REFLECTION HIGH-ENERGY ELECTRON-DIFFRACTION SCANNING-TUNNELING-MICROSCOPY STUDY OF INAS GROWTH ON THE 3 LOW-INDEX ORIENTATIONS OF GAAS - 2-DIMENSIONAL VERSUS 3-DIMENSIONAL GROWTH AND STRAIN RELAXATION
Ba. Joyce et al., REFLECTION HIGH-ENERGY ELECTRON-DIFFRACTION SCANNING-TUNNELING-MICROSCOPY STUDY OF INAS GROWTH ON THE 3 LOW-INDEX ORIENTATIONS OF GAAS - 2-DIMENSIONAL VERSUS 3-DIMENSIONAL GROWTH AND STRAIN RELAXATION, Journal of vacuum science & technology. B, Microelectronics and nanometer structures processing, measurement and phenomena, 16(4), 1998, pp. 2373-2380
It is generally believed that strain relaxation in semiconductor heter
ostructures having a significant misfit (>2%) occurs by the formation
of coherent three-dimensional islands, following the growth of one or
two continuous two-dimensional monolayers in a manifestation of the St
ranski-Krastanov (SK) growth mode. For the InAs-GaAs system, for which
the misfit is approximate to 7.2%, we have shown that this is a very
special case, at least during growth by molecular beam epitaxy, as it
occurs on only one of the low index orientations, the (001), and then
only under As-rich growth conditions. On,(110) and (111) surfaces, gro
wth is always two-dimensional layer by layer and strain is relieved by
the formation of misfit dislocations. Even when three-dimensional isl
ands are formed on (001) substrates, the process is much more complex
than the conventional SK mechanism would imply. We have used a combina
tion of in situ reflection high-energy electron diffraction (RHEED) an
d scanning tunneling microscopy (STM) and ex situ transmission electro
n microscopy to follow the initial growth processes and strain relaxat
ion mechanisms of InAs on GaAs (001), (110), and (111)A surfaces. RHEE
D enables us to establish the symmetry of the wetting layer, whether g
rowth is two- or three-dimensional and the external crystallography of
any three-dimensional islands. STM images obtained by rapid quenching
from the growth temperature show how growth is initiated, provide qua
ntitative data cin island formation (number density and volume), and i
ndicate dislocation formation via strain field morphology effects. Det
ailed results for all three low index surfaces are presented, together
with possible reasons for the major differences between them. (C) 199
8 American Vacuum Society.