• DocumentCode
    35036
  • Title

    Impact of Laser-Processed X´tal Cube Detectors on PET Imaging in a One-Pair Prototype System

  • Author

    Yoshida, Erika ; Hirano, Yoshikuni ; Tashima, Hideaki ; Inadama, Naoko ; Nishikido, Fumihiko ; Moriya, Takehiro ; Omura, T. ; Watanabe, Manabu ; Murayama, Hiroki ; Yamaya, Taiga

  • Author_Institution
    Nat. Inst. of Radiol. Sci., Chiba, Japan
  • Volume
    60
  • Issue
    5
  • fYear
    2013
  • fDate
    Oct. 2013
  • Firstpage
    3172
  • Lastpage
    3180
  • Abstract
    The X´tal cube is our original PET detector, which is being developed to achieve isotropic 3D positioning detectability. The X´tal cube is based on a 3D segmented crystal block for which all surfaces are covered with photo-detectors. Previously, instead of our initial approach of gluing segmented pieces of crystals, we successfully constructed a crystal block segmented by laser processing, and we developed the X´tal cube with the laser-processed 3D square grids of 2 mm length. In this paper, we extend the laser processing to 3D square grids of 1 mm length. The volume of a 1-mm crystal segment is 1/8 of that of a 2-mm crystal segment. We also evaluate imaging resolution performance with a newly developed one-pair prototype system to simulate a ring-type scanner, while our previous reports were limited to development and evaluation of a single detector. In particular, we compare 1-mm X´tal cube detectors to 2-mm X´tal cube detectors. The one-pair prototype system consisted of two X´tal cubes, two rotating stages, and a 192-channel data acquisition system. Each X´tal cube consisted of the LYSO cubic crystal block of 18 × 18 × 18 mm3 in which the 3D grids of 1 mm pitch were fabricated by internal laser processing. The 4 × 4 arrays of multi pixel photon counters were optically coupled to each surface of the crystal block. The detector positions were automatically controlled to simulate a ring-type PET with a 14.6 cm diameter. Data were collected for all assumed detector positions and then a sinogram was obtained. The data were reconstructed using filtered backprojection. The average spatial resolution of the 2-mm X´tal cube was 1.9 mm full width at half maximum (FWHM) over the field-of-view (FOV). On the other hand, the average spatial resolution of the 1-mm X´tal cube was 1.3 mm FWHM over the FOV. By applying deconvolution with the assumption that the point source was a Gaussian function of 1.0 mm FWHM, we estimated the avera- e spatial resolution of the 2-mm X´tal cube and the 1-mm X´tal cube as 1.6 mm FWHM and 0.83 mm FWHM, respectively. The average spatial resolution of the 1-mm X´tal cube was improved approximately 48% compared to the 2-mm X´tal cube. In conclusion, we confirmed the potential of the X´tal cube for uniform and high resolution imaging.
  • Keywords
    Gaussian processes; biomedical equipment; data acquisition; deconvolution; image reconstruction; image resolution; image segmentation; laser applications in medicine; medical image processing; photodetectors; positron emission tomography; 3D segmented crystal block; 3D square grids; FWHM; Gaussian function; LYSO cubic crystal block; PET imaging; crystal segment; data acquisition; deconvolution; filtered backprojection; full width-at-half maximum; image resolution; internal laser processing; isotropic 3D positioning detectability; laser-processed Xtal cube detectors; multipixel photon counters; one-pair prototype system; photodetectors; sinogram; spatial resolution; Crystals; Detectors; Laser beams; Positron emission tomography; Prototypes; Spatial resolution; Three-dimensional displays; Detector instrumentation; PET;
  • fLanguage
    English
  • Journal_Title
    Nuclear Science, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-9499
  • Type

    jour

  • DOI
    10.1109/TNS.2013.2280631
  • Filename
    6616647