Rational approximations of generalized hypergeometric functions pFq\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}_pF_q$$\end{document} of type (n+k,k)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(n+k,k)$$\end{document} are constructed by the Drummond and factorial Levin-type sequence transformations. We derive recurrence relations for these rational approximations that require O[max{p,q}(n+k)]\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathcal {O}[\max \{p,q\}(n+k)]$$\end{document} flops. These recurrence relations come in two forms: for the successive numerators and denominators;and, for an auxiliary rational sequence and the rational approximations themselves. Numerical evidence suggests that these recurrence relations are much more stable than the original formul AE for the Drummond and factorial Levin-type sequence transformations. Theoretical results on the placement of the poles of both transformations confirm the superiority of factorial Levin-type transformation over the Drummond transformation.
For a certain linear operator which is defined by means of the Hadamard product (or convolution) with a generalizedhypergeometric function, the authors aim at investigating various mapping and inclusion properties in...
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For a certain linear operator which is defined by means of the Hadamard product (or convolution) with a generalizedhypergeometric function, the authors aim at investigating various mapping and inclusion properties involving such subclasses, of analytic and univalent functions as (for example) k-uniformly convex functions and k-starlike functions. Relevant connections of the definitions and results presented in this paper with those in several earlier works on the subject are also pointed out. (C) 2002 Elsevier Science Ltd. All rights reserved.
作者:
Rathie, P.N.Institute of Mathematics
Statistics and Computer Science State University of Campinas Campinas S.P. 13081 Ca.ixa Postal 6065 Brazil
In this review article, an attempt has been made to give an up-to-date survey of the work done on the applications of generalized hypergeometric functions (especially G, H and R functions) to the exact distributions o...
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We present a further extension of the HYPERDIRE project, which is devoted to the creation of a set of Mathematica-based program packages for manipulations with Horn-type hypergeometricfunctions on the basis of differ...
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We present a further extension of the HYPERDIRE project, which is devoted to the creation of a set of Mathematica-based program packages for manipulations with Horn-type hypergeometricfunctions on the basis of differential equations. Specifically, we present the implementation of the differential reduction for the Lauricella function F-C of three variables. Program summary Program title: HYPERDIRE Catalogue identifier: AEPP_v4_0 Program summary URL: http://***/summaries/AEPP_v4_*** Program obtainable from: CPC Program Library, Queen's University, Belfast, N. Ireland Licensing provisions: GNU General Public License, version 3 No. of lines in distributed program, including test data, etc.: 243461 No. of bytes in distributed program, including test data, etc.: 61610782 Distribution format: *** Programming language: Mathematica. Computer: All computers running Mathematica. Classification: 4.4. Does the new version supersede the previous version?: No, it significantly extends the previous version. Nature of problem: Reduction of hypergeometric function F-C of three variables to a set of basis functions. Solution method: Differential reduction. Reasons for new version: The extension package allows the user to handle the Lauricella function F-C of three variables. Summary of revisions: The previous version goes unchanged. Running time: Depends on the complexity of the problem. (C) 2016 Elsevier B.V. All rights reserved.
The Cholesky factorization of the moment matrix is applied to discrete orthogonal polynomials on the homogeneous lattice. In particular, semiclassical discrete orthogonal polynomials, which are built in terms of a dis...
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The Cholesky factorization of the moment matrix is applied to discrete orthogonal polynomials on the homogeneous lattice. In particular, semiclassical discrete orthogonal polynomials, which are built in terms of a discrete Pearson equation, are studied. The Laguerre-Freud structure semiinfinite matrix that models the shifts by +/- 1 in the independent variable of the set of orthogonal polynomials is introduced. In the semiclassical case it is proven that this Laguerre-Freud matrix is banded. From the well-known fact that moments of the semiclassical weights are logarithmic derivatives of generalized hypergeometric functions, it is shown how the contiguous relations for these hypergeometricfunctions translate as symmetries for the corresponding moment matrix. It is found that the 3D Nijhoff-Capel discrete Toda lattice describes the corresponding contiguous shifts for the squared norms of the orthogonal polynomials. The continuous 1D Toda equation for these semiclassical discrete orthogonal polynomials is discussed and the compatibility equations are derived. It is also shown that the Kadomtesev-Petviashvilii equation is connected to an adequate deformed semiclassical discrete weight, but in this case, the deformation does not satisfy a Pearson equation.
