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1: Bibliography T
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Coulomb functions with complex angular momenta.
Comput. Phys. Comm. 17 (4), pp. 351–355.
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Une nouvelle représentation explicite des nombres d’Euler.
C. R. Acad. Sci. Paris Sér. A-B 286 (19), pp. A807–A809.
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Rational Chebyshev approximation for the Fermi-Dirac integral
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Solid–State Electronics 41 (5), pp. 771–773.
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Further comments on the computation of modified Bessel function ratios.
Math. Comp. 35 (151), pp. 937–939.
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Sul comportamento asintotico dell’-esimo polinomio di Laguerre nell’intorno dell’ascissa
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Comment. Math. Helv. 22, pp. 150–167.
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2: 6 Exponential, Logarithmic, Sine, and
Cosine Integrals
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3: 7 Error Functions, Dawson’s and Fresnel Integrals
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4: Bibliography K
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An adaptive contour code for the numerical evaluation of the oscillatory cuspoid canonical integrals and their derivatives.
Computer Physics Comm. 132 (1-2), pp. 142–165.
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Comment on “The incomplete beta function law for parallel tempering sampling of classical canonical systems” [J. Chem. Phys. 120, 4119 (2004)].
J. Chem. Phys. 121 (2), pp. 1167.
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A Program for Computing the Conical Functions of the First Kind for and
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Comput. Phys. Comm. 23 (1), pp. 51–61.
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Sur le problème de la rotation d’un corps solide autour d’un point fixe.
Acta Math. 12 (1), pp. 177–232 (French).
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ZEBEC: A mathematical software package for computing simple zeros of Bessel functions of real order and complex argument.
Comput. Phys. Comm. 113 (2-3), pp. 220–238.
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5: Bibliography S
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Répartition du courant alternatif dans un conducteur cylindrique de section elliptique.
Acad. Roy. Belg. Bull. Cl. Sci. (5) 53 (8), pp. 861–878.
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About von Staudt congruences for Bernoulli numbers.
Comment. Math. Univ. St. Paul. 48 (2), pp. 137–144.
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Some comments on Fourier analysis, uncertainty and modeling.
SIAM Rev. 25 (3), pp. 379–393.
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Effective calculation of the incomplete gamma function for parameter values ,
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Angew. Informatik 17, pp. 30–32.
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On the relative extrema of ultraspherical polynomials.
Boll. Un. Mat. Ital. (3) 5, pp. 125–127.
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6: 7.24 Approximations
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Cody et al. (1970) gives minimax rational approximations to Dawson’s integral (maximum relative precision 20S–22S).
Luke (1969b, pp. 323–324) covers and for (the Chebyshev coefficients are given to 20D); and for (the Chebyshev coefficients are given to 20D and 15D, respectively). Coefficients for the Fresnel integrals are given on pp. 328–330 (20D).
Luke (1969b, vol. 2, pp. 422–435) gives main diagonal Padé approximations for , , , , and ; approximate errors are given for a selection of -values.
7: 14.32 Methods of Computation
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►Essentially the same comments that are made in §15.19 concerning the computation of hypergeometric functions apply to the functions described in the present chapter.
In particular, for small or moderate values of the parameters and the power-series expansions of the various hypergeometric function representations given in §§14.3(i)–14.3(iii), 14.19(ii), and 14.20(i) can be selected in such a way that convergence is stable, and reasonably rapid, especially when the argument of the functions is real.
In other cases recurrence relations (§14.10) provide a powerful method when applied in a stable direction (§3.6); see Olver and Smith (1983) and Gautschi (1967).
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8: 27 Functions of Number Theory
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9: 7.22 Methods of Computation
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►The methods available for computing the main functions in this chapter are analogous to those described in §§6.18(i)–6.18(iv) for the exponential integral and sine and cosine integrals, and similar comments apply.
Additional references are Matta and Reichel (1971) for the application of the trapezoidal rule, for example, to the first of (7.7.2), and Gautschi (1970) and Cuyt et al. (2008) for continued fractions.
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►For a comprehensive survey of computational methods for the functions treated in this chapter, see van der Laan and Temme (1984, Ch. V).