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A finely segmented semi‐monolithic detector tailored for high‐resolution PET

Medical Physics, vol. 51, pp. 3421–3436

Abstract

BACKGROUND: Preclinical research and organ-dedicated applications use and require high (spatial-)resolution positron emission tomography (PET) detectors to visualize small structures (early) and understand biological processes at a finer level of detail. Researchers seeking to improve detector and image spatial resolution have explored various detector designs. Current commercial high-resolution systems often employ finely pixelated or monolithic scintillators, each with its limitations. PURPOSE: , coupled to a 12 × 12 readout channel photosensor with 4 mm pitch. The slabs are grouped in two arrays of 44 slabs each to achieve a higher optical photon density despite the fine segmentation. METHODS: We employ a fan beam collimator for fast calibration to train machine-learning-based positioning models for all three dimensions, including slab identification and depth-of-interaction (DOI), utilizing gradient tree boosting (GTB). The data for all dimensions was acquired in less than 2 h. Energy calculation was based on a position-dependent energy calibration. Using an analytical timing calibration, time skews were corrected for coincidence timing resolution (CTR) estimation. RESULTS: Leveraging machine-learning-based calibration in all three dimensions, we achieved high detector spatial resolution: down to 1.18 mm full width at half maximum (FWHM) detector spatial resolution and 0.75 mm mean absolute error (MAE) in the planar-monolithic direction, and 2.14 mm FWHM and 1.03 mm MAE for DOI at an energy window of (435-585) keV. Correct slab interaction identification in planar-segmented direction exceeded 80%, alongside an energy resolution of 12.7% and a CTR of 450 ps FWHM. CONCLUSIONS: The introduced finely segmented, high-resolution slab detector demonstrates appealing performance characteristics suitable for high-resolution PET applications. The current benchtop-based detector calibration routine allows these detectors to be used in PET systems.

Authors 9

  1. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

  2. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

  3. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

  4. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

  5. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Hyperion Hybrid Imaging Systems GmbH Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

    Hyperion Hybrid Imaging Systems GmbH, Aachen, Germany

  6. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Hyperion Hybrid Imaging Systems GmbH Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

    Hyperion Hybrid Imaging Systems GmbH, Aachen, Germany

  7. Affiliation as printed

    Hyperion Hybrid Imaging Systems GmbH Aachen Germany

    Hyperion Hybrid Imaging Systems GmbH, Aachen, Germany

  8. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

  9. RWTH Aachen University

    Affiliation as printed

    Department of Physics of Molecular Imaging Systems Institute for Experimental Molecular Imaging RWTH Aachen University Aachen Germany

    Hyperion Hybrid Imaging Systems GmbH Aachen Germany

    Physics Institute III B RWTH Aachen University Aachen Germany

    Department of Physics of Molecular Imaging Systems, Institute for Experimental Molecular Imaging, RWTH Aachen University, Aachen, Germany

    Hyperion Hybrid Imaging Systems GmbH, Aachen, Germany

    Physics Institute III B, RWTH Aachen University, Aachen, Germany

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References 68