We deduce in an elementary way representations for the Mellin transform of a product of Bessel functions F-0(1)[-a(2)x(2)] and generalized hypergeometric functions F-p(p+1)[-b(2)x(2)] for a,b > 0. As a corollary we...
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We deduce in an elementary way representations for the Mellin transform of a product of Bessel functions F-0(1)[-a(2)x(2)] and generalized hypergeometric functions F-p(p+1)[-b(2)x(2)] for a,b > 0. As a corollary we obtain a transformation formula for F-p+1(p)[1] which was discovered by Wimp in 1987 by using Bailey's method for the specialization F-3(2)[1].
The inductance integrals of air-core circular coils with rectangular cross section and parallel axes are difficult to tackle with analytical method due to the inclusion of Struve functions. Using the inverse Mellin tr...
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The inductance integrals of air-core circular coils with rectangular cross section and parallel axes are difficult to tackle with analytical method due to the inclusion of Struve functions. Using the inverse Mellin transform, these Bessel-Struve integrals will be continued analytically to the complex plane, and then by virtue of contour deformation and residue theorem, they can be expanded to the series containing the generalized hypergeometric functions which are easy to execute in common mathematical software packages. The series solutions are preferable in case the difficulties arise in the evaluations of Bessel-Struve integrals, though they do not cover the whole region of coil geometric parameters. In addition, the obtained series were compared numerically with the corresponding integrals, complete consistency was shown clearly. By means of the proposed method, the computation efficiency can be improved by several orders of magnitude compared to that of the corresponding integral methods.
We express the asymptotics of the remainders of the partial sums {s (n) } of the generalizedhypergeometric function q + 1 Fq ((alpha 1, ... , alpha q+1)(beta 1, ... , beta q) vertical bar z through an inverse power s...
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We express the asymptotics of the remainders of the partial sums {s (n) } of the generalizedhypergeometric function q + 1 Fq ((alpha 1, ... , alpha q+1)(beta 1, ... , beta q) vertical bar z through an inverse power series z(n)n(lambda) Sigma c(k)/n(k), where the exponent lambda and the asymptotic coefficients {c(k)} may be recursively computed to any desired order from the hypergeometric parameters and argument. From this we derive a new series acceleration technique that can be applied to any such function, even with complex parameters and at the branch point z = 1. For moderate parameters (up to approximately ten) a C implementation at fixed precision is very effective at computing these functions;for larger parameters an implementation in higher than machine precision would be needed. Even for larger parameters, however, our C implementation is able to correctly determine whether or not it has converged;and when it converges, its estimate of its error is accurate.
A new class is introduced consisting of harmonic univalent functions on the exterior unit disk defined by convolution. This class generates several known and new subclasses of harmonic univalent functions as special c...
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A new class is introduced consisting of harmonic univalent functions on the exterior unit disk defined by convolution. This class generates several known and new subclasses of harmonic univalent functions as special cases. A necessary and sufficient convolution condition is obtained for functions to belong to the class. A corresponding general class of harmonic functions with negative coefficients is also introduced, and coefficient condition that is both necessary and sufficient is obtained for the class. Extreme points are also determined. As applications, starlikeness conditions of the Liu-Srivastava linear operator involving the generalized hypergeometric functions are discussed.
We herein determine an integral representation of generalized hypergeometric functions mFm extending the usual results on 1F1. After formulating integral operators involving the generalized hypergeometric functions of...
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We herein determine an integral representation of generalized hypergeometric functions mFm extending the usual results on 1F1. After formulating integral operators involving the generalized hypergeometric functions of the form: [image omitted] and [image omitted] we prove that these operators are composition of generalized variants of the Laplace transform (and Watson) and Erdelyi-Kober fractional integral operators. We also prove that these operators are bounded in Lp.
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