Ga. Cooke et al., USE OF MAXIMUM-ENTROPY DECONVOLUTION FOR THE STUDY OF SILICON DELTA-LAYERS IN GAAS, Journal of vacuum science & technology. B, Microelectronics and nanometer structures processing, measurement and phenomena, 14(1), 1996, pp. 132-135
Semiconductor layer structures with sharply changing concentration, an
d more especially delta-doped (single atomic plane) structures, provid
e an ideal environment for the study of the more subtle mass transport
phenomena such as concentration-dependent diffusion and localized mix
ing caused by ion bombardment. However, to be able to extract meaningf
ul parameters from such experiments, accurate depth profiles must be o
btained with extremely high depth resolution and good sensitivity. Sec
ondary ion mass spectrometry (SIMS) provides one of. the most sensitiv
e methods for acquiring such profiles. To obtain high depth resolution
, a number of criteria must be satisfied, not the least of which is th
e reduction of redistribution by the probe; thus it is essential to em
ploy a low energy primary beam. It is also vital that the crater floor
recedes parallel to the original surface of the specimen. This necess
itates accurate scanning of a stable ion beam, so as to ensure a const
ant flux across the entire sampled area. If this is not the case, dept
h resolution will degrade as a function of depth, and important inform
ation will be lost. However, even if probes of the order of 1-2 keV ar
e used, together with a precision scan system, beam-induced redistribu
tion is still a significant limit to the sharpness of the recorded pro
files. To further improve upon the data, the effects of the analysis m
ust be removed from the profile. In this article we demonstrate the us
e of the maximum entropy deconvolution technique, applying it to a SIM
S depth profile of a multilayer silicon in gallium arsenide structure
containing alternating layers of high and low areal density. The impor
tant issue of data validity is discussed and the deconvolved results a
re used to calculate a diffusion constant for the denser layers, the l
ess dense layers show no diffusion at the growth temperature of 450 de
grees C. (C) 1996 American Vacuum Society.