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Development and Validation of an Accurate Gate Model for Neuropet Scanner Publisher Pubmed



Sheikhzadeh P1, 2 ; Sabet H3 ; Ghadiri H1, 2 ; Geramifar P4 ; Mahani H2, 5 ; Ghafarian P6, 7 ; Ay MR1, 2
Authors
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Authors Affiliations
  1. 1. Department of Medical Physics and Biomedical Engineering, Tehran University of Medical Science, Tehran, Iran
  2. 2. Research Center for Molecular and Cellular Imaging, Tehran University of Medical Sciences, Tehran, Iran
  3. 3. Massachusetts General Hospital, Harvard Medical School, Boston, MA, United States
  4. 4. Research Center for Nuclear Medicine, Shariati Hospital, Tehran University of Medical Sciences, Tehran, Iran
  5. 5. Radiation Application Research School, Nuclear Science and Technology Research Institute, Tehran, Iran
  6. 6. Chronic Respiratory Diseases Research Center, National Research Institute of Tuberculosis and Lung Diseases (NRITLD), Shahid Beheshti University of Medical Sciences, Tehran, Iran
  7. 7. PET/CT and Cyclotron Center, Masih Daneshvari Hospital, Shahid Beheshti University of Medical Sciences, Tehran, Iran

Source: Physica Medica Published:2017


Abstract

NeuroPET is a cylindrical full ring mobile PET/CT scanner for brain imaging that was developed by Photo Diagnostic Systems, Inc. The scanner has 7 modules, each with 3 × 4 detector blocks. The detectors have two layers of scintillator arrays with a half pixel pitch offset to realize two levels of depth of interaction. In this study, we evaluated the NeuroPET scanner modeled in the GATE simulation tool and analyzed the acquired data to better understand the contribution of inter-detector scattering (IDS). The results show that the average difference between simulated and measured data for a point-like source is 2.5%. The differences are 4.7% and 2.7% for NEMA line source in two data acquisition modes and 5.5% for peak NECR measurement. IDS evaluation indicated that the total fractions of the cross-layer crystal scatter (CLCS) and inter-layer crystal scatter (ILCS) events in singles detection mode are 1.98% and 7.98%, respectively. Approximately 90% of these CLCS events deposit most of their energy in the crystal layer other than the layer of first interaction. Additionally, no significant difference in ILCS fractions between the two layers (8.05% vs 7.35%) was observed. The simulation results demonstrate that ILCS events account for ∼79% of the total mis-positioned events. © 2017 Associazione Italiana di Fisica Medica
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