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1: 15.10 Hypergeometric Differential Equation
§15.10(ii) Kummer’s 24 Solutions and Connection Formulas
The three pairs of fundamental solutions given by (15.10.2), (15.10.4), and (15.10.6) can be transformed into 18 other solutions by means of (15.8.1), leading to a total of 24 solutions known as Kummer’s solutions. … The ( 6 3 ) = 20 connection formulas for the principal branches of Kummer’s solutions are:
15.10.17 w 3 ( z ) = Γ ( 1 - c ) Γ ( a + b - c + 1 ) Γ ( a - c + 1 ) Γ ( b - c + 1 ) w 1 ( z ) + Γ ( c - 1 ) Γ ( a + b - c + 1 ) Γ ( a ) Γ ( b ) w 2 ( z ) ,
15.10.25 w 1 ( z ) = Γ ( c ) Γ ( b - a ) Γ ( b ) Γ ( c - a ) w 5 ( z ) + Γ ( c ) Γ ( a - b ) Γ ( a ) Γ ( c - b ) w 6 ( z ) ,
2: 13.2 Definitions and Basic Properties
Standard Solutions
The first two standard solutions are: … Another standard solution of (13.2.1) is U ( a , b , z ) , which is determined uniquely by the property …
§13.2(v) Numerically Satisfactory Solutions
3: 12.7 Relations to Other Functions
12.7.12 u 1 ( a , z ) = e - 1 4 z 2 M ( 1 2 a + 1 4 , 1 2 , 1 2 z 2 ) = e 1 4 z 2 M ( - 1 2 a + 1 4 , 1 2 , - 1 2 z 2 ) ,
12.7.13 u 2 ( a , z ) = z e - 1 4 z 2 M ( 1 2 a + 3 4 , 3 2 , 1 2 z 2 ) = z e 1 4 z 2 M ( - 1 2 a + 3 4 , 3 2 , - 1 2 z 2 ) .
4: 13.14 Definitions and Basic Properties
Standard solutions are: …
5: 13.29 Methods of Computation
The integral representations (13.4.1) and (13.4.4) can be used to compute the Kummer functions, and (13.16.1) and (13.16.5) for the Whittaker functions. In Allasia and Besenghi (1991) and Allasia and Besenghi (1987a) the high accuracy of the trapezoidal rule for the computation of Kummer functions is described. … with recessive solutionwith recessive solutionIn Colman et al. (2011) an algorithm is described that uses expansions in continued fractions for high-precision computation of M ( n , b , x ) , when b and x are real and n is a positive integer. …
6: Errata
  • Equation (13.2.7)
    13.2.7 U ( - m , b , z ) = ( - 1 ) m ( b ) m M ( - m , b , z ) = ( - 1 ) m s = 0 m ( m s ) ( b + s ) m - s ( - z ) s

    The equality U ( - m , b , z ) = ( - 1 ) m ( b ) m M ( - m , b , z ) has been added to the original equation to express an explicit connection between the two standard solutions of Kummer’s equation. Note also that the notation a = - n has been changed to a = - m .

    Reported 2015-02-10 by Adri Olde Daalhuis.

  • Equation (13.2.8)
    13.2.8 U ( a , a + n + 1 , z ) = ( - 1 ) n ( 1 - a - n ) n z a + n M ( - n , 1 - a - n , z ) = z - a s = 0 n ( n s ) ( a ) s z - s

    The equality U ( a , a + n + 1 , z ) = ( - 1 ) n ( 1 - a - n ) n z a + n M ( - n , 1 - a - n , z ) has been added to the original equation to express an explicit connection between the two standard solutions of Kummer’s equation.

    Reported 2015-02-10 by Adri Olde Daalhuis.

  • Equation (13.2.10)
    13.2.10 U ( - m , n + 1 , z ) = ( - 1 ) m ( n + 1 ) m M ( - m , n + 1 , z ) = ( - 1 ) m s = 0 m ( m s ) ( n + s + 1 ) m - s ( - z ) s

    The equality U ( - m , n + 1 , z ) = ( - 1 ) m ( n + 1 ) m M ( - m , n + 1 , z ) has been added to the original equation to express an explicit connection between the two standard solutions of Kummer’s equation. Note also that the notation a = - m , m = 0 , 1 , 2 , has been introduced.

    Reported 2015-02-10 by Adri Olde Daalhuis.

  • 7: 31.3 Basic Solutions
    The full set of 192 local solutions of (31.2.1), equivalent in 8 sets of 24, resembles Kummer’s set of 24 local solutions of the hypergeometric equation, which are equivalent in 4 sets of 6 solutions15.10(ii)); see Maier (2007).
    8: 13.28 Physical Applications
    §13.28 Physical Applications
    §13.28(i) Exact Solutions of the Wave Equation
    and V κ , μ ( j ) ( z ) , j = 1 , 2 , denotes any pair of solutions of Whittaker’s equation (13.14.1). …
    9: 12.14 The Function W ( a , x )
    12.14.15 w 1 ( a , x ) = e - 1 4 i x 2 M ( 1 4 - 1 2 i a , 1 2 , 1 2 i x 2 ) = e 1 4 i x 2 M ( 1 4 + 1 2 i a , 1 2 , - 1 2 i x 2 ) ,
    12.14.16 w 2 ( a , x ) = x e - 1 4 i x 2 M ( 3 4 - 1 2 i a , 3 2 , 1 2 i x 2 ) = x e 1 4 i x 2 M ( 3 4 + 1 2 i a , 3 2 , - 1 2 i x 2 ) .
    10: Bibliography K
  • K. Kajiwara and Y. Ohta (1996) Determinant structure of the rational solutions for the Painlevé II equation. J. Math. Phys. 37 (9), pp. 4693–4704.
  • K. Kajiwara and Y. Ohta (1998) Determinant structure of the rational solutions for the Painlevé IV equation. J. Phys. A 31 (10), pp. 2431–2446.
  • A. A. Kapaev (1988) Asymptotic behavior of the solutions of the Painlevé equation of the first kind. Differ. Uravn. 24 (10), pp. 1684–1695 (Russian).
  • N. M. Katz (1975) The congruences of Clausen-von Staudt and Kummer for Bernoulli-Hurwitz numbers. Math. Ann. 216 (1), pp. 1–4.
  • Y. A. Kravtsov (1964) Asymptotic solution of Maxwell’s equations near caustics. Izv. Vuz. Radiofiz. 7, pp. 1049–1056.