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confluent Heun equation

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11: Bibliography S
  • S. Yu. Slavyanov and N. A. Veshev (1997) Structure of avoided crossings for eigenvalues related to equations of Heun’s class. J. Phys. A 30 (2), pp. 673–687.
  • B. D. Sleeman (1966a) Some Boundary Value Problems Associated with the Heun Equation. Ph.D. Thesis, London University.
  • B. D. Sleeman (1969) Non-linear integral equations for Heun functions. Proc. Edinburgh Math. Soc. (2) 16, pp. 281–289.
  • A. O. Smirnov (2002) Elliptic Solitons and Heun’s Equation. In The Kowalevski Property (Leeds, UK, 2000), V. B. Kuznetsov (Ed.), CRM Proc. Lecture Notes, Vol. 32, pp. 287–306.
  • H. Suzuki, E. Takasugi, and H. Umetsu (1998) Perturbations of Kerr-de Sitter black holes and Heun’s equations. Progr. Theoret. Phys. 100 (3), pp. 491–505.
  • 12: Errata
  • Equations (31.3.10), (31.3.11)
    31.3.10 z α H ( 1 a , q a α ( β ϵ ) α a ( β δ ) ; α , α γ + 1 , α β + 1 , δ ; 1 z )
    31.3.11 z β H ( 1 a , q a β ( α ϵ ) β a ( α δ ) ; β , β γ + 1 , β α + 1 , δ ; 1 z )

    In both equations, the second entry in the H has been corrected with an extra minus sign.

  • Equations (13.2.9), (13.2.10)

    There were clarifications made in the conditions on the parameter a in U ( a , b , z ) of those equations.

  • 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 (13.18.7)
    13.18.7 W 1 4 , ± 1 4 ( z 2 ) = e 1 2 z 2 π z erfc ( z )

    Originally the left-hand side was given correctly as W 1 4 , 1 4 ( z 2 ) ; the equation is true also for W 1 4 , + 1 4 ( z 2 ) .

  • 13: 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 (2013) Exponentially small expansions of the confluent hypergeometric functions. Appl. Math. Sci. (Ruse) 7 (133-136), pp. 6601–6609.
  • J. Patera and P. Winternitz (1973) A new basis for the representation of the rotation group. Lamé and Heun polynomials. J. Mathematical Phys. 14 (8), pp. 1130–1139.