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31: 3.6 Linear Difference Equations
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►Given numerical values of and , the solution of the equation
…These errors have the effect of perturbing the solution by unwanted small multiples of and of an independent solution , say.
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►The unwanted multiples of now decay in comparison with , hence are of little consequence.
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►The latter method is usually superior when the true value of is zero or pathologically small.
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►beginning with .
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32: 19.29 Reduction of General Elliptic Integrals
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►Let
…where
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►Next, for , define , and assume both ’s are positive for .
…where
…If , where both linear factors are positive for , and , then (19.29.25) is modified so that
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33: Bibliography F
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Tables of Values of the Function for Complex Argument.
Edited by V. A. Fok; translated from the Russian by D. G. Fry.
Mathematical Tables Series, Vol. 11, Pergamon Press, Oxford.
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Polynomial relations in the Heisenberg algebra.
J. Math. Phys. 35 (11), pp. 6144–6149.
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On a unified approach to transformations and elementary solutions of Painlevé equations.
J. Math. Phys. 23 (11), pp. 2033–2042.
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Application of the -function theory of Painlevé equations to random matrices: , the JUE, CyUE, cJUE and scaled limits.
Nagoya Math. J. 174, pp. 29–114.
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Algorithm 435: Modified incomplete gamma function.
Comm. ACM 15 (11), pp. 993–995.
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34: 9.18 Tables
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Harvard University (1945) tabulates the real and imaginary parts of , , , for , , , with interval 0.1 in and . Precision is 8D. Here , .
Sherry (1959) tabulates , , , , ; 20S.
National Bureau of Standards (1958) tabulates and for and ; for . Precision is 8D.
Nosova and Tumarkin (1965) tabulates , , , for ; 7D. Also included are the real and imaginary parts of and , where and ; 6-7D.
Gil et al. (2003c) tabulates the only positive zero of , the first 10 negative real zeros of and , and the first 10 complex zeros of , , , and . Precision is 11 or 12S.
35: 26.10 Integer Partitions: Other Restrictions
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denotes the number of partitions of into at most distinct parts.
…The set is denoted by .
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►It is known that for , , with strict inequality for sufficiently large, provided that , or ; see Yee (2004).
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►where is the modified Bessel function (§10.25(ii)), and
…The quantity is real-valued.
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36: 24.12 Zeros
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►For the interval denote the zeros of by , , with
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►Let be the total number of real zeros of .
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►For the interval denote the zeros of by , , with
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►When is odd ,
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, , has no multiple zeros.
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37: Bibliography B
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Evaluation of the incomplete gamma function of imaginary argument by Chebyshev polynomials.
Math. Comp. 15 (73), pp. 7–11.
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Ramanujan’s theories of elliptic functions to alternative bases.
Trans. Amer. Math. Soc. 347 (11), pp. 4163–4244.
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Vortices in Ginzburg-Landau Equations.
In Proceedings of the International Congress of Mathematicians,
Vol. III (Berlin, 1998),
pp. 11–19.
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Theoretical and experimental investigation of the elliptical annual ring antenna.
IEEE Trans. Antennas and Propagation 36 (11), pp. 1526–1530.
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Rainbow over Woolsthorpe Manor.
Notes and Records Roy. Soc. London 36 (1), pp. 3–11 (1 plate).
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38: 5.10 Continued Fractions
39: 34.3 Basic Properties: Symbol
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►When any one of is equal to , or , the symbol has a simple algebraic form.
…For these and other results, and also cases in which any one of is or , see Edmonds (1974, pp. 125–127).
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►Even permutations of columns of a symbol leave it unchanged; odd permutations of columns produce a phase factor , for example,
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►Similar conventions
apply to all subsequent summations in this chapter.
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►For the polynomials see §18.3, and for the function see §14.30.
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40: 28.8 Asymptotic Expansions for Large
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►Also let and (§18.3).
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28.8.11
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►The approximations are expressed in terms of Whittaker functions and with ; compare §2.8(vi).
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►Subsequently the asymptotic solutions involving either elementary or Whittaker functions are identified in terms of the Floquet solutions (§28.12(ii)) and modified Mathieu functions (§28.20(iii)).
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