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31: 18.8 Differential Equations
Table 18.8.1: Classical OP’s: differential equations A ( x ) f ′′ ( x ) + B ( x ) f ( x ) + C ( x ) f ( x ) + λ n f ( x ) = 0 .
# f ( x ) A ( x ) B ( x ) C ( x ) λ n
2 ( sin 1 2 x ) α + 1 2 ( cos 1 2 x ) β + 1 2 × P n ( α , β ) ( cos x ) 1 0 1 4 α 2 4 sin 2 1 2 x + 1 4 β 2 4 cos 2 1 2 x ( n + 1 2 ( α + β + 1 ) ) 2
5 T n ( x ) 1 x 2 x 0 n 2
9 e 1 2 x 2 x α + 1 2 L n ( α ) ( x 2 ) 1 0 x 2 + ( 1 4 α 2 ) x 2 4 n + 2 α + 2
12 H n ( x ) 1 2 x 0 2 n
13 e 1 2 x 2 H n ( x ) 1 0 x 2 2 n + 1
32: 22.21 Tables
Spenceley and Spenceley (1947) tabulates sn ( K x , k ) , cn ( K x , k ) , dn ( K x , k ) , am ( K x , k ) , ( K x , k ) for arcsin k = 1 ( 1 ) 89 and x = 0 ( 1 90 ) 1 to 12D, or 12 decimals of a radian in the case of am ( K x , k ) . Curtis (1964b) tabulates sn ( m K / n , k ) , cn ( m K / n , k ) , dn ( m K / n , k ) for n = 2 ( 1 ) 15 , m = 1 ( 1 ) n 1 , and q (not k ) = 0 ( .005 ) 0.35 to 20D. … 5 to 2. 2. … Zhang and Jin (1996, p. 678) tabulates sn ( K x , k ) , cn ( K x , k ) , dn ( K x , k ) for k = 1 4 , 1 2 and x = 0 ( .1 ) 4 to 7D. …
33: 11.14 Tables
  • Abramowitz and Stegun (1964, Chapter 12) tabulates 𝐇 n ( x ) , 𝐇 n ( x ) Y n ( x ) , and I n ( x ) 𝐋 n ( x ) for n = 0 , 1 and x = 0 ( .1 ) 5 , x 1 = 0 ( .01 ) 0.2 to 6D or 7D.

  • Abramowitz and Stegun (1964, Chapter 12) tabulates 0 x ( I 0 ( t ) 𝐋 0 ( t ) ) d t and ( 2 / π ) x t 1 𝐇 0 ( t ) d t for x = 0 ( .1 ) 5 to 5D or 7D; 0 x ( 𝐇 0 ( t ) Y 0 ( t ) ) d t ( 2 / π ) ln x , 0 x ( I 0 ( t ) 𝐋 0 ( t ) ) d t ( 2 / π ) ln x , and x t 1 ( 𝐇 0 ( t ) Y 0 ( t ) ) d t for x 1 = 0 ( .01 ) 0.2 to 6D.

  • Jahnke and Emde (1945) tabulates 𝐄 n ( x ) for n = 1 , 2 and x = 0 ( .01 ) 14.99 to 4D.

  • Agrest and Maksimov (1971, Chapter 11) defines incomplete Struve, Anger, and Weber functions and includes tables of an incomplete Struve function 𝐇 n ( x , α ) for n = 0 , 1 , x = 0 ( .2 ) 10 , and α = 0 ( .2 ) 1.4 , 1 2 π , together with surface plots.

