房产继承公证书【somewhat微aptao168】83w
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11: Bibliography V
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Some novel infinite series of spherical Bessel functions.
Quart. Appl. Math. 42 (3), pp. 321–324.
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Dritter Beweis der die unvollständige Gammafunktion betreffenden Lochsschen Ungleichungen.
Österreich. Akad. Wiss. Math.-Natur. Kl. Sitzungsber. II 192 (1-3), pp. 83–91 (German).
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12: Bibliography D
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The Radon Transform and Some of Its Applications.
A Wiley-Interscience Publication, John Wiley & Sons Inc., New York.
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Über die Bestimmung der mittleren Werthe in der Zahlentheorie.
Abhandlungen der Königlich Preussischen Akademie der
Wissenschaften von 1849, pp. 69–83 (German).
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Infinite integrals in the theory of Bessel functions.
Quart. J. Math., Oxford Ser. 1 (1), pp. 122–145.
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Hydrodynamic Stability.
Cambridge University Press, Cambridge.
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Uniform asymptotic approximations for the Whittaker functions and
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Anal. Appl. (Singap.) 1 (2), pp. 199–212.
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13: 4.44 Other Applications
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►For applications of generalized exponentials and generalized logarithms to computer arithmetic see §3.1(iv).
►For an application of the Lambert -function to generalized Gaussian noise see Chapeau-Blondeau and Monir (2002).
For other applications of the Lambert -function see Corless et al. (1996).
14: 9.11 Products
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►where and are any solutions of (9.2.1).
For example, , , , .
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►Let be any solutions of (9.2.1), not necessarily distinct.
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9.11.10
►For , , , where is any positive integer, see Albright (1977).
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15: 10.13 Other Differential Equations
16: 1.13 Differential Equations
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►The equation
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►Two solutions and are called a fundamental pair if any other solution is expressible as
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►The Wronskian of and is defined by
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►The following three statements are equivalent: and comprise a fundamental pair in ; does not vanish in ; and are linearly independent, that is, the only constants and such that
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►then is a solution of
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17: 10.36 Other Differential Equations
18: 3.6 Linear Difference Equations
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►Given numerical values of and , the solution of the equation
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►But suppose that is a nontrivial solution such that
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►Then computation of by forward recursion is unstable.
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►beginning with .
…Then is generated by backward recursion from
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19: 28.30 Expansions in Series of Eigenfunctions
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►Let , , be the set of characteristic values (28.29.16) and (28.29.17), arranged in their natural order (see (28.29.18)), and let , , be the eigenfunctions, that is, an orthonormal set of -periodic solutions; thus
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28.30.1
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28.30.2
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28.30.3
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28.30.4
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