I present here a general formalism that allows the construction of the cros
s section of any electron spectroscopy in a straightforward and transparent
way. This approach does not make any assumption concerning the choice of t
he basis functions used to expand the wave function of the electron. In thi
s sense, it generalizes existing theories. It allows us to keep the physics
well in view and offers, due to the relationship between operators and par
ts of a pictorial representation of the experiments, a type of a graphical
interface to the problem at hand. Moreover, it does not assume any particul
ar shape for the potential.