A reduced version of the independent-electron theory of Auger line shapes is given that takes advantage of the general smallness of those components of a solid's local density of states (LDOS) matrix which are off-diagonal in angular momentum. Thus we present approximate formulae which relate the valence-band Auger line shapes of a soslid simply to its angular-momentum projected LDOS near a surface. Using these simplified formulae, we have located and corrected a number of numerical errors in our previous calculations of the Auger line shapes of Si. We present corrected results here, showing that the independent-electron theory, coupled with the use of atomic Auger matrix elements for Si, actually predicts too large a probability of L2,3M₁M2,3 decay relative to that for L2,3M2,3M2,3 decay to give good agreement with measured Si L2,3VV Auger line shapes. Possible reasons for the experimental smallness of the L2,3M₁M2,3 Auger decay rate are discussed. The Si L₁L2,3V Coster-Kronig line is also recalculated and shown to be in correspondence with the simplified theory of Auger transitions.
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Feibelman et al. (1978) studied this question.
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