Investigation of the "block effect" on spatial resolution in PET detectors

Previous studies suggest that when block detectors are used in positron emission tomography (PET) scanners, a "block effect" of about 2 mm can be added in quadrature to the other effects blurring spatial resolution (SR). However, no explanation of the cause of the effect has ever been published. We studied the origin of the "block effect", using experiments in which all other blurring effects on SR were minimized and precisely determined. Thin (1 mm) bismuth germanate (BGO) crystals and a small (1 mm) /sup 68/Ge source were used to probe the SR of a CTI HR+ block detector and two precise translation stages to move detectors. We compared coincidence aperture functions (CAFs) for crystals in the block with CAFs of single crystals of various widths. From those measurements, done with one block detector, we concluded that the central crystals in the block showed an additional blurring of 0.8 mm whereas the edge ones showed no additional blurring. The obtained full width at half maximum (FWHM) for central crystals was found to be 2.20 /spl plusmn/ 0.05 mm and for edge crystals 1.98 /spl plusmn/ 0.03 mm. The FWHM for 4.4 mm width crystals (as used in the HR+ block) was estimated to be 2.1 /spl plusmn/ 0.2 mm. Results from the crystal identification matrix show that the apparent centroids of the crystals are not located at the geometric centers, which would give errors in the reconstruction algorithm assumed uniform sampling. Our results suggest that the additional blurring previously reported in PET scanners with block detectors is not only due to the use of block detectors.