This letter concentrates on a quantitative description of surface roughness effects on Auger peak-line profiles for pure and alloyed specimens. The nanometer lateral electron probe size of the order of 10 nm yielded peak-line profiles that capture surface topology variations down to nanometer-length scales. Surface roughness leads to peak-intensity fluctuations, which are described within the weak roughness limit by a simple form, I(r)≈Iav[1+βh(r)]. Iav is the average peak intensity, h(r) represents the roughness fluctuation along a lateral in-planar distance r, and β is a constant (<1). In addition, analyses of the peak-difference correlation function Iz(r)=〈|I(r)−I(0)|2〉1/2 showed a power-law behavior Iz(r)∝rα with α ranging between 0.7 and 1 at small-length scales, i.e., for r≪ξ, with ξ a peak correlation length that was comparable to average specimen cluster sizes.
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Agterveld et al. (1999) studied this question.
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