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11: 19.29 Reduction of General Elliptic Integrals
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►and is any permutation of the numbers
, then
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►Moreover, the requirement that one limit of integration be a branch point of the integrand is eliminated without doubling the number of standard integrals in the result.
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►The integrals in (19.29.4), (19.29.7), and (19.29.8) are , , and , respectively.
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►where is any permutation of the numbers
, and
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12: 26.11 Integer Partitions: Compositions
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denotes the number of compositions of , and is the number of compositions into exactly
parts.
is the number of compositions of with no 1’s, where again .
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26.11.2
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►The Fibonacci numbers are determined recursively by
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►Additional information on Fibonacci numbers can be found in Rosen et al. (2000, pp. 140–145).
13: 31.7 Relations to Other Functions
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31.7.1
►Other reductions of to a , with at least one free parameter, exist iff the pair takes one of a finite number of values, where .
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31.7.2
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31.7.3
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14: 36.7 Zeros
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36.7.6
►The rings are almost circular (radii close to and varying by less than 1%), and almost flat (deviating from the planes by at most ).
…, ), the number of rings in the th row, measured from the origin and before the transition to hairpins, is given by
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15: Mathematical Introduction
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►The NIST Handbook has essentially the same objective as the Handbook of Mathematical Functions that was issued in 1964 by the National Bureau of Standards as Number 55 in the NBS Applied Mathematics Series (AMS).
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►These include, for example, multivalued functions of complex variables, for which new definitions of branch points and principal values are supplied (§§1.10(vi), 4.2(i)); the Dirac delta (or delta function), which is introduced in a more readily comprehensible way for mathematicians (§1.17); numerically satisfactory solutions of differential and difference equations (§§2.7(iv), 2.9(i)); and numerical analysis for complex variables (Chapter 3).
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►For equations or other technical information that appeared previously in AMS 55, the DLMF usually includes the corresponding AMS 55 equation number, or other form of reference, together with corrections, if needed.
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complex plane (excluding infinity). | |
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or | Kronecker delta: 0 if ; 1 if . |
(or ) | forward difference operator: . |
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16: 34.2 Definition: Symbol
17: 31.3 Basic Solutions
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denotes the solution of (31.2.1) that corresponds to the exponent at and assumes the value there.
If the other exponent is not a positive integer, that is, if , then from §2.7(i) it follows that exists, is analytic in the disk , and has the Maclaurin expansion
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►Solutions of (31.2.1) corresponding to the exponents and at are respectively,
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31.3.7
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►For example, is equal to
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18: 2.11 Remainder Terms; Stokes Phenomenon
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►uniformly when () and is bounded.
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►One is uniformly valid for with bounded , and achieves uniform exponential improvement throughout :
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►For the sector the conjugate result applies.
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►We now compute the forward differences , , of the moduli of the rounded values of the first 6 neglected terms:
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►Similar improvements are achievable by Aitken’s -process, Wynn’s -algorithm, and other acceleration transformations.
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19: 18.26 Wilson Class: Continued
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18.26.4_1
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18.26.4_2
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►For comments on the use of the forward-difference operator , the backward-difference operator , and the central-difference operator , see §18.2(ii).
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18.26.16
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18.26.17
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