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11: 28.31 Equations of Whittaker–Hill and Ince
For proofs and further information, including convergence of the series (28.31.4), (28.31.5), see Arscott (1967). …
ℎ𝑠 2 n + 2 2 m + 2 ( z , ξ ) = ( 1 ) m ℎ𝑠 2 n + 2 2 m + 2 ( 1 2 π z , ξ ) .
More important are the double orthogonality relations for p 1 p 2 or m 1 m 2 or both, given by …
12: 16.5 Integral Representations and Integrals
where the contour of integration separates the poles of Γ ( a k + s ) , k = 1 , , p , from those of Γ ( s ) . … Then the integral converges when p < q + 1 provided that z 0 , or when p = q + 1 provided that 0 < | z | < 1 , and provides an integral representation of the left-hand side with these conditions. … Then the integral converges when q < p + 1 and | ph ( z ) | < ( p + 1 q ) π / 2 . …
13: 13.2 Definitions and Basic Properties
§13.2 Definitions and Basic Properties
The series (13.2.2) and (13.2.3) converge for all z . … … Another standard solution of (13.2.1) is U ( a , b , z ) , which is determined uniquely by the property
14: 20.11 Generalizations and Analogs
For applications to rapidly convergent expansions for π see Chudnovsky and Chudnovsky (1988), and for applications in the construction of elliptic-hypergeometric series see Rosengren (2004). … Multidimensional theta functions with characteristics are defined in §21.2(ii) and their properties are described in §§21.3(ii), 21.5(ii), and 21.6. …
15: 18.38 Mathematical Applications
The monic Chebyshev polynomial 2 1 n T n ( x ) , n 1 , enjoys the ‘minimax’ property on the interval [ 1 , 1 ] , that is, | 2 1 n T n ( x ) | has the least maximum value among all monic polynomials of degree n . In consequence, expansions of functions that are infinitely differentiable on [ 1 , 1 ] in series of Chebyshev polynomials usually converge extremely rapidly. …
16: 33.14 Definitions and Basic Properties
§33.14 Definitions and Basic Properties
§33.14(i) Coulomb Wave Equation
This includes ϵ = 0 , hence f ( ϵ , ; r ) can be expanded in a convergent power series in ϵ in a neighborhood of ϵ = 0 33.20(ii)).
§33.14(iii) Irregular Solution h ( ϵ , ; r )
The function s ( ϵ , ; r ) has the following properties: …
17: 8.17 Incomplete Beta Functions
§8.17(i) Definitions and Basic Properties
The 4 m and 4 m + 1 convergents are less than I x ( a , b ) , and the 4 m + 2 and 4 m + 3 convergents are greater than I x ( a , b ) . … The expansion (8.17.22) converges rapidly for x < ( a + 1 ) / ( a + b + 2 ) . For x > ( a + 1 ) / ( a + b + 2 ) or 1 x < ( b + 1 ) / ( a + b + 2 ) , more rapid convergence is obtained by computing I 1 x ( b , a ) and using (8.17.4). …
§8.17(vii) Addendum to 8.17(i) Definitions and Basic Properties
18: 10.74 Methods of Computation
In other circumstances the power series are prone to slow convergence and heavy numerical cancellation. … Moreover, because of their double asymptotic properties10.41(v)) these expansions can also be used for large x or | z | , whether or not ν is large. … Newton’s rule is quadratically convergent and Halley’s rule is cubically convergent. …
19: 3.11 Approximation Techniques
The iterative process converges locally and quadratically (§3.8(i)). … They enjoy an orthogonal property with respect to integrals: … converges uniformly. … The property
20: 3.6 Linear Difference Equations
The normalizing factor Λ can be the true value of w 0 divided by its trial value, or Λ can be chosen to satisfy a known property of the wanted solution of the form … For further information on Miller’s algorithm, including examples, convergence proofs, and error analyses, see Wimp (1984, Chapter 4), Gautschi (1967, 1997b), and Olver (1964a). … For further information, including a more general form of normalizing condition, other examples, convergence proofs, and error analyses, see Olver (1967a), Olver and Sookne (1972), and Wimp (1984, Chapter 6). …