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Energy of Auger Peaks

The energy of an Auger transition, for example KLM, is to a first approximation given by  [Pg.76]

Ek is the binding energy of an electron in the K-shell, etc. rp is the work function  [Pg.76]

The SE term accounts for the relaxation effects involved in the decay process, which leads to a final state consisting of a heavily excited, doubly ionized atom. [Pg.76]

Auger energies are as element-specific as binding energies in XPS. However, chemical information such as oxidation states is much more difficult to abstract. [Pg.76]

In general, XPS is the preferred technique for studying oxidation states and ligand effects. However, there is a good reason why one should be interested in deriving chemical information from AES. Whereas the spatial resolution of XPS is at best a few micrometers, Auger spectra can be obtained from spots with diameters as small as a few nanometers. It would be extremely interesting to have oxidation state information on the same scale as well  [Pg.77]


See other pages where Energy of Auger Peaks is mentioned: [Pg.84]    [Pg.69]    [Pg.75]   


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