Abstract

A quantitative comparison between an experimental and a theoretical description of any Auger spectrum requires a common energy reference point such as the Fermi level. With non-conductors this is problematic, because the Fermi level is not well defined and charging may shift the Fermi level. A common approach used to overcome this problem employs spectra containing the Auger peak, core, and valence band (VB) photoemission peaks. It is then necessary only to locate a common reference point in the Auger and VB spectra relative to the core level peak. We have developed a procedure in which a comparison is made between model theoretical and experimental spectra so that a large energy range (about 20 eV) of each spectrum can be utilized to locate the common reference points. We have found that this method enables accurate reference points to be determined even with severe sample charging. The method is precise enough to observe a differential charging effect in the polyethylene (PE) spectra. Although much smaller than that previously reported, a breakdown in the Cini-Sawatzky expression as modified for covalent systems still is suggested for PE. This breakdown can now be attributed to the limited one-dimensional delocalization required in long chain polymers.

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