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21: 18.16 Zeros
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►Let be the th positive zero of the Bessel function (§10.21(i)).
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►Let .
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►For , and with as in §18.16(ii),
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►In the notation of this reference , , and .
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§18.16(vii) Discriminants
…22: Bibliography T
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Asymptotic estimates of Stirling numbers.
Stud. Appl. Math. 89 (3), pp. 233–243.
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High Speed Numerical Integration of Fermi Dirac Integrals.
Master’s Thesis, Naval Postgraduate School, Monterey, CA.
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The Theory of Functions.
2nd edition, Oxford University Press, Oxford.
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Numerical Linear Algebra.
Society for Industrial and Applied Mathematics (SIAM), Philadelphia, PA.
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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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23: Bibliography G
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On high precision methods for computing integrals involving Bessel functions.
Math. Comp. 33 (147), pp. 1049–1057.
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On the generalization of a method for computing Bessel function integrals.
J. Comput. Appl. Math. 6 (2), pp. 167–168.
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The triplets of helium.
Philos. Trans. Roy. Soc. London Ser. A 228, pp. 151–196.
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Matrix Computations.
3rd edition, Johns Hopkins University Press, Baltimore, MD.
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Constructing wavefunctions for nonlocal potentials.
J. Chem. Phys. 52, pp. 6211–6217.
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24: 12.10 Uniform Asymptotic Expansions for Large Parameter
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►These cases are treated in §§12.10(vii)–12.10(viii).
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►Higher polynomials can be calculated from the recurrence relation
…and the then follow from
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§12.10(vii) Negative , . Expansions in Terms of Airy Functions
… ►The coefficients and are given by …25: 1.10 Functions of a Complex Variable
26: Bibliography
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Some orthogonal -polynomials.
Math. Nachr. 30, pp. 47–61.
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Solid State Physics.
Holt, Rinehart and Winston, New York.
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Orthogonal Polynomials and Special Functions.
CBMS-NSF Regional Conference Series in Applied Mathematics, Vol. 21, Society for Industrial and Applied Mathematics, Philadelphia, PA.
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Continuous -Hermite Polynomials when
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In
-series and Partitions (Minneapolis, MN, 1988),
IMA Vol. Math. Appl., Vol. 18, pp. 151–158.
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Singular Continuous Spectrum for a Class of Almost Periodic Jacobi Matrices.
Bulletin of the American Mathematical Society 6 (1), pp. 81–85.
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27: 32.7 Bäcklund Transformations
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►Let , , be solutions of with
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►satisfies with
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§32.7(vii) Sixth Painlevé Equation
►Let , , be solutions of with … ►Also, …28: Bibliography Q
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“Best possible” upper and lower bounds for the zeros of the Bessel function
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Trans. Amer. Math. Soc. 351 (7), pp. 2833–2859.
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29: 10.75 Tables
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Wills et al. (1982) tabulates , , , for , 35D.
MacDonald (1989) tabulates the first 30 zeros, in ascending order of absolute value in the fourth quadrant, of the function , 6D. (Other zeros of this function can be obtained by reflection in the imaginary axis).
Abramowitz and Stegun (1964, Chapter 11) tabulates , , , 10D; , , , 8D.
§10.75(vii) Integrals of Modified Bessel Functions
►Abramowitz and Stegun (1964, Chapter 11) tabulates , , , 7D; , , , 6D.
30: Bibliography N
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Error bounds for the large-argument asymptotic expansions of the Lommel and allied functions.
Stud. Appl. Math. 140 (4), pp. 508–541.
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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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COULN, a program for evaluating negative energy Coulomb functions.
Comput. Phys. Comm. 33 (4), pp. 413–419.
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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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