A. Charai et al., Structural change induced on an atomic scale by equilibrium sulphur segregation in tilt germanium grain boundaries, PHIL MAG B, 81(11), 2001, pp. 1821-1832
In the present study, structural modifications induced by equilibrium sulph
ur segregation in pure tilt germanium {710}< 001 >, Sigma = 25 (theta = 16.
26 degrees) and {551}< 011 >, Sigma = 51 (theta = 16.10 degrees) grain boun
daries (GBs) were investigated using high-resolution electron microscopy co
upled to electron-energy-loss spectroscopy and supported by structural mode
lling and image simulations. Our results showed that the as-grown Sigma = 2
5 GB is composed of two parts: a stable structural region and a variable pe
rturbed core. On the basis of our simulations, it is shown that this bounda
ry can only be formed by a multiplicity of configurations which are energet
ically close to each other but differently configured along the boundary pl
ane. When sulphurized, drastic changes in the structure of the GB were obse
rved. Energy-filtered electron microscopy imaging revealed a sulphur enrich
ment at the perturbed part of the boundary. Although sulphur segregation at
the boundary is detected, no information can at the present stage be extra
cted on segregation sites and bonding configurations because of the complex
ity of the boundary structure. To simplify this aspect, a simpler GB, that
is germanium Sigma = 51, was studied. The structure of such a GB is a well-
known configuration, that is a Lomer dislocation, which is basically a five
fold ring adjacent to a sevenfold ring. After sulphur treatment, high-resol
ution electron microscopy imaging also shows significant contrast modificat
ions apparently concentrated on the dislocation core. Chemical imaging indi
cates again the presence of sulphur enrichment along the boundary plane str
ongly sustaining that equilibrium sulphur segregation in the Ge(S) system o
ccurs into the GB and therefore confirms our previous results on the Sigma
= 25 GB. One can therefore argue that it is the presence of those odd-membe
red rings at the boundary, which should possess a specific crystallographic
and electronic nature, coupled to the electronic properties of sulphur, th
at are responsible for the preferential segregation into the boundary.