Lommel function

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thumb thumb The Lommel differential equation, named after Eugen von Lommel, is an inhomogeneous form of the Bessel differential equation:

z2d2ydz2+zdydz+(z2−ν2)y=zμ+1.

Solutions are given by the Lommel functions sμ,ν(z) and Sμ,ν(z), introduced by Eugen von Lommel (1880),

sμ,ν(z)=π2[Yν(z)∫0zxμJν(x)dx−Jν(z)∫0zxμYν(x)dx],
Sμ,ν(z)=sμ,ν(z)+2μ−1Γ(μ+ν+12)Γ(μ−ν+12)(sin⁡[(μ−ν)π2]Jν(z)−cos⁡[(μ−ν)π2]Yν(z)),

where Jν(z) is a Bessel function of the first kind and Yν(z) a Bessel function of the second kind.

The s function can also be written as[1]

sμ,ν(z)=zμ+1(μ−ν+1)(μ+ν+1)1F2(1;μ2−ν2+32,μ2+ν2+32;−z24),

where pFq is a generalized hypergeometric function.

See also

References

  1. ↑ Watson's "Treatise on the Theory of Bessel functions" (1966), Section 10.7, Equation (10)