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21—30 of 67 matching pages
21: Bibliography C
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A recurrence formula for
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Proc. Amer. Math. Soc. 12 (6), pp. 991–992.
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Hadronic matter at high density.
Phys. Rev. D 5 (12), pp. 3231–3242.
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Numerical integration of related Hankel transforms by quadrature and continued fraction expansion.
Geophysics 48 (12), pp. 1671–1686.
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Incomplete Hankel and modified Bessel functions: A class of special functions for electromagnetics.
IEEE Trans. Antennas and Propagation 52 (12), pp. 3373–3389.
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Algorithm 352: Characteristic values and associated solutions of Mathieu’s differential equation.
Comm. ACM 12 (7), pp. 399–407.
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22: 2.8 Differential Equations with a Parameter
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►For example, can be the order of a Bessel function or degree of an orthogonal polynomial.
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§2.8(iv) Case III: Simple Pole
… ►For error bounds, more delicate error estimates, extensions to complex , , and , zeros, and examples see Olver (1997b, Chapter 12), Boyd (1990a), and Dunster (1990a). … ►For a coalescing turning point and double pole see Boyd and Dunster (1986) and Dunster (1990b); in this case the uniform approximants are Bessel functions of variable order. … ►Lastly, for an example of a fourth-order differential equation, see Wong and Zhang (2007). …23: Bibliography K
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The Rayleigh function: Theory and computational methods.
Zh. Vychisl. Mat. Mat. Fiz. 39 (12), pp. 1962–2006.
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Exponentially accurate uniform asymptotic approximations for integrals and Bleistein’s method revisited.
Proc. R. Soc. Lond. Ser. A Math. Phys. Eng. Sci. 469 (2153), pp. 20130008, 12.
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Algorithm 877: A subroutine package for cylindrical functions of complex order and nonnegative argument.
ACM Trans. Math. Software 34 (4), pp. Art. 22, 21.
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Electromagnetic eigenfrequencies in a spheroidal cavity (calculation by spheroidal eigenvectors).
J. Electromagn. Waves Appl. 12 (12), pp. 1601–1624.
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Sur le problème de la rotation d’un corps solide autour d’un point fixe.
Acta Math. 12 (1), pp. 177–232 (French).
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24: Software Index
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25: 3.6 Linear Difference Equations
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►Many special functions satisfy second-order recurrence relations, or difference equations, of the form
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§3.6(vii) Linear Difference Equations of Other Orders
►Similar considerations apply to the first-order equation … ►For a difference equation of order (), …or for systems of first-order inhomogeneous equations, boundary-value methods are the rule rather than the exception. …26: Bibliography T
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Error bounds for the Liouville-Green approximation to initial-value problems.
Z. Angew. Math. Mech. 58 (12), pp. 529–537.
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Steepest descent paths for integrals defining the modified Bessel functions of imaginary order.
Methods Appl. Anal. 1 (1), pp. 14–24.
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Eigenfunction Expansions Associated with Second-Order Differential Equations.
Clarendon Press, Oxford.
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Representation Theory and Harmonic Analysis.
Contemporary Mathematics, Vol. 191, American Mathematical Society, Providence, RI.
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Algebraic transformations of hypergeometric functions and automorphic forms on Shimura curves.
Trans. Amer. Math. Soc. 365 (12), pp. 6697–6729.
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27: 27.13 Functions
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27.13.3
►where the are integers, positive, negative, or zero, and the order of the summands is taken into account.
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►In fact, there are four representations, given by , and four more with the order of summands reversed.
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►Explicit formulas for have been obtained by similar methods for , and , but they are more complicated.
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28: Bibliography I
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The eigenvalue problem for infinite compact complex symmetric matrices with application to the numerical computation of complex zeros of and of Bessel functions of any real order
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Linear Algebra Appl. 194, pp. 35–70.
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Computing zeros and orders of Bessel functions.
J. Comput. Appl. Math. 38 (1-3), pp. 169–184.
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Computation of integrals over the half-line involving products of Bessel functions, with application to microwave transmission lines.
Z. Angew. Math. Mech. 75 (12), pp. 917–926.
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29: 3.5 Quadrature
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3.5.1
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3.5.3
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►If in (3.5.4) is not arbitrarily large, and if odd-order derivatives of are known at the end points and , then the composite trapezoidal rule can be improved by means of the Euler–Maclaurin formula (§2.10(i)).
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►The Gauss nodes (the zeros of ) are the eigenvalues of the (symmetric tridiagonal) Jacobi matrix of order
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►With function values, the Monte Carlo method aims at an error of order
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30: Bibliography R
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A code to calculate (high order) Bessel functions based on the continued fractions method.
Comput. Phys. Comm. 76 (3), pp. 381–388.
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Algorithm 935: IIPBF, a MATLAB toolbox for infinite integral of products of two Bessel functions.
ACM Trans. Math. Softw. 40 (2), pp. 14:1–14:12.
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On the definition and properties of generalized - symbols.
J. Math. Phys. 20 (12), pp. 2398–2415.
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Mathieu functions of integral orders and real arguments.
IEEE Trans. Microwave Theory Tech. 28 (3), pp. 276–277.
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Another proof of the triple sum formula for Wigner -symbols.
J. Math. Phys. 40 (12), pp. 6689–6691.
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