• DocumentCode
    1826320
  • Title

    Design of an inexpensive high-sensitivity rodent-research PET camera (RRPET)

  • Author

    Wong, Wai-Hoi ; Li, Hongdi ; Xie, Shuping ; Ramirez, Rocio ; Kim, Soonseok ; Uribe, Jorge ; Wang, Yu ; Liu, Yaqiang ; Xing, Tao ; Baghaei, Hossain

  • Author_Institution
    Texas Univ., Houston, TX, USA
  • Volume
    3
  • fYear
    2003
  • fDate
    19-25 Oct. 2003
  • Firstpage
    2058
  • Abstract
    A small animal PET is being developed. The design goals are lower cost, higher sensitivity and same image resolution as commercial animal PET. It uses a new version of our PMT-quadrant-sharing (PQS) detector with a 98% crystal-packing fraction to maximize sensitivity and no light-guides to maximize light output (decoding resolution). It uses 168 low-cost 19-mm PMT and 9216 BGO for its high photoelectric fraction. Each block is 8×8 with an average pitch of 2×2 mm (10 mm deep) to provide image resolution similar to commercial systems using LSO, position-sensitive PMT and optical fibers. The number-of-crystals-per-PMT decoding ratio achieved was 55, similar to an animal PET using GSO that has 3 times more light output than BGO. To maximize image resolution, we "circularize" the PQS detector design, where each block is one side of a 24-sided polygon (the detector ring). Circularizing PQS detector requires the block to be ground slightly into a pentagon (166° apex). The edge rows of crystals in the block are also tapered, so that blocks can be glued together to form a solid BGO ring with nearly 100% packing. The ring diameter is 13 cm. 6 rings provide a 12-cm axial FOV. The large axial FOV increases coincidence sensitivity. An automatic PMT-equalization system can tune the PET in 1 minute without radiation, for PMT tuning before each study to minimize the effects of prior radiation loading and temperature drift. Detector-pileup-recovery electronics were used to prevent imaging artifacts and count-loss in BGO detectors. Experiments showed that 2×2×10 mm BGO can be decoded (energy resolution 23%). Monte Carlo simulation showed a detection efficiency of 5.9% (350-700 KeV) for a central point source. The 3.7× increase in coincidence sensitivity comes from (a) larger axial-FOV (1.8×), (b) BGO higher photoelectric fraction (1.5×) and (c) high packing fraction (1.3×).
  • Keywords
    Monte Carlo methods; decoding; gamma-ray detection; image resolution; medical image processing; positron emission tomography; solid scintillation detectors; 1 min; 10 mm; 12 cm; 13 cm; 19 mm; 2 mm; 350 to 700 keV; BGO detectors; Monte Carlo simulation; decoding resolution; detector-pileup-recovery electronics; image resolution; inexpensive high-sensitivity rodent-research PET camera; optical fibers; photoelectric fraction; photomultiplier-quadrant-sharing detector; position-sensitive photomultipliers; small animal PET; Animals; Cameras; Costs; Crystals; Decoding; Detectors; Image edge detection; Image resolution; Optical fibers; Positron emission tomography;
  • fLanguage
    English
  • Publisher
    ieee
  • Conference_Titel
    Nuclear Science Symposium Conference Record, 2003 IEEE
  • ISSN
    1082-3654
  • Print_ISBN
    0-7803-8257-9
  • Type

    conf

  • DOI
    10.1109/NSSMIC.2003.1352285
  • Filename
    1352285