4704.
  • K. Kajiwara and Y. Ohta (1998) Determinant structure of the rational solutions for the Painlevé IV equation. J. Phys. A 31 (10), pp. 2431–2446.
  • V. Kourganoff (1952) Basic Methods in Transfer Problems. Radiative Equilibrium and Neutron Diffusion. Oxford University Press, Oxford.
  • C. Krattenthaler (1993) HYP and HYPQ. Mathematica packages for the manipulation of binomial sums and hypergeometric series respectively q -binomial sums and basic hypergeometric series. Séminaire Lotharingien de Combinatoire 30, pp. 61–76.
  • Y. A. Kravtsov (1964) Asymptotic solution of Maxwell’s equations near caustics. Izv. Vuz. Radiofiz. 7, pp. 1049–1056.
  • 17: 28.12 Definitions and Basic Properties
    §28.12 Definitions and Basic Properties
    In consequence, for the Floquet solutions w ( z ) the factor e π i ν in (28.2.14) is no longer ± 1 . … The Floquet solution with respect to ν is denoted by me ν ( z , q ) . …The other eigenfunction is me ν ( z , q ) , a Floquet solution with respect to ν with a = λ ν ( q ) . …They have the following pseudoperiodic and orthogonality properties: …
    18: Bibliography M
  • R. S. Maier (2007) The 192 solutions of the Heun equation. Math. Comp. 76 (258), pp. 811–843.
  • M. Mazzocco (2001a) Rational solutions of the Painlevé VI equation. J. Phys. A 34 (11), pp. 2281–2294.
  • M. Mazzocco (2001b) Picard and Chazy solutions to the Painlevé VI equation. Math. Ann. 321 (1), pp. 157–195.
  • S. C. Milne (1985c) A new symmetry related to 𝑆𝑈 ( n ) for classical basic hypergeometric series. Adv. in Math. 57 (1), pp. 71–90.
  • S. C. Milne (1997) Balanced Θ 2 3 summation theorems for U ( n ) basic hypergeometric series. Adv. Math. 131 (1), pp. 93–187.
  • 19: 10.47 Definitions and Basic Properties
    §10.47 Definitions and Basic Properties
    §10.47(ii) Standard Solutions
    §10.47(iii) Numerically Satisfactory Pairs of Solutions
    For (10.47.1) numerically satisfactory pairs of solutions are given by Table 10.2.1 with the symbols J , Y , H , and ν replaced by 𝗃 , 𝗒 , 𝗁 , and n , respectively. For (10.47.2) numerically satisfactory pairs of solutions are 𝗂 n ( 1 ) ( z ) and 𝗄 n ( z ) in the right half of the z -plane, and 𝗂 n ( 1 ) ( z ) and 𝗄 n ( z ) in the left half of the z -plane. …
    20: 13.2 Definitions and Basic Properties
    §13.2 Definitions and Basic Properties
    Standard Solutions
    The first two standard solutions are: …
    §13.2(v) Numerically Satisfactory Solutions