Crystallographically orientated samples of synthetic optical-grade col
ourless quartz with high chemical purity and low dislocation density t
ogether with synthetic,oem-grade amethyst with high Fe-concentration a
nd ca. 250 H/10(6) Si (''dry'') or 600 H/10(6) Si (''wet'') and with v
ery high dislocation densities were irradiated using TEM. Samples of c
uts perpendicular ([c]-cuts) and parallel ([X]-cuts) to the c-axis, th
at were as-grown or pretreated for 5 days at 820 K on air or under p(H
2O) = 10(8) Pa were prepared. Characterization methods used include AA
S, FTIR, Raman-spectroscopy, X-ray-topography, REM, TEM in SAED and br
ight-field mode and polarized light microscopy. Radiolysis was carried
out in TEM from 10 to 300 K with 100 kV and from 70-850 K (low-high-t
ransition temperature of quartz) with 200 kV. Irradiation damage was i
nvestigated by decay of Kikuchi-lines or of Bragg-reflections in SAED
and in bright-field mode by development of strain contrast centres and
of noncrystalline volume areas. Special preparates where the irradiat
ion damage was of microscopic dimensions were investigated using Raman
-spectroscopy. Radiolysis of quartz is able to proceed at 10 K with me
asurable velocity. The required electron dose for a standardized irrad
iation damage decreases with increasing temperature. At ca. 500 K it g
oes through a minimum and then increases steadily up to ca. 700 K. Fro
m there the increase is steep until ca. 820 K where it culminates shar
ply, showing strong fluctuations until 850 K. The [X]-cuts in the as-g
rown state show significantly higher irradiation damage sensitivity th
an [E1]-cuts. Dry or hydrothermal preheating increases the overall sen
sitivity of irradiation damage and levels out the orientation differen
ces. The high Fe-concentrations in amethyst in comparison with very pu
re quartz have no detectable influence on the damage sensitivity. This
is also true for different water concentrations independently from th
e ratio of silanole-group to molecular water. Sample thinning by ion e
tching with different gun currents produces differences in irradiation
sensitivity. Thinning by crushing produces samples with sensitivities
comparable with ion-etching at low gun current.