relation to logarithmic integral
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31: 2.1 Definitions and Elementary Properties
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►Integration of asymptotic and order relations is permissible, subject to obvious convergence conditions.
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►Condition (2.1.13) is equivalent to
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►means that for each , the difference between and the th partial sum on the right-hand side is as in .
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►Substitution, logarithms, and powers are also permissible; compare Olver (1997b, pp. 19–22).
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►The asymptotic property may also hold uniformly with respect to parameters.
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32: 7.2 Definitions
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§7.2(ii) Dawson’s Integral
… ►§7.2(iii) Fresnel Integrals
… ►Values at Infinity
… ►§7.2(iv) Auxiliary Functions
… ►§7.2(v) Goodwin–Staton Integral
…33: Errata
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Additions
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Equation (19.20.11)
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Equations (10.22.37), (10.22.38), (14.17.6)–(14.17.9)
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Chapter 25 Zeta and Related Functions
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Chapter 27
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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 , (15.4.34), (19.5.4_1), (19.5.4_2) and (19.5.4_3).
19.20.11
as , () real, we have added the constant term and the order term , and hence was replaced by .
The Kronecker delta symbols have been moved furthest to the right, as is common convention for orthogonality relations.
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.
For consistency of notation across all chapters, the notation for logarithm has been changed to from throughout Chapter 27.
34: 18.27 -Hahn Class
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►Thus in addition to a relation of the form (18.27.2), such systems may also satisfy orthogonality relations with respect to a continuous weight function on some interval.
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From Big -Jacobi to Jacobi
… ►From Big -Jacobi to Little -Jacobi
… ►From Little -Jacobi to Jacobi
… ►From Little -Laguerre to Laguerre
…35: Bibliography M
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Chebyshev expansions for modified Struve and related functions.
Math. Comp. 60 (202), pp. 735–747.
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Connection between quantum systems involving the fourth Painlevé transcendent and -step rational extensions of the harmonic oscillator related to Hermite exceptional orthogonal polynomial.
J. Math. Phys. 57 (5), pp. Paper 052101, 15 pp..
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Recursion relations for the - symbols.
Nuclear Physics A 113 (1), pp. 215–220.
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Evaluation of complex logarithms and related functions.
SIAM J. Numer. Anal. 18 (4), pp. 744–750.
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A new symmetry related to
for classical basic hypergeometric series.
Adv. in Math. 57 (1), pp. 71–90.
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36: 18.34 Bessel Polynomials
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§18.34(i) Definitions and Recurrence Relation
… ►With the notation of Koekoek et al. (2010, (9.13.1)) the left-hand side of (18.34.1) has to be replaced by . …where is a modified spherical Bessel function (10.49.9), and … … ►where primes denote derivatives with respect to . …37: 6.5 Further Interrelations
38: 5.17 Barnes’ -Function (Double Gamma Function)
§5.17 Barnes’ -Function (Double Gamma Function)
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5.17.4
►In this equation (and in (5.17.5) below), the ’s have their principal values on the positive real axis and are continued via continuity, as in §4.2(i).
►When in ,
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5.17.7
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39: 2.6 Distributional Methods
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►This leads to integrals of the form
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►To assign a distribution to the function , we first let denote the th repeated integral (§1.4(v)) of :
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►An application has been given by López (2000) to derive asymptotic expansions of standard symmetric elliptic integrals, complete with error bounds; see §19.27(vi).
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►The replacement of by its asymptotic expansion (2.6.9), followed by term-by-term integration leads to convolution integrals of the form
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►The method of distributions can be further extended to derive asymptotic expansions for convolution integrals:
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