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13 Confluent Hypergeometric FunctionsWhittaker Functions

§13.14 Definitions and Basic Properties

Contents
  1. §13.14(i) Differential Equation
  2. §13.14(ii) Analytic Continuation
  3. §13.14(iii) Limiting Forms as z\to 0
  4. §13.14(iv) Limiting Forms as z\to\infty
  5. §13.14(v) Numerically Satisfactory Solutions
  6. §13.14(vi) Wronskians
  7. §13.14(vii) Connection Formulas

§13.14(i) Differential Equation

Whittaker’s Equation

13.14.1 \frac{{\mathrm{d}}^{2}W}{{\mathrm{d}z}^{2}}+\left(-\frac{1}{4}+\frac{\kappa}{z%
}+\frac{\frac{1}{4}-\mu^{2}}{z^{2}}\right)W=0.

This equation is obtained from Kummer’s equation (13.2.1) via the substitutions W=e^{-\frac{1}{2}z}z^{\frac{1}{2}+\mu}w, \kappa=\tfrac{1}{2}b-a, and \mu=\tfrac{1}{2}b-\tfrac{1}{2}. It has a regular singularity at the origin with indices \tfrac{1}{2}\pm\mu, and an irregular singularity at infinity of rank one.

Standard Solutions

Standard solutions are:

13.14.2 M_{\kappa,\mu}\left(z\right)=e^{-\frac{1}{2}z}z^{\frac{1}{2}+\mu}M\left(\tfrac%
{1}{2}+\mu-\kappa,1+2\mu,z\right),
13.14.3 W_{\kappa,\mu}\left(z\right)=e^{-\frac{1}{2}z}z^{\frac{1}{2}+\mu}U\left(\tfrac%
{1}{2}+\mu-\kappa,1+2\mu,z\right),

except that M_{\kappa,\mu}\left(z\right) does not exist when 2\mu=-1,-2,-3,\dots.

In general M_{\kappa,\mu}\left(z\right) and W_{\kappa,\mu}\left(z\right) are many-valued functions of z with branch points at z=0 and z=\infty. The principal branches correspond to the principal branches of the functions z^{\frac{1}{2}+\mu} and U\left(\tfrac{1}{2}+\mu-\kappa,1+2\mu,z\right) on the right-hand sides of the equations (13.14.2) and (13.14.3); compare §4.2(i).

Although M_{\kappa,\mu}\left(z\right) does not exist when 2\mu=-1,-2,-3,\dots, many formulas containing M_{\kappa,\mu}\left(z\right) continue to apply in their limiting form. For example, if n=0,1,2,\dots, then

If 2\mu=\pm n, where n=0,1,2,\dots, then

§13.14(ii) Analytic Continuation

Except when z=0, each branch of the functions \ifrac{M_{\kappa,\mu}\left(z\right)}{\Gamma\left(2\mu+1\right)} and W_{\kappa,\mu}\left(z\right) is entire in \kappa and \mu. Also, unless specified otherwise M_{\kappa,\mu}\left(z\right) and W_{\kappa,\mu}\left(z\right) are assumed to have their principal values.

§13.14(iii) Limiting Forms as z\to 0

In cases when \frac{1}{2}-\kappa\pm\mu=-n, where n is a nonnegative integer,

In all other cases

For W_{\kappa,\mu}\left(z\right) with \Re\mu<0 use (13.14.31).

§13.14(v) Numerically Satisfactory Solutions

A fundamental pair of solutions that is numerically satisfactory in the sector |\operatorname{ph}{z}|\leq\pi near the origin is

When 2\mu is an integer we may use the results of §13.2(v) with the substitutions b=2\mu+1, a=\mu-\kappa+\tfrac{1}{2}, and W=e^{-\frac{1}{2}z}z^{\frac{1}{2}+\mu}w, where W is the solution of (13.14.1) corresponding to the solution w of (13.2.1).

§13.14(vi) Wronskians

13.14.25 \mathscr{W}\left\{M_{\kappa,\mu}\left(z\right),M_{\kappa,-\mu}\left(z\right)%
\right\}=-2\mu,

§13.14(vii) Connection Formulas

13.14.35 \frac{2\pi\mathrm{i}}{\Gamma\left(\frac{1}{2}+\mu-\kappa\right)\Gamma\left(%
\frac{1}{2}-\mu-\kappa\right)}W_{-\kappa,\mu}\left(z\right)={\mathrm{e}}^{-%
\kappa\pi\mathrm{i}}W_{\kappa,\mu}\left({\mathrm{e}}^{\pi\mathrm{i}}z\right)-{%
\mathrm{e}}^{\kappa\pi\mathrm{i}}W_{\kappa,\mu}\left({\mathrm{e}}^{-\pi\mathrm%
{i}}z\right).