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21—30 of 706 matching pages
21: 3.6 Linear Difference Equations
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►In practice, however, problems of severe instability often arise and in §§3.6(ii)–3.6(vii) we show how these difficulties may be overcome.
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►with , , can be computed recursively for .
Unless exact arithmetic is being used, however, each step of the calculation introduces rounding errors.
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►In the notation of §3.6(v) we have and .
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►For further information see Wimp (1984, Chapters 7–8), Cash and Zahar (1994), and Lozier (1980).
22: 5.11 Asymptotic Expansions
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►The expansion (5.11.1) is called Stirling’s series (Whittaker and Watson (1927, §12.33)), whereas the expansion (5.11.3), or sometimes just its leading term, is known as Stirling’s formula (Abramowitz and Stegun (1964, §6.1), Olver (1997b, p. 88)).
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23: 24.2 Definitions and Generating Functions
24: 23.21 Physical Applications
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►For applications to soliton solutions of the Korteweg–de Vries (KdV) equation see McKean and Moll (1999, p. 91), Deconinck and Segur (2000), and Walker (1996, §8.1).
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►Ellipsoidal coordinates may be defined as the three roots of the equation
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25: Bibliography N
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Generalization of Binet’s Gamma function formulas.
Integral Transforms Spec. Funct. 24 (8), pp. 597–606.
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On the large argument asymptotics of the Lommel function via Stieltjes transforms.
Asymptot. Anal. 91 (3-4), pp. 265–281.
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Elliptic integrals of the second and third kinds.
Zastos. Mat. 11, pp. 99–102.
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On the calculation of elliptic integrals of the second and third kinds.
Zastos. Mat. 11, pp. 91–94.
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The asymptotic behavior of the general real solution of the third Painlevé equation.
Dokl. Akad. Nauk SSSR 283 (5), pp. 1161–1165 (Russian).
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26: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
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►General references for this subsection include Friedman (1990, pp. 4–6), Shilov (2013, pp. 249–256), Riesz and Sz.-Nagy (1990, Ch. 5, §82).
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►The implicit boundary conditions taken here are that the and vanish as , which in this case is equivalent to requiring , see Pauling and Wilson (1985, pp. 67–82) for a discussion of this latter point.
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►More generally, for , , see (1.4.24),
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►See Titchmarsh (1962a, pp. 87–90) for a first principles derivation for the case .
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►More generally, continuous spectra may occur in sets of disjoint finite intervals , often called bands, when is periodic, see Ashcroft and Mermin (1976, Ch 8) and Kittel (1996, Ch 7).
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27: Bibliography V
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Integrating products of Bessel functions with an additional exponential or rational factor.
Comput. Phys. Comm. 178 (8), pp. 578–590.
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Expansion of vacuum magnetic fields in toroidal harmonics.
Comput. Phys. Comm. 81 (1-2), pp. 74–90.
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Dritter Beweis der die unvollständige Gammafunktion betreffenden Lochsschen Ungleichungen.
Österreich. Akad. Wiss. Math.-Natur. Kl. Sitzungsber. II 192 (1-3), pp. 83–91 (German).
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On the rational solutions of the second Painlevé equation.
Differ. Uravn. 1 (1), pp. 79–81 (Russian).
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28: 27.2 Functions
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►Functions in this section derive their properties from the fundamental
theorem of arithmetic, which states that every integer can be represented uniquely as a product of prime powers,
…( is defined to be 0.)
…It can be expressed as a sum over all primes :
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►is the sum of the th powers of the divisors of , where the exponent can be real or complex.
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29: 3.9 Acceleration of Convergence
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►It should be borne in mind that a sequence (series) transformation can be effective for one type of sequence (series) but may not accelerate convergence for another type.
It may even fail altogether by not being limit-preserving.
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►Let
be a fixed positive integer.
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►The ratio of the Hankel determinants in (3.9.9) can be computed recursively by Wynn’s epsilon algorithm:
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►For further information on the epsilon algorithm see Brezinski and Redivo Zaglia (1991, pp. 78–95).
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30: 20.5 Infinite Products and Related Results
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