We have developed new methods to quantify the data acquired by electro
n spectroscopic imaging (ESI) which are based on recording series of e
nergy filtered images across inner shell loss edges or in the low loss
region. From the series of ESI images, electron energy loss (EEL) spe
ctra can be extracted for any given image area, i.e. each individual p
ixel or an array of pixels over which the signal is integrated. The EE
L spectra can subsequently be analysed using standard EELS quantificat
ion techniques. This makes it possible to obtain a measure of the abso
lute amount (area density) of an element in the given sample area or o
f the concentration ratios of one element with respect to other elemen
ts. From a series of ESI images in the low-loss region, accurate value
s of the specimen thickness can be obtained, provided the mean free pa
th for inelastic scattering is known. As examples, results obtained on
Si2N2O ceramics and thin Al2O3 films, which were grown by anodical ox
idation, will be shown. The number densities of the atoms and concentr
ation ratios can be measured with an accuracy of 10-15% using calculat
ed inelastic scattering cross-sections. Similar accuracies can be obta
ined for the measurements of the specimen thickness, as will be shown
for the thin Al2O3 films and for a wedge shaped silicon crystal. In th
e case of Si, convergent beam electron diffraction was employed to det
ermine the mean free path for inelastic scattering. For the same sampl
e, the thickness of the carbon contamination layers and the amorphous
surface oxide layers were measured. The results of the latter measurem
ents may provide important information for the quantitative evaluation
of high resolution images or CBED patterns. (C) 1997 Elsevier Science
Ltd. All rights reserved.