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Kummer equation

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11: 13.11 Series
13.11.2 M ( a , b , z ) = Γ ( b - a - 1 2 ) e 1 2 z ( 1 4 z ) a - b + 1 2 s = 0 ( - 1 ) s ( 2 b - 2 a - 1 ) s ( b - 2 a ) s ( b - a - 1 2 + s ) ( b ) s s ! I b - a - 1 2 + s ( 1 2 z ) , b - a + 1 2 , b 0 , - 1 , - 2 , .
13.11.3 M ( a , b , z ) = e 1 2 z s = 0 A s ( b - 2 a ) 1 2 ( 1 - b - s ) ( 1 2 z ) 1 2 ( 1 - b + s ) J b - 1 + s ( 2 z ( b - 2 a ) ) ,
12: 13.6 Relations to Other Functions
13.6.11_1 M ( ν + 1 2 , 2 ν + 1 + n , 2 z ) = Γ ( ν ) e z ( z / 2 ) - ν k = 0 n ( - n ) k ( 2 ν ) k ( ν + k ) ( 2 ν + 1 + n ) k k ! I ν + k ( z ) ,
13.6.11_2 M ( ν + 1 2 , 2 ν + 1 - n , 2 z ) = Γ ( ν - n ) e z ( z / 2 ) n - ν k = 0 n ( - 1 ) k ( - n ) k ( 2 ν - 2 n ) k ( ν - n + k ) ( 2 ν + 1 - n ) k k ! I ν + k - n ( z ) .
13: 13.13 Addition and Multiplication Theorems
§13.13(i) Addition Theorems for M ( a , b , z )
The function M ( a , b , x + y ) has the following expansions: …
§13.13(ii) Addition Theorems for U ( a , b , z )
The function U ( a , b , x + y ) has the following expansions: …
§13.13(iii) Multiplication Theorems for M ( a , b , z ) and U ( a , b , z )
14: 9.6 Relations to Other Functions
9.6.26 Bi ( z ) = 3 1 / 6 Γ ( 1 3 ) e - ζ F 1 1 ( - 1 6 ; - 1 3 ; 2 ζ ) + 3 7 / 6 2 7 / 3 Γ ( 2 3 ) ζ 4 / 3 e - ζ F 1 1 ( 7 6 ; 7 3 ; 2 ζ ) .
15: 10.16 Relations to Other Functions
Principal values on each side of these equations correspond. …
10.16.5 J ν ( z ) = ( 1 2 z ) ν e i z Γ ( ν + 1 ) M ( ν + 1 2 , 2 ν + 1 , ± 2 i z ) ,
10.16.6 H ν ( 1 ) ( z ) H ν ( 2 ) ( z ) } = 2 π - 1 2 i e ν π i ( 2 z ) ν e ± i z U ( ν + 1 2 , 2 ν + 1 , 2 i z ) .
For the functions M and U see §13.2(i). …
16: 10.39 Relations to Other Functions
Principal values on each side of these equations correspond. …
10.39.5 I ν ( z ) = ( 1 2 z ) ν e ± z Γ ( ν + 1 ) M ( ν + 1 2 , 2 ν + 1 , 2 z ) ,
For the functions M , U , M 0 , ν , and W 0 , ν see §§13.2(i) and 13.14(i). …
17: Bibliography K
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  • 18: Bibliography Z
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  • A. Zarzo, J. S. Dehesa, and R. J. Yañez (1995) Distribution of zeros of Gauss and Kummer hypergeometric functions. A semiclassical approach. Ann. Numer. Math. 2 (1-4), pp. 457–472.
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  • 19: Bibliography D
  • A. Deaño, J. Segura, and N. M. Temme (2010) Computational properties of three-term recurrence relations for Kummer functions. J. Comput. Appl. Math. 233 (6), pp. 1505–1510.
  • A. Debosscher (1998) Unification of one-dimensional Fokker-Planck equations beyond hypergeometrics: Factorizer solution method and eigenvalue schemes. Phys. Rev. E (3) 57 (1), pp. 252–275.
  • A. Decarreau, M.-Cl. Dumont-Lepage, P. Maroni, A. Robert, and A. Ronveaux (1978a) Formes canoniques des équations confluentes de l’équation de Heun. Ann. Soc. Sci. Bruxelles Sér. I 92 (1-2), pp. 53–78.
  • A. Decarreau, P. Maroni, and A. Robert (1978b) Sur les équations confluentes de l’équation de Heun. Ann. Soc. Sci. Bruxelles Sér. I 92 (3), pp. 151–189.
  • B. Deconinck and H. Segur (1998) The KP equation with quasiperiodic initial data. Phys. D 123 (1-4), pp. 123–152.
  • 20: Bibliography P
  • P. Painlevé (1906) Sur les équations différentielles du second ordre à points critiques fixès. C.R. Acad. Sc. Paris 143, pp. 1111–1117.
  • R. B. Paris (1992a) Smoothing of the Stokes phenomenon for high-order differential equations. Proc. Roy. Soc. London Ser. A 436, pp. 165–186.
  • R. B. Paris (2002b) A uniform asymptotic expansion for the incomplete gamma function. J. Comput. Appl. Math. 148 (2), pp. 323–339.
  • R. B. Paris (2005a) A Kummer-type transformation for a F 2 2 hypergeometric function. J. Comput. Appl. Math. 173 (2), pp. 379–382.
  • G. Pólya (1949) Remarks on computing the probability integral in one and two dimensions. In Proceedings of the Berkeley Symposium on Mathematical Statistics and Probability, 1945, 1946, pp. 63–78.