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11—20 of 919 matching pages
11: 9.10 Integrals
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βΊ
9.10.8
βΊ
9.10.9
βΊ
9.10.10
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βΊFor the confluent hypergeometric function and the incomplete gamma function see §§13.1, 13.2, and 8.2(i).
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βΊFor further integrals, including the Airy transform, see §9.11(iv), Widder (1979), Prudnikov et al. (1990, §1.8.1), Prudnikov et al. (1992a, pp. 405–413), Prudnikov et al. (1992b, §4.3.25), Vallée and Soares (2010, Chapters 3, 4).
12: Mark J. Ablowitz
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βΊTheir similarity solutions lead to special ODEs which have the Painlevé property; i.
…ODEs which do not have moveable branch point singularities.
ODEs with the Painlevé property contain the well-known Painlevé equations which are special second order scalar equations; their solutions are often called Painlevé transcendents.
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13: Bibliography I
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βΊ
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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The factorization method.
Rev. Modern Phys. 23 (1), pp. 21–68.
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The real roots of Bernoulli polynomials.
Ann. Univ. Turku. Ser. A I 37, pp. 1–20.
βΊ
Centre for Experimental and Constructive Mathematics, Simon Fraser University, Canada.
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βΊ
Bounds for the small real and purely imaginary zeros of Bessel and related functions.
Methods Appl. Anal. 2 (1), pp. 1–21.
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14: Sidebar 9.SB1: Supernumerary Rainbows
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βΊPhotograph by Dr. Roy Bishop, Physics Department, Acadia
University, Nova Scotia, Canada.
See Bishop (1981).
©R. L. Bishop.
15: Karl Dilcher
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βΊ 1954 in Wabern-Harle, Germany) is Professor in the Department of Mathematics and Statistics at Dalhousie University in Halifax, Nova Scotia, Canada.
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16: Stephen M. Watt
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βΊ 1959 in Montreal, Canada) is Professor of Computer Science in the David R.
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17: 22.19 Physical Applications
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βΊThis formulation gives the bounded and unbounded solutions from the same formula (22.19.3), for and , respectively.
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βΊ
Case I:
… βΊCase II:
… βΊCase III:
… βΊ§22.19(iii) Nonlinear ODEs and PDEs
…18: 28.9 Zeros
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βΊFor real each of the functions , , , and has exactly zeros in .
…For the zeros of and approach asymptotically the zeros of , and the zeros of and approach asymptotically the zeros of .
…There are no zeros within the strip other than those on the real and imaginary axes.
βΊFor further details see McLachlan (1947, pp. 234–239) and Meixner and Schäfke (1954, §§2.331, 2.8, 2.81, and 2.85).
19: Bibliography N
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βΊ
The resurgence properties of the large order asymptotics of the Anger-Weber function I.
J. Class. Anal. 4 (1), pp. 1–39.
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βΊ
Coulomb Functions for Large Values of the Parameter
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Technical report
Atomic Energy of Canada Limited, Chalk
River, Ontario.
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βΊ
Bisection hardly ever converges linearly.
Numer. Math. 70 (1), pp. 111–118.
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βΊ
Evaluation of negative energy Coulomb (Whittaker) functions.
Comput. Phys. Comm. 159 (1), pp. 55–62.
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βΊ
High-frequency scattering by an impenetrable sphere.
Ann. Physics 34 (1), pp. 23–95.
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20: Bibliography J
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βΊ
Density matrix of an impenetrable Bose gas and the fifth Painlevé transcendent.
Phys. D 1 (1), pp. 80–158.
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βΊ
Uniform asymptotic expansions for Meixner polynomials.
Constr. Approx. 14 (1), pp. 113–150.
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βΊ
REMES2 — a Fortran program to calculate rational minimax approximations to a given function.
Technical Report
Technical Report AECL-4210, Atomic Energy of Canada Limited. Chalk River Nuclear Laboratories, Chalk River, Ontario.
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βΊ
Note sur la série
.
Bull. Soc. Math. France 17, pp. 142–152 (French).
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βΊ
Memoire sur l’itération des fonctions rationnelles.
J. Math. Pures Appl. 8 (1), pp. 47–245 (French).