Lommel function

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

z2d2ydz2+zdydz+(z2ν2)y=zμ+1.

Solutions are given by the Lommel functions sμ,ν(z) and Sμ,ν(z), introduced by Template:Harvs,

sμ,ν(z)=π2[Yν(z)0zxμJν(x)dxJν(z)0zxμYν(x)dx],
Sμ,ν(z)=sμ,ν(z)+2μ1Γ(μ+ν+12)Γ(μν+12)(sin[(μν)π2]Jν(z)cos[(μν)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(μν+1)(μ+ν+1)1F2(1;μ2ν2+32,μ2+ν2+32;z24),

where pFq is a generalized hypergeometric function.

See also

References

Template:Reflist

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