Abstract
We return to the Cauchy integral equations encountered in transfer problems when formulated in plane-parallel media. Light scattering is assumed isotropic for simplicity. The analytical properties of the classical N-function are reviewed. This function is sectionally analytic in the complex plane cut along the segment [0, 1]. Its domain is extended to the whole complex plane, except at +1 where it diverges. We write down the functional relations satisfied by N outside [0, 1] and extend them on the cut with the help of Plemelj's formulae. This article is an introduction to a revisited derivation of the functions H and X, Y of plane-parallel media from the singular integral equations they satisfy.

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