Abstract
Purpose: To compare slitāslat collimators in singleālayer and staggered arrays with standard parallelābeam collimators in a dedicated breast SPECT system. Methods: A ring of slitāslat collimators surrounds a cylindrical region of 20 cm diameter for SPECTimaging of a pendant breast. A second ring of cameras, viewing between cameras in the first ring, may be added to give a staggered array of cameras. Such arrays could be static or rotating; for now, we assume a rotating array, for a radially symmetric ray pattern. Slit width and slat design are specified to match the spatial resolution of a lowāenergy allāpurpose parallelāhole (LEAP) collimator at the axis of rotation. Sensitivity is calculated for arrays of slitāslat and parallelāhole collimated cameras, using the maximum number of cameras possible for each. Results: With focal length of 5.7 cm, detector width of 6.5 cm, and 15 cm radius of rotation (ROR), the slitāslat array could contain twenty cameras for one ring, and forty cameras for two rings. A LEAPācollimated system with 10 cm ROR could contain four cameras and would have a spatial resolution of 8.0 mm at the axis of rotation. To match this, the slitāslat collimators would have slit widths of 2.2mm/1.8mm for first and second rows respectively, and slats designed for similar axial resolution. A single row of twenty slitāslat collimated cameras would have a sensitivity of 8.66Ć10, ā4photons transmitted per photon emitted, while a staggered array would have a sensitivity of 1.28Ć10, ā3. The array of four LEAPācollimated cameras would have a sensitivity of 6.48 Ć10, ā4. Conclusions: The singleā ring configuration of cameras gives sensitivity 34% greater than the LEAPā collimated system, while the staggered array gives a 98% sensitivity increase. This doubling in sensitivity comes with a large increase in complexity. Further optimizations for the slitāslat system are possible in both areas.
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