The dose distribution in water from Ge-71 K-shell x-rays (E-ave = 9.44
keV) was calculated for various source configurations using both anal
ytic and EGS4 Monte Carlo calculations. The point source kernel and th
e buildup factor are presented. The buildup factor for a point source
in water has been found to increase up to about 1.1 as radial distance
approaches 1 cm. Comparison between Ge-71 and Sr-90/Y shows a similar
ity between their relative dose distribution in water. The dose distri
bution from a disc source was calculated using the EGS4 code and compa
red with the results from analytic calculation. Excellent agreement wa
s observed, confirming the validity of analytic calculations. The dose
rate at 0.01 cm from a Ge-71 disc source was calculated to be about 1
.3 x 10(-5) Gy MBq(-1) s(-1). Based on the results from this study, Ge
-71 activity of the order of 3.7 x 10(10) Bq (-1 Ci) might be necessar
y to obtain dose rates typical of Sr-90/Y ophthalmic applicators. The
possibility of using Ge-71 as a source of radioactive stents was also
investigated. A Ge-71 stent was modelled as a cylindrical shell source
and the dose rates were determined by Monte Carlo calculations. Some
calculated results are compared with published values for a P-32-coate
d stent. The dose rate at 0.01 cm from a Ge-71 stent has been calculat
ed to be about 6.5 x 10(-3) Gy MBq(-1) h(-1), which is much lower than
the reported dose rate at the same distance from a P-32-coated stent.
However, an initial source activity of the order of 3.7 x 10(7) Bq (s
imilar to 1 mCi) would easily result in a typical target dose (similar
to 24 Gy) needed for intravascular stent applications. In conclusion,
Ge-71 sources could be used as alternatives to beta sources and, unli
ke high-energy (similar to MeV) beta sources, may provide easily predi
ctable dose distributions in heterogeneous media and low dose rates, w
hich might be beneficial for some clinical applications.