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21: 4.14 Definitions and Periodicity
4.14.3 cos z ± i sin z = e ± i z ,
22: Bibliography B
  • R. Barakat (1961) Evaluation of the incomplete gamma function of imaginary argument by Chebyshev polynomials. Math. Comp. 15 (73), pp. 7–11.
  • A. O. Barut and L. Girardello (1971) New “coherent” states associated with non-compact groups. Comm. Math. Phys. 21 (1), pp. 41–55.
  • B. C. Berndt, S. Bhargava, and F. G. Garvan (1995) Ramanujan’s theories of elliptic functions to alternative bases. Trans. Amer. Math. Soc. 347 (11), pp. 4163–4244.
  • F. Bethuel (1998) Vortices in Ginzburg-Landau Equations. In Proceedings of the International Congress of Mathematicians, Vol. III (Berlin, 1998), pp. 11–19.
  • R. L. Bishop (1981) Rainbow over Woolsthorpe Manor. Notes and Records Roy. Soc. London 36 (1), pp. 3–11 (1 plate).
  • 23: 8.21 Generalized Sine and Cosine Integrals
    8.21.4 si ( a , z ) = z t a 1 sin t d t , a < 1 ,
    8.21.5 ci ( a , z ) = z t a 1 cos t d t , a < 1 ,
    8.21.18 f ( a , z ) = si ( a , z ) cos z ci ( a , z ) sin z ,
    8.21.22 f ( a , z ) = 0 sin t ( t + z ) 1 a d t ,
    8.21.23 g ( a , z ) = 0 cos t ( t + z ) 1 a d t .
    24: 10.12 Generating Function and Associated Series
    For z and t { 0 } , …
    25: Bibliography M
  • D. A. MacDonald (1997) On the computation of zeroes of J n ( z ) i J n + 1 ( z ) = 0 . Quart. Appl. Math. 55 (4), pp. 623–633.
  • M. Mazzocco (2001a) Rational solutions of the Painlevé VI equation. J. Phys. A 34 (11), pp. 2281–2294.
  • L. Moser and M. Wyman (1958b) Stirling numbers of the second kind. Duke Math. J. 25 (1), pp. 29–43.
  • D. Müller, B. G. Kelly, and J. J. O’Brien (1994) Spheroidal eigenfunctions of the tidal equation. Phys. Rev. Lett. 73 (11), pp. 1557–1560.
  • L. A. Muraveĭ (1976) Zeros of the function A i ( z ) σ A i ( z ) . Differential Equations 11, pp. 797–811.
  • 26: 22.15 Inverse Functions
    Comprehensive treatments are given by Carlson (2005), Lawden (1989, pp. 52–55), Bowman (1953, Chapter IX), and Erdélyi et al. (1953b, pp. 296–301). …
    27: 4.24 Inverse Trigonometric Functions: Further Properties
    4.24.13 Arcsin u ± Arcsin v = Arcsin ( u ( 1 v 2 ) 1 / 2 ± v ( 1 u 2 ) 1 / 2 ) ,
    4.24.14 Arccos u ± Arccos v = Arccos ( u v ( ( 1 u 2 ) ( 1 v 2 ) ) 1 / 2 ) ,
    4.24.15 Arctan u ± Arctan v = Arctan ( u ± v 1 u v ) ,
    4.24.16 Arcsin u ± Arccos v = Arcsin ( u v ± ( ( 1 u 2 ) ( 1 v 2 ) ) 1 / 2 ) = Arccos ( v ( 1 u 2 ) 1 / 2 u ( 1 v 2 ) 1 / 2 ) ,
    4.24.17 Arctan u ± Arccot v = Arctan ( u v ± 1 v u ) = Arccot ( v u u v ± 1 ) .
    28: 24.13 Integrals
    For other integrals see Prudnikov et al. (1990, pp. 55–57).
    29: Staff
  • Adri B. Olde Daalhuis, University of Edinburgh, Chaps. 13, 15, 16

  • Richard B. Paris, University of Abertay, Chaps. 8, 11

  • Hans Volkmer, University of Wisconsin, Milwaukee, Chaps. 29, 30

  • Richard B. Paris, University of Abertay Dundee, for Chaps. 8, 11 (deceased)

  • Hans Volkmer, University of Wisconsin–Milwaukee, for Chaps. 29, 30

  • 30: 34.6 Definition: 9 j Symbol
    34.6.1 { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } = all  m r s ( j 11 j 12 j 13 m 11 m 12 m 13 ) ( j 21 j 22 j 23 m 21 m 22 m 23 ) ( j 31 j 32 j 33 m 31 m 32 m 33 ) ( j 11 j 21 j 31 m 11 m 21 m 31 ) ( j 12 j 22 j 32 m 12 m 22 m 32 ) ( j 13 j 23 j 33 m 13 m 23 m 33 ) ,
    34.6.2 { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } = j ( 1 ) 2 j ( 2 j + 1 ) { j 11 j 21 j 31 j 32 j 33 j } { j 12 j 22 j 32 j 21 j j 23 } { j 13 j 23 j 33 j j 11 j 12 } .