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31: 25.16 Mathematical Applications
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§25.16(i) Distribution of Primes
β–ΊIn studying the distribution of primes p x , Chebyshev (1851) introduced a function ψ ⁑ ( x ) (not to be confused with the digamma function used elsewhere in this chapter), given by … β–Ί H ⁑ ( s ) is the special case H ⁑ ( s , 1 ) of the function … β–Ί
25.16.14 r = 1 k = 1 r 1 r ⁒ k ⁒ ( r + k ) = 5 4 ⁒ ΢ ⁑ ( 3 ) ,
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25.16.15 r = 1 k = 1 r 1 r 2 ⁒ ( r + k ) = 3 4 ⁒ ΢ ⁑ ( 3 ) .
32: 3.5 Quadrature
β–ΊA special case is the rule for Hilbert transforms (§1.14(v)): … β–ΊIn more advanced methods points are sampled from a probability distribution, so that they are concentrated in regions that make the largest contribution to the integral. …
33: Bibliography M
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  • A. J. MacLeod (1996a) Algorithm 757: MISCFUN, a software package to compute uncommon special functions. ACM Trans. Math. Software 22 (3), pp. 288–301.
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  • A. J. MacLeod (2002a) Asymptotic expansions for the zeros of certain special functions. J. Comput. Appl. Math. 145 (2), pp. 261–267.
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  • A. M. Mathai (1993) A Handbook of Generalized Special Functions for Statistical and Physical Sciences. Oxford Science Publications, The Clarendon Press Oxford University Press, New York.
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  • L. C. Maximon (1955) On the evaluation of indefinite integrals involving the special functions: Application of method. Quart. Appl. Math. 13, pp. 84–93.
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  • J. W. Meijer and N. H. G. Baken (1987) The exponential integral distribution. Statist. Probab. Lett. 5 (3), pp. 209–211.
  • 34: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
    β–ΊIn this section we will only consider the special case w ⁒ ( x ) = 1 , so d Ξ± ⁒ ( x ) = d x ; in which case L 2 ⁑ ( X ) L 2 ⁑ ( X , d x ) . … β–Ίof the Dirac delta distribution. … β–ΊThe special form of (1.18.28) is especially useful for applications in physics, as the connection to non-relativistic quantum mechanics is immediate:  d 2 d x 2 being proportional to the kinetic energy operator for a single particle in one dimension, q ⁒ ( x ) being proportional to the potential energy, often written as V ⁒ ( x ) , of that same particle, and which is simply a multiplicative operator. … β–ΊFor a formally self-adjoint second order differential operator β„’ , such as that of (1.18.28), the space π’Ÿ ⁒ ( β„’ ) can be seen to consist of all f L 2 ⁑ ( X ) such that the distribution β„’ ⁒ f can be identified with a function in L 2 ⁑ ( X ) , which is the function β„’ ⁒ f . …