Abstract
The calculation of cross sections for the collision of electrons with molecular targets presents a considerably more difficult challenge than the corresponding problem for atomic systems. First, the non-spherically symmetric character of the electron-molecule interaction potential makes many of the numerical methods used for electron-atom scattering extremely difficult to apply and second, the nuclear motion introduces additional (ro-vibrational) degrees of freedom which can increase the number of channels far beyond the capabilities of even the most sophisticated computer.
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