  • 34: 34.1 Special Notation
    2 j 1 , 2 j 2 , 2 j 3 , 2 l 1 , 2 l 2 , 2 l 3 nonnegative integers.
    ( j 1 j 2 j 3 m 1 m 2 m 3 ) ,
    { j 1 j 2 j 3 l 1 l 2 l 3 } ,
    { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } .
    An often used alternative to the 3 j symbol is the Clebsch–Gordan coefficient …
    35: 27.14 Unrestricted Partitions
    For example, p ( 5 ) = 7 because there are exactly seven partitions of 5 : 5 = 4 + 1 = 3 + 2 = 3 + 1 + 1 = 2 + 2 + 1 = 2 + 1 + 1 + 1 = 1 + 1 + 1 + 1 + 1 . … where the exponents 1 , 2 , 5 , 7 , 12 , 15 , are the pentagonal numbers, defined by … where K = π 2 / 3 (Hardy and Ramanujan (1918)). … where ε = exp ( π i ( ( ( a + d ) / ( 12 c ) ) s ( d , c ) ) ) and s ( d , c ) is given by (27.14.11). … The 24th power of η ( τ ) in (27.14.12) with e 2 π i τ = x is an infinite product that generates a power series in x with integer coefficients called Ramanujan’s tau function τ ( n ) : …
    36: 28.26 Asymptotic Approximations for Large q
    28.26.1 Mc m ( 3 ) ( z , h ) = e i ϕ ( π h cosh z ) 1 / 2 ( Fc m ( z , h ) i Gc m ( z , h ) ) ,
    28.26.3 ϕ = 2 h sinh z ( m + 1 2 ) arctan ( sinh z ) .
    Then as h + with fixed z in z > 0 and fixed s = 2 m + 1 ,
    28.26.4 Fc m ( z , h ) 1 + s 8 h cosh 2 z + 1 2 11 h 2 ( s 4 + 86 s 2 + 105 cosh 4 z s 4 + 22 s 2 + 57 cosh 2 z ) + 1 2 14 h 3 ( s 5 + 14 s 3 + 33 s cosh 2 z 2 s 5 + 124 s 3 + 1122 s cosh 4 z + 3 s 5 + 290 s 3 + 1627 s cosh 6 z ) + ,
    28.26.5 Gc m ( z , h ) sinh z cosh 2 z ( s 2 + 3 2 5 h + 1 2 9 h 2 ( s 3 + 3 s + 4 s 3 + 44 s cosh 2 z ) + 1 2 14 h 3 ( 5 s 4 + 34 s 2 + 9 s 6 47 s 4 + 667 s 2 + 2835 12 cosh 2 z + s 6 + 505 s 4 + 12139 s 2 + 10395 12 cosh 4 z ) ) + .
    37: Bibliography K
  • M. K. Kerimov and S. L. Skorokhodov (1985c) Calculation of the multiple zeros of the derivatives of the cylindrical Bessel functions J ν ( z ) and Y ν ( z ) . Zh. Vychisl. Mat. i Mat. Fiz. 25 (12), pp. 1749–1760, 1918.
  • M. K. Kerimov (1999) The Rayleigh function: Theory and computational methods. Zh. Vychisl. Mat. Mat. Fiz. 39 (12), pp. 1962–2006.
  • S. F. Khwaja and A. B. Olde Daalhuis (2013) 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.
  • G. C. Kokkorakis and J. A. Roumeliotis (1998) Electromagnetic eigenfrequencies in a spheroidal cavity (calculation by spheroidal eigenvectors). J. Electromagn. Waves Appl. 12 (12), pp. 1601–1624.
  • S. Kowalevski (1889) Sur le problème de la rotation d’un corps solide autour d’un point fixe. Acta Math. 12 (1), pp. 177–232 (French).
  • 38: 11 Struve and Related Functions
    39: 35.11 Tables
    Tables of zonal polynomials are given in James (1964) for | κ | 6 , Parkhurst and James (1974) for | κ | 12 , and Muirhead (1982, p. 238) for | κ | 5 . …
    40: Bibliography B
  • L. V. Babushkina, M. K. Kerimov, and A. I. Nikitin (1997) New tables of Bessel functions of complex argument. Comput. Math. Math. Phys. 37 (12), pp. 1480–1482.
  • J. Baik, P. Deift, and K. Johansson (1999) On the distribution of the length of the longest increasing subsequence of random permutations. J. Amer. Math. Soc. 12 (4), pp. 1119–1178.
  • W. N. Bailey (1938) The generating function of Jacobi polynomials. J. London Math. Soc. 13, pp. 8–12.
  • M. V. Berry (1977) Focusing and twinkling: Critical exponents from catastrophes in non-Gaussian random short waves. J. Phys. A 10 (12), pp. 2061–2081.
  • J. Buhler, R. Crandall, R. Ernvall, T. Metsänkylä, and M. A. Shokrollahi (2001) Irregular primes and cyclotomic invariants to 12 million. J. Symbolic Comput. 31 (1-2), pp. 89–96.