Quire

Lommel function

From Quire, the open reference··1 min read
Image: source and license

In mathematics, the Lommel differential equation, named after Eugen von Lommel, is an inhomogeneous form of the Bessel differential equation

{\displaystyle z^{2}{\frac {d^{2}y}{dz^{2+z{\frac {dy}{dz+(z^{2}-\nu ^{2})y=z^{\mu +1}.}

Its solutions are given by the Lommel functions {\displaystyle s_{\mu ,\nu }(z)} and {\displaystyle S_{\mu ,\nu }(z)}:[1]

{\displaystyle s_{\mu ,\nu }(z)={\frac {\pi }{2\left(Y_{\nu }(z)\!\int _{0}^{z}\!\!x^{\mu }J_{\nu }(x)\,dx-J_{\nu }(z)\!\int _{0}^{z}\!\!x^{\mu }Y_{\nu }(x)\,dx\
{\displaystyle S_{\mu ,\nu }(z)=s_{\mu ,\nu }(z)+2^{\mu -1}\Gamma \left({\frac {\mu +\nu +1}{2\right)\Gamma \left({\frac {\mu -\nu +1}{2\right)\left(\sin \left[(\mu -\nu ){\frac {\pi }{2\right]

where {\displaystyle J_{\nu }(z)} is a Bessel function of the first kind and {\displaystyle Y_{\nu }(z)} a Bessel function of the second kind.

Image: source and license

The function {\displaystyle s_{\mu ,\nu can also be written as[2]

{\displaystyle s_{\mu ,\nu }(z)={\frac {z^{\mu +1{(\mu -\nu +1)(\mu +\nu +1){}_{1}F_{2}{\bigg (}1;{\frac {\mu }{2-{\frac {\nu }{2+{\frac {3}{2,{\frac {

where {\displaystyle {}_{1}F_{2 is a generalized hypergeometric function.

See also#edit

References#edit

  1. ^ Lommel (1880).
  2. ^ Watson (1922), p. 346, equation 10.

This article is mirrored from “Lommel function” on English Wikipedia, revision 1374410996, written by Wikipedia's contributors and licensed CC BY-SA 4.0. Editing it here creates a Quire copy with its own history.

Synced with Wikipedia revision 1374410996 · just now