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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→0
  4. §13.14(iv) Limiting Forms as z→∞
  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 d2Wdz2+(−14+κz+14−μ2z2)⁢W=0.

This equation is obtained from Kummer’s equation (13.2.1) via the substitutions W=e−12⁢z⁢z12+μ⁢w, κ=12⁢b−a, and μ=12⁢b−12. It has a regular singularity at the origin with indices 12±μ, and an irregular singularity at infinity of rank one.

Standard Solutions

Standard solutions are:

13.14.2 Mκ,μ⁡(z)=e−12⁢z⁢z12+μ⁢M⁡(12+μ−κ,1+2⁢μ,z),
13.14.3 Wκ,μ⁡(z)=e−12⁢z⁢z12+μ⁢U⁡(12+μ−κ,1+2⁢μ,z),

except that Mκ,μ⁡(z) does not exist when 2⁢μ=−1,−2,−3,….

The series

13.14.6 Mκ,μ⁡(z)=e−12⁢z⁢z12+μ⁢∑s=0∞(12+μ−κ)s(1+2⁢μ)s⁢s!⁢zs=z12+μ⁢∑n=0∞F12⁡(−n,12+μ−κ1+2⁢μ;2)⁢(−12⁢z)nn!,
2⁢μ≠−1,−2,−3,…,

converge for all z∈ℂ.

In general Mκ,μ⁡(z) and Wκ,μ⁡(z) are many-valued functions of z with branch points at z=0 and z=∞. The principal branches correspond to the principal branches of the functions z12+μ and U⁡(12+μ−κ,1+2⁢μ,z) on the right-hand sides of the equations (13.14.2) and (13.14.3); compare §4.2(i).

Although Mκ,μ⁡(z) does not exist when 2⁢μ=−1,−2,−3,…, many formulas containing Mκ,μ⁡(z) continue to apply in their limiting form. For example, if n=0,1,2,…, then

13.14.7 lim2⁢μ→−n−1Mκ,μ⁡(z)Γ⁡(2⁢μ+1)=(−12⁢n−κ)n+1(n+1)!⁢Mκ,12⁢(n+1)⁡(z)=e−12⁢z⁢z−12⁢n⁢∑s=n+1∞(−12⁢n−κ)sΓ⁡(s−n)⁢s!⁢zs.

If 2⁢μ=±n, where n=0,1,2,…, then

13.14.8 Wκ,±12⁢n⁡(z)=(−1)n⁢e−12⁢z⁢z12⁢n+12n!⁢Γ⁡(12−12⁢n−κ)⁢(∑k=1nn!⁢(k−1)!(n−k)!⁢(κ+12−12⁢n)k⁢z−k−∑k=0∞(12⁢n+12−κ)k(n+1)k⁢k!⁢zk⁢(ln⁡z+ψ⁡(12⁢n+12−κ+k)−ψ⁡(1+k)−ψ⁡(n+1+k))),
κ−12⁢n−12≠0,1,2,…,

or

13.14.9 Wκ,±12⁢n⁡(z)=(−1)κ−12⁢n−12⁢e−12⁢z⁢z12⁢n+12×∑k=0κ−12⁢n−12(κ−12⁢n−12k)⁢(n+1+k)κ−k−12⁢n−12⁢(−z)k,
κ−12⁢n−12=0,1,2,….

§13.14(ii) Analytic Continuation

In (13.14.11)–(13.14.13) m is any integer.

13.14.11 Mκ,μ⁡(z⁢e2⁢m⁢π⁢i)=(−1)m⁢e2⁢m⁢μ⁢π⁢i⁢Mκ,μ⁡(z).
13.14.12 Wκ,μ⁡(z⁢e2⁢m⁢π⁢i)=(−1)m+1⁢2⁢π⁢i⁢sin⁡(2⁢π⁢μ⁢m)Γ⁡(12−μ−κ)⁢Γ⁡(1+2⁢μ)⁢sin⁡(2⁢π⁢μ)⁢Mκ,μ⁡(z)+(−1)m⁢e−2⁢m⁢μ⁢π⁢i⁢Wκ,μ⁡(z).
13.14.13 (−1)m⁢Wκ,μ⁡(z⁢e2⁢m⁢π⁢i)=−e2⁢κ⁢π⁢i⁢sin⁡(2⁢m⁢μ⁢π)+sin⁡((2⁢m−2)⁢μ⁢π)sin⁡(2⁢μ⁢π)⁢Wκ,μ⁡(z)−sin⁡(2⁢m⁢μ⁢π)⁢2⁢π⁢i⁢eκ⁢π⁢isin⁡(2⁢μ⁢π)⁢Γ⁡(12+μ−κ)⁢Γ⁡(12−μ−κ)⁢W−κ,μ⁡(z⁢eπ⁢i).

