Whittaker function explained

In mathematics, a Whittaker function is a special solution of Whittaker's equation, a modified form of the confluent hypergeometric equation introduced by to make the formulas involving the solutions more symmetric. More generally, introduced Whittaker functions of reductive groups over local fields, where the functions studied by Whittaker are essentially the case where the local field is the real numbers and the group is SL2(R).

Whittaker's equation is

d2w+\left(-
dz2
1+
4
\kappa+
z
1/4-\mu2
z2

\right)w=0.

It has a regular singular point at 0 and an irregular singular point at ∞. Two solutions are given by the Whittaker functions Mκ,μ(z), Wκ,μ(z), defined in terms of Kummer's confluent hypergeometric functions M and U by

M\kappa,\mu\left(z\right)=\exp\left(-z/2\right)z\mu+\tfrac{1{2}}M\left(\mu-\kappa+\tfrac{1}{2},1+2\mu,z\right)

W\kappa,\mu\left(z\right)=\exp\left(-z/2\right)z\mu+\tfrac{1{2}}U\left(\mu-\kappa+\tfrac{1}{2},1+2\mu,z\right).

The Whittaker function

W\kappa,\mu(z)

is the same as those with opposite values of, in other words considered as a function of at fixed and it is even functions. When and are real, the functions give real values for real and imaginary values of . These functions of play a role in so-called Kummer spaces.[1]

Whittaker functions appear as coefficients of certain representations of the group SL2(R), called Whittaker models.

References

Further reading

Notes and References

  1. Book: Hilbert spaces of entire functions. registration. Prentice-Hall. Louis de Branges. Louis de Branges. B0006BUXNM. 1968. Sections 55-57.

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