In I-131 SPECT, image quality and quantification accuracy are degraded by o
bject scatter as well as scatter and penetration in the collimator. The cha
racterization of energy and spatial distributions of scatter and penetratio
n performed in this study by Monte Carlo simulation will be useful for the
development and evaluation of techniques that compensate for such events in
I-131 imaging. Methods: First, to test the accuracy of the Monte Carlo mod
el, simulated and measured data were compared for both a point source and a
phantom. Next, simulations to investigate scatter and penetration were per
formed for four geometries: point source in air, point source in a water-fi
lled cylinder, hot sphere in a cylinder filled with nonradioactive water, a
nd hot sphere in a cylinder filled with radioactive water. Energy spectra w
ere separated according to order of scatter, type of interaction, and gamma
-ray emission energy. A preliminary evaluation of the triple-energy window
(TEW) scatter correction method was performed. Results: The accuracy of the
Monte Carlo model was verified by the good agreement between measured and
simulated energy spectra and radial point spread functions. For a point sou
rce in air, simulations show that 73% of events in the photopeak window had
either scattered in or penetrated the collimator, indicating the significa
nce of collimator interactions. For a point source in a water-filled phanto
m, the separated energy spectra showed that a 20% photopeak window can be u
sed to eliminate events that scatter more than two times in the phantom. Fo
r the hot sphere phantoms, it was shown that in the photopeak region the sp
ectrum shape of penetration events is very similar to that of primary (no s
catter and no penetration) events. For the hot sphere regions of interest,
the percentage difference between true scatter counts and the TEW estimate
of scatter counts was <12%. Conclusion: In I-131 SPECT, object scatter as w
ell as collimator scatter and penetration are significant. The TEW method p
rovides a reasonable correction for scatter, but the similarity between the
364-keV primary and penetration energy spectra makes it difficult to compe
nsate for these penetration events using techniques that are based on spect
ral analysis.