There are several functions called "Lommel functions." One type of Lommel function appear in the solution to the Lommel differential equation and are given by
(1)
(2)
(3)
where and are generalized and confluence hypergeometric functions, respectively and is typically denoted just as .
The function defined by Gradshteyn and Ryzhik (2000, p. 936) is identical to .
The Lommel functions and will be implemented in a future version of the Wolfram Language as LommelS1[m, n, z] and LommelS2[m, n, z], respectively.
Lommel functions of two variables are related to the Bessel function of the first kind and arise in the theory of diffraction (Chandrasekhar 1960, p. 369) and, in particular, Mie scattering (Watson 1966, p. 537),
(6)
(7)
These functions were first defined by Lommel (1884-1886ab). Note that the definition (7) of differs by a factor of from the modern convention (Watson 1966, p. 537) and from the definition of Born and Wolf (1989, p. 438).
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