The usage of Auger depth profiling technique in its conventional form
was limited considerably by surface roughening accompanying the ion sp
uttering. The depth resolution thus decreased with the thickness of th
e removed layer. Introducing rotation of the specimen and using glanci
ng-incidence-angle ions the surface roughening was greatly reduced. Ap
plying these conditions, one can study the ion mixing effect, which is
another limiting factor for the depth resolution. A Mo 3.6 - Si 3.3 n
m multilayer system deposited on a Si substrate has been studied by AE
S depth profiling with specimen rotation and glancing-incidence-angle
ions (87-degrees to the surface normal) in the 1-2 keV electron and 1-
5 keV ion energy ranges, using a special ion gun. Depth profiling was
followed by plasmon loss and elastic peak electron spectroscopy (EPES)
. EPES enables variation of the sampling depth, while the AES sampling
depth was approximately 0.4 nm. Plasmon loss spectra have been record
ed on the Mo and Si layers and are considerably different from those o
btained on pure Mo and Si, respectively. Simulation of the elastic pea
k intensity versus profiling depth resulted in good agreement with exp
erimental data. The calculation was based on a single elastic scatteri
ng approach and with Liau's ion mixing model.