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Weierstrass%0Aelliptic functions

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31: 22.15 Inverse Functions
§22.15 Inverse Functions
§22.15(i) Definitions
Each of these inverse functions is multivalued. The principal values satisfy …
32: 30.11 Radial Spheroidal Wave Functions
§30.11 Radial Spheroidal Wave Functions
§30.11(i) Definitions
In (30.11.3) z 0 when j = 1 , and | z | > 1 when j = 2 , 3 , 4 .
Connection Formulas
§30.11(ii) Graphics
33: 28.12 Definitions and Basic Properties
The introduction to the eigenvalues and the functions of general order proceeds as in §§28.2(i), 28.2(ii), and 28.2(iii), except that we now restrict ν ^ 0 , 1 ; equivalently ν n . … As a function of ν with fixed q ( 0 ), λ ν ( q ) is discontinuous at ν = ± 1 , ± 2 , . …
§28.12(ii) Eigenfunctions me ν ( z , q )
For q = 0 , … However, these functions are not the limiting values of me ± ν ( z , q ) as ν n ( 0 ) . …
34: 1.16 Distributions
The closure of the set of points where ϕ 0 is called the support of ϕ . … A sequence { ϕ n } of test functions converges to a test function ϕ if the support of every ϕ n is contained in a fixed compact set K and as n the sequence { ϕ n ( k ) } converges uniformly on K to ϕ ( k ) for k = 0 , 1 , 2 , . … Λ : 𝒟 ( I ) is called a distribution, or generalized function, if it is a continuous linear functional on 𝒟 ( I ) , that is, it is a linear functional and for every ϕ n ϕ in 𝒟 ( I ) , … Suppose f ( x ) is infinitely differentiable except at x 0 , where left and right derivatives of all orders exist, and … For α > 0 , …
35: 35.5 Bessel Functions of Matrix Argument
§35.5 Bessel Functions of Matrix Argument
§35.5(i) Definitions
§35.5(ii) Properties
§35.5(iii) Asymptotic Approximations
For asymptotic approximations for Bessel functions of matrix argument, see Herz (1955) and Butler and Wood (2003).
36: 16.17 Definition
§16.17 Definition
Assume also that m and n are integers such that 0 m q and 0 n p , and none of a k b j is a positive integer when 1 k n and 1 j m . Then the Meijer G -function is defined via the Mellin–Barnes integral representation: …
  • (ii)

    L is a loop that starts at infinity on a line parallel to the positive real axis, encircles the poles of the Γ ( b s ) once in the negative sense and returns to infinity on another line parallel to the positive real axis. The integral converges for all z ( 0 ) if p < q , and for 0 < | z | < 1 if p = q 1 .

  • Then …
    37: 22.2 Definitions
    §22.2 Definitions
    For k [ 0 , 1 ] , all functions are real for z . … The Jacobian functions are related in the following way. … In terms of Neville’s theta functions20.1) …
    38: 21.2 Definitions
    §21.2(i) Riemann Theta Functions
    §21.2(ii) Riemann Theta Functions with Characteristics
    This function is referred to as a Riemann theta function with characteristics [ 𝜶 𝜷 ] . …Characteristics whose elements are either 0 or 1 2 are called half-period characteristics. …
    §21.2(iii) Relation to Classical Theta Functions
    39: 35.7 Gaussian Hypergeometric Function of Matrix Argument
    §35.7 Gaussian Hypergeometric Function of Matrix Argument
    §35.7(i) Definition
    Jacobi Form
    Let f : 𝛀 (a) be orthogonally invariant, so that f ( 𝐓 ) is a symmetric function of t 1 , , t m , the eigenvalues of the matrix argument 𝐓 𝛀 ; (b) be analytic in t 1 , , t m in a neighborhood of 𝐓 = 𝟎 ; (c) satisfy f ( 𝟎 ) = 1 . … Systems of partial differential equations for the F 1 0 (defined in §35.8) and F 1 1 functions of matrix argument can be obtained by applying (35.8.9) and (35.8.10) to (35.7.9). …
    40: 35.8 Generalized Hypergeometric Functions of Matrix Argument
    §35.8 Generalized Hypergeometric Functions of Matrix Argument
    §35.8(i) Definition
    §35.8(ii) Relations to Other Functions
    Value at 𝐓 = 𝟎
    A similar result for the F 1 0 function of matrix argument is given in Faraut and Korányi (1994, p. 346). …