Single dissolved nitrogen, boron or hydrogen atoms cause the diamond l
attice around them to expand by 40%, 33.7% and 31%, respectively. Such
large atomic strains generate short-range stresses around each dissol
ved impurity atom. If the impurity is dissolved uniformly in a diamond
crystal, the atomic strains around each impurity atom will produce an
overall uniform expansion that will not generate macro stresses in th
e diamond crystal. However, if the impurity is not dissolved uniformly
, incompatible macrostrains will result that will generate large elast
ic stresses in the diamond crystal. These stresses may strengthen or w
eaken a diamond crystal depending on their magnitudes, signs (i.e. com
pression or tension) and spatial distributions in the crystal. An inho
mogeneous distribution of impurities can be generated either by the ap
pearance of higher order growth facets during crystal growth, which ge
nerate differential segregation of impurities between the high- and lo
w-order crystal growth sectors or by temporal changes in growth condit
ions which generate radial impurity gradients. Since growth conditions
control the distribution of impurities in the diamond, diamonds can b
e strengthened or weakened by different growth conditions.