Except when z=0, each branch of the functions Mκ,μ⁡(z)/Γ⁡(2⁢μ+1) and Wκ,μ⁡(z) is entire in κ and μ. Also, unless specified otherwise Mκ,μ⁡(z) and Wκ,μ⁡(z) are assumed to have their principal values.

§13.14(iii) Limiting Forms as z→0

13.14.14 Mκ,μ⁡(z)=zμ+12⁢(1+O⁡(z)),
2⁢μ≠−1,−2,−3,….

In cases when 12−κ±μ=−n, where n is a nonnegative integer,

13.14.15 W12±μ+n,μ⁡(z)=(−1)n⁢(1±2⁢μ)n⁢z12±μ+O⁡(z32±μ).

In all other cases

13.14.16 Wκ,μ⁡(z)=Γ⁡(2⁢μ)Γ⁡(12+μ−κ)⁢z12−μ+O⁡(z32−ℜ⁡μ),
ℜ⁡μ≥12, μ≠12,
13.14.18 Wκ,μ⁡(z)=Γ⁡(2⁢μ)Γ⁡(12+μ−κ)⁢z12−μ+Γ⁡(−2⁢μ)Γ⁡(12−μ−κ)⁢z12+μ+O⁡(z32−ℜ⁡μ),
0≤ℜ⁡μ<12, μ≠0,

For Wκ,μ⁡(z) with ℜ⁡μ<0 use (13.14.31).

§13.14(iv) Limiting Forms as z→∞

Except when μ−κ=−12,−32,… (polynomial cases),

where δ is an arbitrary small positive constant. Also,

§13.14(v) Numerically Satisfactory Solutions

Fundamental pairs of solutions of (13.14.1) that are numerically satisfactory (§2.7(iv)) in the neighborhood of infinity are

13.14.22 Wκ,μ⁡(z),
W−κ,μ⁡(e−π⁢i⁢z),
−12⁢π≤ph⁡z≤32⁢π,
13.14.23 Wκ,μ⁡(z),
W−κ,μ⁡(eπ⁢i⁢z),
−32⁢π≤ph⁡z≤12⁢π.

A fundamental pair of solutions that is numerically satisfactory in the sector |ph⁡z|≤π near the origin is

13.14.24 Mκ,μ⁡(z),
Mκ,−μ⁡(z),
2⁢μ∉ℤ.

When 2⁢μ is an integer we may use the results of §13.2(v) with the substitutions b=2⁢μ+1, a=μ−κ+12, and W=e−12⁢z⁢z12+μ⁢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 𝒲⁡{Mκ,μ⁡(z),Mκ,−μ⁡(z)}=−2⁢μ,
13.14.26 𝒲⁡{Mκ,μ⁡(z),Wκ,μ⁡(z)}=−Γ⁡(1+2⁢μ)Γ⁡(12+μ−κ),
13.14.28 𝒲⁡{Mκ,−μ⁡(z),Wκ,μ⁡(z)}=−Γ⁡(1−2⁢μ)Γ⁡(12−μ−κ),

§13.14(vii) Connection Formulas

13.14.31 Wκ,μ⁡(z)=Wκ,−μ⁡(z).
13.14.32 1Γ⁡(1+2⁢μ)⁢Mκ,μ⁡(z)=e±(κ−μ−12)⁢π⁢iΓ⁡(12+μ+κ)⁢Wκ,μ⁡(z)+e±κ⁢π⁢iΓ⁡(12+μ−κ)⁢W−κ,μ⁡(e±π⁢i⁢z).

When 2⁢μ is not an integer

13.14.33 Wκ,μ⁡(z)=Γ⁡(−2⁢μ)Γ⁡(12−μ−κ)⁢Mκ,μ⁡(z)+Γ⁡(2⁢μ)Γ⁡(12+μ−κ)⁢Mκ,−μ⁡(z).
13.14.34 2⁢πΓ⁡(1+2⁢μ)⁢Γ⁡(12−μ−κ)⁢M−κ,μ⁡(z)=eμ⁢π⁢i⁢Wκ,μ⁡(eπ⁢i⁢z)+e−μ⁢π⁢i⁢Wκ,μ⁡(e−π⁢i⁢z),
13.14.35 2⁢π⁢iΓ⁡(12+μ−κ)⁢Γ⁡(12−μ−κ)⁢W−κ,μ⁡(z)=e−κ⁢π⁢i⁢Wκ,μ⁡(eπ⁢i⁢z)−eκ⁢π⁢i⁢Wκ,μ⁡(e−π⁢i⁢z).