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21: 36.4 Bifurcation Sets
β–ΊThese are real solutions t j ⁑ ( 𝐱 ) , 1 j j max ⁑ ( 𝐱 ) K + 1 , of … β–ΊThese are real solutions { s j ⁒ ( 𝐱 ) , t j ⁑ ( 𝐱 ) } , 1 j j max ⁑ ( 𝐱 ) 4 , of …
22: 36.11 Leading-Order Asymptotics
β–Ί
36.11.1 t 1 ⁑ ( 𝐱 ) < t 2 ⁑ ( 𝐱 ) < β‹― < t j max ⁑ ( 𝐱 ) ,
β–Ί
36.11.2 Ξ¨ K ⁑ ( 𝐱 ) = 2 ⁒ Ο€ ⁒ j = 1 j max ⁒ ( 𝐱 ) exp ⁑ ( i ⁒ ( Ξ¦ K ⁑ ( t j ⁑ ( 𝐱 ) ; 𝐱 ) + 1 4 ⁒ Ο€ ⁒ ( 1 ) j + K + 1 ) ) ⁒ | 2 Ξ¦ K ⁑ ( t j ⁑ ( 𝐱 ) ; 𝐱 ) t 2 | 1 / 2 ⁒ ( 1 + o ⁑ ( 1 ) ) .
23: Bibliography T
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  • G. Taubmann (1992) Parabolic cylinder functions U ⁒ ( n , x ) for natural n and positive x . Comput. Phys. Commun. 69, pp. 415–419.
  • β–Ί
  • N. M. Temme (1978) The numerical computation of special functions by use of quadrature rules for saddle point integrals. II. Gamma functions, modified Bessel functions and parabolic cylinder functions. Report TW 183/78 Mathematisch Centrum, Amsterdam, Afdeling Toegepaste Wiskunde.
  • β–Ί
  • H. C. Thacher Jr. (1963) Algorithm 165: Complete elliptic integrals. Comm. ACM 6 (4), pp. 163–164.
  • β–Ί
  • W. J. Thompson (1997) Atlas for Computing Mathematical Functions: An Illustrated Guide for Practitioners. John Wiley & Sons Inc., New York.
  • 24: 19.27 Asymptotic Approximations and Expansions
    β–Ί
    19.27.13 R J ⁑ ( x , y , z , p ) = 3 2 ⁒ z ⁒ p ⁒ ( ln ⁑ ( 8 ⁒ z a + g ) 2 ⁒ R C ⁑ ( 1 , p z ) + O ⁑ ( ( a z + a p ) ⁒ ln ⁑ p a ) ) , max ⁑ ( x , y ) / min ⁑ ( z , p ) 0 .
    β–Ί
    19.27.14 R J ⁑ ( x , y , z , p ) = 3 y ⁒ z ⁒ R C ⁑ ( x , p ) 6 y ⁒ z ⁒ R G ⁑ ( 0 , y , z ) + O ⁑ ( x + 2 ⁒ p y ⁒ z ) , max ⁑ ( x , p ) / min ⁑ ( y , z ) 0 .
    β–Ί
    19.27.16 R J ⁑ ( x , y , z , p ) = ( 3 / x ) ⁒ R C ⁑ ( ( h + p ) 2 , 2 ⁒ ( b + h ) ⁒ p ) + O ⁑ ( 1 x 3 / 2 ⁒ ln ⁑ x b + h ) , max ⁑ ( y , z , p ) / x 0 .
    25: 3.11 Approximation Techniques
    β–ΊA sufficient condition for p n ⁑ ( x ) to be the minimax polynomial is that | Ο΅ n ⁑ ( x ) | attains its maximum at n + 2 distinct points in [ a , b ] and Ο΅ n ⁑ ( x ) changes sign at these consecutive maxima. … β–Ί(Thus the m j are approximations to m , where ± m is the maximum value of | Ο΅ n ⁑ ( x ) | on [ a , b ] .) … β–ΊMore precisely, it is known that for the interval [ a , b ] , the ratio of the maximum value of the remainder …to the maximum error of the minimax polynomial p n ⁑ ( x ) is bounded by 1 + L n , where L n is the n th Lebesgue constant for Fourier series; see §1.8(i). … β–Ίand ± m is the maximum of | Ο΅ k , β„“ ⁑ ( x ) | on [ a , b ] . …
    26: Bibliography D
    β–Ί
  • Delft Numerical Analysis Group (1973) On the computation of Mathieu functions. J. Engrg. Math. 7, pp. 39–61.
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  • G. Delic (1979a) Chebyshev expansion of the associated Legendre polynomial P L M ⁒ ( x ) . Comput. Phys. Comm. 18 (1), pp. 63–71.
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  • A. R. DiDonato and A. H. Morris (1987) Algorithm 654: Fortran subroutines for computing the incomplete gamma function ratios and their inverses. ACM Trans. Math. Software 13 (3), pp. 318–319.
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  • A. R. DiDonato and A. H. Morris (1992) Algorithm 708: Significant digit computation of the incomplete beta function ratios. ACM Trans. Math. Software 18 (3), pp. 360–373.
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  • E. Dorrer (1968) Algorithm 322. F-distribution. Comm. ACM 11 (2), pp. 116–117.
  • 27: 6.16 Mathematical Applications
    β–ΊThe first maximum of 1 2 ⁒ Si ⁑ ( x ) for positive x occurs at x = Ο€ and equals ( 1.1789 ⁒ ) × 1 4 ⁒ Ο€ ; compare Figure 6.3.2. …
    28: 14.21 Definitions and Basic Properties
    β–ΊThe generating function expansions (14.7.19) (with 𝖯 replaced by P ) and (14.7.22) apply when | h | < min ⁑ | z ± ( z 2 1 ) 1 / 2 | ; (14.7.21) (with 𝖯 replaced by P ) applies when | h | > max ⁑ | z ± ( z 2 1 ) 1 / 2 | .
    29: 19.34 Mutual Inductance of Coaxial Circles
    β–Ίis the square of the maximum (upper signs) or minimum (lower signs) distance between the circles. …
    30: 27.4 Euler Products and Dirichlet Series
    β–Ί
    27.4.11 n = 1 Οƒ Ξ± ⁑ ( n ) ⁒ n s = ΞΆ ⁑ ( s ) ⁒ ΞΆ ⁑ ( s Ξ± ) , ⁑ s > max ⁑ ( 1 , 1 + ⁑ Ξ± ) ,