Lommel function

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thumb In mathematics, 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.

Its solutions are given by the Lommel functions sμ,ν(z) and Sμ,ν(z):[1]

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.

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The function sμ,ν can also be written as[2]

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

where 1F2 is a generalized hypergeometric function.

See also

References

  1. ↑ Lommel (1880).
  2. ↑ Watson (1922), p. 346, equation 10.
  • Erdélyi, Arthur; Magnus, Wilhelm; Oberhettinger, Fritz; Tricomi, Francesco G. (1953). Higher Transcendental Functions. I, II. New York: McGraw-Hill. 
  • Treatise on the Theory of Bessel Functions. Cambridge University Press. 1922.