Physics in Medicine and Biology · 1992 · 293 citations · 15 references
MedicineNuclear MedicineRadiologyBiomedical ImagingDiagnostic ImagingDiagnostic RadiologyBrain ImagingImagingMedical ImagingMedical Imaging InstrumentationPositron Emission TomographyPositron Emission Tomography PhysicsDead Time EffectsDetectorsPet Image ReconstructionPositron Emission Tomography DetectorsPositron Emission Tomography InstrumentationThree-dimensional Positron Emission TomographyTomographic Imaging Systems
Performance characteristics of a new design of positron tomograph with automatically retractable septa for brain imaging have been studied. The device, consisting of block BGO detectors (8 x 8 elements per block), has a ring diameter of 76 cm and an axial FOV of 106.5 mm. The in-plane resolution is on average 5.8 mm and 5.0 mm (FWHM) for stationary and wobble sampling, respectively, over the central 18 cm of the transaxial FOV. Its unique feature is the capability of data acquisition both in the 'conventional' 2D mode (with septa) or 3D mode (septa retracted) where coincidences between any of the 16 detector rings are acquired. When scattered events are subtracted, the efficiency for a 20 cm diameter uniform cylinder increases overall by a factor of 4.8 between 2D (septa extended) and 3D modes. For a 20 cm phantom the trues/singles ratio is higher for 3D than for 2D but for a given unscattered trues rate, the randoms rate in 3D is higher. At 380 keV the scatter fraction within a 20 cm cylinder is 10% (septa extended) and 36% (retracted). In spite of the increase in scatter when septa are retracted, the increased efficiency in the 3D mode of acquisition yields distinct advantages, particularly in the many studies where tracer concentration is low and consequently where dead time and random rates are less important.
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Fully-three-dimensional positron emission tomography
James G. Colsher · Physics in Medicine and Biology · 1980 · 233 citations