• DocumentCode
    58170
  • Title

    Evaluation of PET Imaging Resolution Using 350 \\mu\\hbox {m} Pixelated CZT as a VP-PET Insert Detector

  • Author

    Yongzhi Yin ; Ximeng Chen ; Chongzheng Li ; Heyu Wu ; Komarov, Sergey ; Qingzhen Guo ; Krawczynski, H. ; Ling-Jian Meng ; Yuan-Chuan Tai

  • Author_Institution
    Sch. of Nucl. Sci. & Technol., Lanzhou Univ., Lanzhou, China
  • Volume
    61
  • Issue
    1
  • fYear
    2014
  • fDate
    Feb. 2014
  • Firstpage
    154
  • Lastpage
    161
  • Abstract
    A cadmium-zinc-telluride (CZT) detector with 350 μm pitch pixels was studied in high-resolution positron emission tomography (PET) imaging applications. The PET imaging system was based on coincidence detection between a CZT detector and a lutetium oxyorthosilicate (LSO)-based Inveon PET detector in virtual-pinhole PET geometry. The LSO detector is a 20 ×20 array, with 1.6 mm pitches, and 10 mm thickness. The CZT detector uses ac 20 ×20 ×5 mm substrate, with 350 μm pitch pixelated anodes and a coplanar cathode. A NEMA NU4 Na-22 point source of 250 μm in diameter was imaged by this system. Experiments show that the image resolution of single-pixel photopeak events was 590 μm FWHM while the image resolution of double-pixel photopeak events was 640 μm FWHM. The inclusion of double-pixel full-energy events increased the sensitivity of the imaging system. To validate the imaging experiment, we conducted a Monte Carlo (MC) simulation for the same PET system in Geant4 Application for Emission Tomography. We defined LSO detectors as a scanner ring and 350 μm pixelated CZT detectors as an insert ring. GATE simulated coincidence data were sorted into an insert-scanner sinogram and reconstructed. The image resolution of MC-simulated data (which did not factor in positron range and acolinearity effect) was 460 μm at FWHM for single-pixel events. The image resolutions of experimental data, MC simulated data, and theoretical calculation are all close to 500 μm FWHM when the proposed 350 μm pixelated CZT detector is used as a PET insert. The interpolation algorithm for the charge sharing events was also investigated. The PET image that was reconstructed using the interpolation algorithm shows improved image resolution compared with the image resolution without interpolation algorithm.
  • Keywords
    Monte Carlo methods; biomedical equipment; cadmium compounds; coincidence techniques; image resolution; interpolation; medical image processing; positron emission tomography; semiconductor counters; solid scintillation detectors; zinc compounds; CdZnTe; FWHM; GATE simulated coincidence data; Geant4 Application for Emission Tomography; Monte Carlo simulation data; NEMA NU4 Na-22 point source; PET imaging resolution; VP-PET insert detector; acolinearity effect; charge sharing events; coincidence detection; coplanar cathode; double-pixel full-energy events; double-pixel photopeak events; high-resolution positron emission tomography imaging applications; imaging experiment; imaging system; improved image resolution; insert ring; insert-scanner sinogram; interpolation algorithm; lutetium oxyorthosilicate-based Inveon PET detector; pixelated anodes; pixelated cadmium-zinc-telluride detector; scanner ring; single-pixel events; single-pixel photopeak events; virtual-pinhole PET geometry; Detectors; Image quality; Image reconstruction; Image resolution; Positron emission tomography; Positrons; Cadmium–zinc–telluride (CZT) detectors; coincidence techniques; imaging applications; positron emission tomography (PET);
  • fLanguage
    English
  • Journal_Title
    Nuclear Science, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-9499
  • Type

    jour

  • DOI
    10.1109/TNS.2013.2294011
  • Filename
    6710182