G. Kowalski et al., SYNCHROTRON X-RAY STUDIES OF STRAIN IN (100)-ORIENTED HIGH-PRESSURE HIGH-TEMPERATURE (HP-HT) SYNTHETIC DIAMONDS, DIAMOND AND RELATED MATERIALS, 5(11), 1996, pp. 1254-1263
The wavelength tunability and high intensity of a dedicated synchrotro
n X-ray source were extensively used in four-azimuth double-crystal di
ffraction experiments to study synthetic diamonds with (001) polished
faces. These had major growth sectors of {001} and {111} type and some
minor sectors of {110} and {113}. Many series of topographs (up to 80
per sample) in symmetric Bragg reflection geometry mere recorded. Som
e of the common features frequently present in synthetic diamonds, nam
ely metallic cylindrical inclusions as well as the growth sectors and
growth sector boundaries, were the subject of this study. The presence
of any source of strain in the crystal map seriously affect its perfo
rmance in applications: mechanical (tools), optical (IR windows) or el
ectronic (radiation detectors). X-Ray ''pinhole'' rocking curve measur
ements as well as detailed analysis of the topographic records yielded
interesting new results concerning the state Of the lattice in close
proximity to each inclusion and inside growth sectors of the minor for
ms of {113} and {110} type. The axisymmetric strain field caused by th
e embedded body of each cylindrical caused by the embedded body of eac
h cylindrical inclusion was recorded as a symmetrically compressed lat
tice. The lattice parameter of the I smaller (by 7 ppm) than that of t
he surrounding major growth sectors. More importantly, it Is recorded
and reported here for the first time that in addition to lattice param
eter differences there exists significant lattice bending (radius R =
7.5 m) inside the minor sectors that is created by the compressive act
ion of the surrounding major {001} and {111} growth sectors. Previous
experiments have been unable to record this component of stress in syn
thetic diamonds either because of an inappropriate choice of diffracti
on geometry or because of incompleteness of the experimental procedure
s.