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1: 1.13 Differential Equations
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§1.13(vii) Closed-Form Solutions
… βΊ§1.13(viii) Eigenvalues and Eigenfunctions: Sturm-Liouville and Liouville forms
… βΊThis is the Sturm-Liouville form of a second order differential equation, where ′ denotes . Assuming that satisfies un-mixed boundary conditions of the form … βΊTransformation to Liouville normal Form
…2: 26.3 Lattice Paths: Binomial Coefficients
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Table 26.3.2: Binomial coefficients for lattice paths.
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3 | 1 | 4 | 10 | 20 | 35 | 56 | 84 | 120 | 165 |
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26.3.4
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26.3.11
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§26.3(v) Limiting Form
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26.3.12
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3: 26.5 Lattice Paths: Catalan Numbers
4: 20 Theta Functions
Chapter 20 Theta Functions
…5: 33.18 Limiting Forms for Large
6: 26.9 Integer Partitions: Restricted Number and Part Size
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βΊThe conjugate to the example in Figure 26.9.1 is .
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βΊEquations (26.9.2)–(26.9.3) are examples of closed forms that can be computed explicitly for any positive integer .
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§26.9(iv) Limiting Form
…7: 26.10 Integer Partitions: Other Restrictions
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βΊThe set is denoted by .
If more than one restriction applies, then the restrictions are separated by commas, for example, .
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βΊwhere the sum is over nonnegative integer values of for which .
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βΊwhere the sum is over nonnegative integer values of for which .
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§26.10(v) Limiting Form
…8: 26.12 Plane Partitions
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βΊThe number of self-complementary plane partitions in is
…in it is
…in it is
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§26.12(iv) Limiting Form
…9: Bibliography D
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Recherches analytiques sur la théorie des nombres premiers. Première partie. La fonction de Riemann et les nombres premiers en général, suivi d’un Appendice sur des réflexions applicables à une formule donnée par Riemann.
Ann. Soc. Sci. Bruxelles 20, pp. 183–256 (French).
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Recherches analytiques sur la théorie des nombres premiers. Deuxième partie. Les fonctions de Dirichlet et les nombres premiers de la forme linéaire
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Ann. Soc. Sci. Bruxelles 20, pp. 281–397 (French).
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Complex zeros of cylinder functions.
Math. Comp. 20 (94), pp. 215–222.
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Uniform asymptotic expansions for Whittaker’s confluent hypergeometric functions.
SIAM J. Math. Anal. 20 (3), pp. 744–760.
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Bessel functions of purely imaginary order, with an application to second-order linear differential equations having a large parameter.
SIAM J. Math. Anal. 21 (4), pp. 995–1018.
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10: 6.16 Mathematical Applications
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βΊThese limits are not approached uniformly, however.
The first maximum of for positive occurs at and equals ; compare Figure 6.3.2.
Hence if and , then the limiting value of overshoots by approximately 18%.
Similarly if , then the limiting value of undershoots by approximately 10%, and so on.
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βΊIf we assume Riemann’s hypothesis that all nonreal zeros of have real part of (§25.10(i)), then
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