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31: Software Index
Open Source With Book Commercial
13 Confluent Hypergeometric Functions
13.32(ii) M ( a , b , x ) , U ( a , b , x ) , 𝐌 ( a , b , x ) , M κ , μ ( x ) , W κ , μ ( x ) , x , a , b a
13.32(iii) M ( a , b , z ) , U ( a , b , z ) , 𝐌 ( a , b , z ) , M κ , μ ( z ) , W κ , μ ( z ) , z , a , b a
  • Open Source Collections and Systems.

    These are collections of software (e.g. libraries) or interactive systems of a somewhat broad scope. Contents may be adapted from research software or may be contributed by project participants who donate their services to the project. The software is made freely available to the public, typically in source code form. While formal support of the collection may not be provided by its developers, within active projects there is often a core group who donate time to consider bug reports and make updates to the collection.

  • 32: 18.39 Applications in the Physical Sciences
    The fundamental quantum Schrödinger operator, also called the Hamiltonian, , is a second order differential operator of the formBelow we consider two potentials with analytically known eigenfunctions and eigenvalues where the spectrum is entirely point, or discrete, with all eigenfunctions being L 2 and forming a complete set. … The solutions (18.39.8) are called the stationary states as separation of variables in (18.39.9) yields solutions of formThe orthonormal stationary states and corresponding eigenvalues are then of the formThese, taken together with the infinite sets of bound states for each l , form complete sets. …
    33: 8.19 Generalized Exponential Integral
    The right-hand sides are replaced by their limiting forms when p = 1 , 2 , 3 , . …
    §8.19(vi) Relation to Confluent Hypergeometric Function
    For U ( a , b , z ) see §13.2(i). …
    34: 32.10 Special Function Solutions
    All solutions of P II P VI  that are expressible in terms of special functions satisfy a first-order equation of the form
    32.10.27 ϕ ( z ) = C 1 M κ , μ ( ζ ) + C 2 W κ , μ ( ζ ) ζ ( a b + 1 ) / 2 exp ( 1 2 ζ ) ,
    The solution (32.10.34) is an essentially transcendental function of both constants of integration since P VI  with α = β = γ = 0 and δ = 1 2 does not admit an algebraic first integral of the form P ( z , w , w , C ) = 0 , with C a constant. …
    35: Bibliography S
  • A. Sharples (1967) Uniform asymptotic forms of modified Mathieu functions. Quart. J. Mech. Appl. Math. 20 (3), pp. 365–380.
  • G. Shimura (1982) Confluent hypergeometric functions on tube domains. Math. Ann. 260 (3), pp. 269–302.
  • H. Skovgaard (1966) Uniform Asymptotic Expansions of Confluent Hypergeometric Functions and Whittaker Functions. Doctoral dissertation, University of Copenhagen, Vol. 1965, Jul. Gjellerups Forlag, Copenhagen.
  • L. J. Slater (1960) Confluent Hypergeometric Functions. Cambridge University Press, Cambridge-New York.
  • A. D. Smirnov (1960) Tables of Airy Functions and Special Confluent Hypergeometric Functions. Pergamon Press, New York.
  • 36: 9.6 Relations to Other Functions
    §9.6(iii) Airy Functions as Confluent Hypergeometric Functions
    9.6.21 Ai ( z ) = 1 2 π 1 / 2 z 1 / 4 W 0 , 1 / 3 ( 2 ζ ) = 3 1 / 6 π 1 / 2 ζ 2 / 3 e ζ U ( 5 6 , 5 3 , 2 ζ ) ,
    9.6.22 Ai ( z ) = 1 2 π 1 / 2 z 1 / 4 W 0 , 2 / 3 ( 2 ζ ) = 3 1 / 6 π 1 / 2 ζ 4 / 3 e ζ U ( 7 6 , 7 3 , 2 ζ ) ,
    9.6.23 Bi ( z ) = 1 2 1 / 3 Γ ( 2 3 ) z 1 / 4 M 0 , 1 / 3 ( 2 ζ ) + 3 2 5 / 3 Γ ( 1 3 ) z 1 / 4 M 0 , 1 / 3 ( 2 ζ ) ,
    9.6.24 Bi ( z ) = 2 1 / 3 Γ ( 1 3 ) z 1 / 4 M 0 , 2 / 3 ( 2 ζ ) + 3 2 10 / 3 Γ ( 2 3 ) z 1 / 4 M 0 , 2 / 3 ( 2 ζ ) ,
    37: 7.18 Repeated Integrals of the Complementary Error Function
    7.18.2 i n erfc ( z ) = z i n 1 erfc ( t ) d t = 2 π z ( t z ) n n ! e t 2 d t .
    Confluent Hypergeometric Functions
    7.18.9 i n erfc ( z ) = e z 2 ( 1 2 n Γ ( 1 2 n + 1 ) M ( 1 2 n + 1 2 , 1 2 , z 2 ) z 2 n 1 Γ ( 1 2 n + 1 2 ) M ( 1 2 n + 1 , 3 2 , z 2 ) ) ,
    The confluent hypergeometric function on the right-hand side of (7.18.10) is multivalued and in the sectors 1 2 π < | ph z | < π one has to use the analytic continuation formula (13.2.12). …
    38: Errata
    The spectral theory of these operators, based on Sturm-Liouville and Liouville normal forms, distribution theory, is now discussed more completely, including linear algebra, matrices, matrices as linear operators, orthonormal expansions, Stieltjes integrals/measures, generating functions. …
  • Paragraph Confluent Hypergeometric Functions (in §7.18(iv))

    A note about the multivalued nature of the Kummer confluent hypergeometric function of the second kind U on the right-hand side of (7.18.10) was inserted.

  • Paragraph Confluent Hypergeometric Functions (in §10.16)

    Confluent hypergeometric functions were incorrectly linked to the definitions of the Kummer confluent hypergeometric and parabolic cylinder functions. However, to the eye, the functions appeared correct. The links were corrected.

  • 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.

  • Subsection 13.29(v)

    A new Subsection Continued Fractions, has been added to cover computation of confluent hypergeometric functions by continued fractions.

  • 39: Bibliography B
  • H. Buchholz (1969) The Confluent Hypergeometric Function with Special Emphasis on Its Applications. Springer-Verlag, New York.
  • W. Bühring (1994) The double confluent Heun equation: Characteristic exponent and connection formulae. Methods Appl. Anal. 1 (3), pp. 348–370.
  • W. S. Burnside and A. W. Panton (1960) The Theory of Equations: With an Introduction to the Theory of Binary Algebraic Forms. Dover Publications, New York.
  • 40: Bibliography O
  • F. W. J. Olver (1991b) Uniform, exponentially improved, asymptotic expansions for the confluent hypergeometric function and other integral transforms. SIAM J. Math. Anal. 22 (5), pp. 1475–1489.
  • F. W. J. Olver (1993a) Exponentially-improved asymptotic solutions of ordinary differential equations I: The confluent hypergeometric function. SIAM J. Math. Anal. 24 (3), pp. 756–767.
  • M. K. Ong (1986) A closed form solution of the s -wave Bethe-Goldstone equation with an infinite repulsive core. J. Math. Phys. 27 (4), pp. 1154–1158.