Earlier investigations with EGO positron emission tomography (PET) scanners
showed that the scatter correction technique based on multiple acquisition
s with different energy windows are problematic to implement because of the
poor energy resolution of EGO (22%), particularly for whole-body studies.
We believe that these methods are likely to work better with NaI(TI) becaus
e of the better energy resolution achievable with NaI(TI) detectors (10%),
Therefore, we investigate two different choices for the energy window, a lo
w-energy window (LEW) on the Compton spectrum at 400-450 keV, and a high-en
ergy window (HEW) within the photopeak (lower threshold above 511 keV). The
results obtained for our three-dimensional (3-D) (septa-less) whole-body s
canners [axial field of view (FOV) of 12.8 cm and 25.6 cm] as well as for o
ur 3-D brain scanner (axial FOV of 25.6 cm) show an accurate prediction of
the scatter distribution for the estimation of trues method (ETM) using a H
EW, leading to a significant reduction of the scatter contamination. The du
al-energy window (DEW) technique using a LEW is shown to be intrinsically w
rong; in particular, it fails for line source and bar phantom measurements,
However, the method is able to produce good results for homogeneous activi
ty distributions. Both methods are easy to implement, are fast, have a low
noise propagation, and will be applicable to other PET scanners with good e
nergy resolution and stability, such as hybrid NaI(TI) PET/SPECT dual-head
cameras and future PET cameras with GSO or LSO scintillators.