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21—30 of 983 matching pages
21: 16.4 Argument Unity
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►The function is well-poised if
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►See Raynal (1979) for a statement in terms of symbols (Chapter 34).
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►Transformations for both balanced and very well-poised are included in Bailey (1964, pp. 56–63).
A similar theory is available for very well-poised ’s which are 2-balanced.
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22: 15.8 Transformations of Variable
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►All functions in this subsection and §15.8(ii) assume their principal values.
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►When is an integer limits are taken in (15.8.2) and (15.8.3) as follows.
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►In (15.8.8) when is a nonpositive integer is interpreted as .
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►Alternatively, if is a negative integer, then we interchange and
in
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►In a similar way, when is an integer limits are taken in (15.8.4) and (15.8.5) as follows.
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23: Bibliography M
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Two-point quasi-fractional approximations to the Airy function
.
J. Comput. Phys. 99 (2), pp. 337–340.
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On the roots of the Bessel and certain related functions.
Ann. of Math. 9 (1-6), pp. 23–30.
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Orthogonale Polynomsysteme mit einer besonderen Gestalt der erzeugenden Funktion.
J. Lond. Math. Soc. 9, pp. 6–13 (German).
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An improved calculation of the general elliptic integral of the second kind in the neighbourhood of
.
Numer. Math. 25 (1), pp. 99–101.
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A connection formula for the -confluent hypergeometric function.
SIGMA Symmetry Integrability Geom. Methods Appl. 9, pp. Paper 050, 13.
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24: Bibliography S
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Orthogonal polynomials arising in the numerical evaluation of inverse Laplace transforms.
Math. Tables Aids Comput. 9 (52), pp. 164–177.
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Evaluation of associated Legendre functions off the cut and parabolic cylinder functions.
Electron. Trans. Numer. Anal. 9, pp. 137–146.
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Perturbational results for diffraction of water-waves by nearly-vertical barriers.
IMA J. Appl. Math. 34 (1), pp. 99–117.
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A new Fortran program for the - angular momentum coefficient.
Comput. Phys. Comm. 56 (2), pp. 231–248.
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An Introduction to Basic Fourier Series.
Developments in Mathematics, Vol. 9, Kluwer Academic Publishers, Dordrecht.
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25: 19.5 Maclaurin and Related Expansions
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►where is the Gauss hypergeometric function (§§15.1 and 15.2(i)).
…where is an Appell function (§16.13).
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►Coefficients of terms up to are given in Lee (1990), along with tables of fractional errors in
and , , obtained by using 12 different truncations of (19.5.6) in (19.5.8) and (19.5.9).
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►Series expansions of and are surveyed and improved in Van de Vel (1969), and the case of is summarized in Gautschi (1975, §1.3.2).
For series expansions of when see Erdélyi et al. (1953b, §13.6(9)).
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26: 19.21 Connection Formulas
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►The complete cases of and have connection formulas resulting from those for the Gauss hypergeometric function (Erdélyi et al. (1953a, §2.9)).
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►The complete case of can be expressed in terms of and :
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is symmetric only in
and , but either (nonzero) or (nonzero) can be moved to the third position by using
…Because is completely symmetric, can be permuted on the right-hand side of (19.21.10) so that if the variables are real, thereby avoiding cancellations when is calculated from and (see §19.36(i)).
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►Connection formulas for are given in Carlson (1977b, pp. 99, 101, and 123–124).
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27: 34.4 Definition: Symbol
§34.4 Definition: Symbol
►The symbol is defined by the following double sum of products of symbols: …where the summation is taken over all admissible values of the ’s and ’s for each of the four symbols; compare (34.2.2) and (34.2.3). … ►where is defined as in §16.2. ►For alternative expressions for the symbol, written either as a finite sum or as other terminating generalized hypergeometric series of unit argument, see Varshalovich et al. (1988, §§9.2.1, 9.2.3).28: 16.26 Approximations
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►For discussions of the approximation of generalized hypergeometric functions and the Meijer -function in terms of polynomials, rational functions, and Chebyshev polynomials see Luke (1975, §§5.12 - 5.13) and Luke (1977b, Chapters 1 and 9).
29: 18.13 Continued Fractions
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►The following formulae are explicit cases of (18.2.34)–(18.2.36); this area is fully explored in §§18.30(vi) and 18.30(vii).
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18.13.3
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18.13.4
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►See also Cuyt et al. (2008, pp. 91–99).