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21: 12.3 Graphics
See accompanying text
Figure 12.3.1: U ( a , x ) , a = 0. 5, 2, 3. 5, 5, 8. Magnify
See accompanying text
Figure 12.3.2: V ( a , x ) , a = 0. …5, 5, 8. Magnify
See accompanying text
Figure 12.3.5: U ( 8 , x ) , U ¯ ( 8 , x ) , F ( 8 , x ) , 4 2 x 4 2 . Magnify
See accompanying text
Figure 12.3.6: U ( 8 , x ) , U ¯ ( 8 , x ) , G ( 8 , x ) , 4 2 x 4 2 . Magnify
22: 17.16 Mathematical Applications
More recent applications are given in Gasper and Rahman (2004, Chapter 8) and Fine (1988, Chapters 1 and 2).
23: Bibliography
  • A. Abramov (1960) Tables of ln Γ ( z ) for Complex Argument. Pergamon Press, New York.
  • G. B. Airy (1849) Supplement to a paper “On the intensity of light in the neighbourhood of a caustic”. Trans. Camb. Phil. Soc. 8, pp. 595–599.
  • F. Alhargan and S. Judah (1992) Frequency response characteristics of the multiport planar elliptic patch. IEEE Trans. Microwave Theory Tech. 40 (8), pp. 1726–1730.
  • W. L. Anderson (1982) Algorithm 588. Fast Hankel transforms using related and lagged convolutions. ACM Trans. Math. Software 8 (4), pp. 369–370.
  • D. Atkinson and P. W. Johnson (1988) Chiral-symmetry breaking in QCD. I. The infrared domain. Phys. Rev. D (3) 37 (8), pp. 2290–2295.
  • 24: 24.21 Software
    §24.21(ii) B n , B n ( x ) , E n , and E n ( x )
    25: 24.8 Series Expansions
    If n = 1 with 0 < x < 1 , or n = 2 , 3 , with 0 x 1 , then …
    24.8.4 E 2 n ( x ) = ( 1 ) n 4 ( 2 n ) ! π 2 n + 1 k = 0 sin ( ( 2 k + 1 ) π x ) ( 2 k + 1 ) 2 n + 1 ,
    24.8.5 E 2 n 1 ( x ) = ( 1 ) n 4 ( 2 n 1 ) ! π 2 n k = 0 cos ( ( 2 k + 1 ) π x ) ( 2 k + 1 ) 2 n .
    24.8.6 B 4 n + 2 = ( 8 n + 4 ) k = 1 k 4 n + 1 e 2 π k 1 , n = 1 , 2 , ,
    24.8.9 E 2 n = ( 1 ) n k = 1 k 2 n cosh ( 1 2 π k ) 4 k = 0 ( 1 ) k ( 2 k + 1 ) 2 n e 2 π ( 2 k + 1 ) 1 , n = 1 , 2 , .
    26: 9.4 Maclaurin Series
    9.4.1 Ai ( z ) = Ai ( 0 ) ( 1 + 1 3 ! z 3 + 1 4 6 ! z 6 + 1 4 7 9 ! z 9 + ) + Ai ( 0 ) ( z + 2 4 ! z 4 + 2 5 7 ! z 7 + 2 5 8 10 ! z 10 + ) ,
    9.4.2 Ai ( z ) = Ai ( 0 ) ( 1 + 2 3 ! z 3 + 2 5 6 ! z 6 + 2 5 8 9 ! z 9 + ) + Ai ( 0 ) ( 1 2 ! z 2 + 1 4 5 ! z 5 + 1 4 7 8 ! z 8 + ) ,
    9.4.3 Bi ( z ) = Bi ( 0 ) ( 1 + 1 3 ! z 3 + 1 4 6 ! z 6 + 1 4 7 9 ! z 9 + ) + Bi ( 0 ) ( z + 2 4 ! z 4 + 2 5 7 ! z 7 + 2 5 8 10 ! z 10 + ) ,
    9.4.4 Bi ( z ) = Bi ( 0 ) ( 1 + 2 3 ! z 3 + 2 5 6 ! z 6 + 2 5 8 9 ! z 9 + ) + Bi ( 0 ) ( 1 2 ! z 2 + 1 4 5 ! z 5 + 1 4 7 8 ! z 8 + ) .
    27: 10.62 Graphs
    See accompanying text
    Figure 10.62.1: ber x , bei x , ber x , bei x , 0 x 8 . Magnify
    See accompanying text
    Figure 10.62.2: ker x , kei x , ker x , kei x , 0 x 8 . Magnify
    See accompanying text
    Figure 10.62.3: e x / 2 ber x , e x / 2 bei x , e x / 2 M ( x ) , 0 x 8 . Magnify
    See accompanying text
    Figure 10.62.4: e x / 2 ker x , e x / 2 kei x , e x / 2 N ( x ) , 0 x 8 . Magnify
    28: Software Index
    29: 19.2 Definitions
    The integral for E ( ϕ , k ) is well defined if k 2 = sin 2 ϕ = 1 , and the Cauchy principal value (§1.4(v)) of Π ( ϕ , α 2 , k ) is taken if 1 α 2 sin 2 ϕ vanishes at an interior point of the integration path. … The principal branch of K ( k ) and E ( k ) is | ph ( 1 k 2 ) | π , that is, the branch-cuts are ( , 1 ] [ 1 , + ) . The principal values of K ( k ) and E ( k ) are even functions. …
    §19.2(iv) A Related Function: R C ( x , y )
    For the special cases of R C ( x , x ) and R C ( 0 , y ) see (19.6.15). …
    30: 6.8 Inequalities
    6.8.1 1 2 ln ( 1 + 2 x ) < e x E 1 ( x ) < ln ( 1 + 1 x ) ,
    6.8.2 x x + 1 < x e x E 1 ( x ) < x + 1 x + 2 ,
    6.8.3 x ( x + 3 ) x 2 + 4 x + 2 < x e x E 1 ( x ) < x 2 + 5 x + 2 x 2 + 6 x + 6 .