Af. Chatziioannou et al., Performance evaluation of microPET: A high-resolution lutetium oxyorthosilicate PET scanner for animal imaging, J NUCL MED, 40(7), 1999, pp. 1164-1175
Citations number
40
Categorie Soggetti
Radiology ,Nuclear Medicine & Imaging","Medical Research Diagnosis & Treatment
A new dedicated PET scanner, microPET, was designed and developed at the Un
iversity of California, Los Angeles, for imaging small laboratory animals.
The goal was to provide a compact system with superior spatial resolution a
t a fraction of the cost of a clinical PFT scanner. Methods: The system use
s fiberoptic readout of individually cut lutetium oxyorthosilicate (LSO) cr
ystals to achieve high spatial resolution. Each microPET detector consists
of an 8 X 8 array of 2 x 2 x 10-mm LSO scintillation crystals that are coup
led to a 64-channel photomultiplier tube by optical fibers. The tomograph c
onsists of 30 detectors in a continuous ring with a 17.2-cm diameter and fi
elds of view (FOVs) of 11.25 cm in the transaxial direction and 1.8 cm in t
he axial direction. The system has eight crystal rings and no interplane se
pta. It operates exclusively in the three-dimensional mode and has an elect
ronically controlled bed that is capable of wobbling with a radius of 300 m
u m. We describe the performance of the tomograph in terms of its spatial,
energy and timing resolution, as well as its sensitivity and counting-rate
performance. We also illustrate its overall imaging performance with phanto
m and animal studies that demonstrate the potential applications of this de
vice to biomedical research. Results: Images reconstructed with three-dimen
sional filtered backprojection show a spatial resolution of 1.8 mm at the c
enter of the FOV (CFOV), which remains <2.5 mm for the central 5 cm of the
transaxial FOV. The resulting volumetric resolution of the system is <8 mu
L. The absolute system sensitivity measured with a 0.74 MBq (20 mu Ci) Ge-6
8 point source at the CFOV is 5.62 Hz/kBq. The maximum noise equivalent cou
nting rate obtained with a 6.4-cm diameter cylinder spanning the central 56
% of the FOV is 10 kcps, whereas the scatter fraction is 37% at the CFOV fo
r an energy window of 250-650 keV and the same diameter cylinder. Conclusio
n: This is the first PET scanner to use the new scintillator LSO and uses a
novel detector design to achieve high volumetric spatial resolution. The c
ombination of imaging characteristics of this prototype system (resolution,
sensitivity, counting rate performance and scatter fraction) opens up new
possibilities in the study of animal models with PET.