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11: Bibliography S
  • F. C. Smith (1939a) On the logarithmic solutions of the generalized hypergeometric equation when p = q + 1 . Bull. Amer. Math. Soc. 45 (8), pp. 629–636.
  • F. C. Smith (1939b) Relations among the fundamental solutions of the generalized hypergeometric equation when p = q + 1 . II. Logarithmic cases. Bull. Amer. Math. Soc. 45 (12), pp. 927–935.
  • C. Snow (1952) Hypergeometric and Legendre Functions with Applications to Integral Equations of Potential Theory. National Bureau of Standards Applied Mathematics Series, No. 19, U. S. Government Printing Office, Washington, D.C..
  • 12: 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 solutions (§15.10(ii)); see Maier (2007).
    13: 19.4 Derivatives and Differential Equations
    If ϕ = π / 2 , then these two equations become hypergeometric differential equations (15.10.1) for K ( k ) and E ( k ) . …
    14: 15.19 Methods of Computation
    A comprehensive and powerful approach is to integrate the hypergeometric differential equation (15.10.1) by direct numerical methods. …
    15: 15.5 Derivatives and Contiguous Functions
    15.5.16_5 F ( a , b ; c ; z ) F ( a 1 , b ; c ; z ) ( b / c ) z F ( a , b + 1 ; c + 1 ; z ) = 0 ,
    An equivalent equation to the hypergeometric differential equation (15.10.1) is …
    16: 32.10 Special Function Solutions
    §32.10(vi) Sixth Painlevé Equation
    where the fundamental periods 2 ϕ 1 and 2 ϕ 2 are linearly independent functions satisfying the hypergeometric equation
    17: 16.13 Appell Functions
    The following four functions of two real or complex variables x and y cannot be expressed as a product of two F 1 2 functions, in general, but they satisfy partial differential equations that resemble the hypergeometric differential equation (15.10.1): …
    18: 17.17 Physical Applications
    See Kassel (1995). …
    19: 13.2 Definitions and Basic Properties
    13.2.1 z d 2 w d z 2 + ( b z ) d w d z a w = 0 .
    It can be regarded as the limiting form of the hypergeometric differential equation15.10(i)) that is obtained on replacing z by z / b , letting b , and subsequently replacing the symbol c by b . In effect, the regular singularities of the hypergeometric differential equation at b and coalesce into an irregular singularity at . …
    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 .
    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 .
    20: Bibliography M
  • R. S. Maier (2005) On reducing the Heun equation to the hypergeometric equation. J. Differential Equations 213 (1), pp. 171–203.