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Zeng X, Zhang Z, Li D, Huang X, Wang Z, Wang Y, Zhou W, Wang P, Zhu M, Wei Q, Gong H, Wei L. Evaluation of monolithic crystal detector with dual-ended readout utilizing multiplexing method. Phys Med Biol 2024; 69:085003. [PMID: 38484392 DOI: 10.1088/1361-6560/ad3417] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/01/2023] [Accepted: 03/14/2024] [Indexed: 04/04/2024]
Abstract
Objective.Monolithic crystal detectors are increasingly being applied in positron emission tomography (PET) devices owing to their excellent depth-of-interaction (DOI) resolution capabilities and high detection efficiency. In this study, we constructed and evaluated a dual-ended readout monolithic crystal detector based on a multiplexing method.Approach.We employed two 12 × 12 silicon photomultiplier (SiPM) arrays for readout, and the signals from the 12 × 12 array were merged into 12 X and 12 Y channels using channel multiplexing. In 2D reconstruction, three methods based on the centre of gravity (COG) were compared, and the concept of thresholds was introduced. Furthermore, a light convolutional neural network (CNN) was employed for testing. To enhance depth localization resolution, we proposed a method by utilizing the mutual information from both ends of the SiPMs. The source width and collimation effect were simulated using GEANT4, and the intrinsic spatial resolution was separated from the measured values.Main results.At an operational voltage of 29 V for the SiPM, an energy resolution of approximately 12.5 % was achieved. By subtracting a 0.8 % threshold from the total energy in every channel, a 2D spatial resolution of approximately 0.90 mm full width at half maximum (FWHM) can be obtained. Furthermore, a higher level of resolution, approximately 0.80 mm FWHM, was achieved using a CNN, with some alleviation of edge effects. With the proposed DOI method, a significant 1.36 mm FWHM average DOI resolution can be achieved. Additionally, it was found that polishing and black coating on the crystal surface yielded smaller edge effects compared to a rough surface with a black coating.Significance.The introduction of a threshold in COG method and a dual-ended readout scheme can lead to excellent spatial resolution for monolithic crystal detectors, which can help to develop PET systems with both high sensitivity and high spatial resolution.
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Affiliation(s)
- Xiangtao Zeng
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Zhiming Zhang
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Daowu Li
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Xianchao Huang
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Zhuoran Wang
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Yingjie Wang
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Wei Zhou
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Peilin Wang
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Meiling Zhu
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Qing Wei
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Huixing Gong
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
| | - Long Wei
- Beijing Engineering Research Centre of Radiographic Techniques and Equipment, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- School of Nuclear Science and Technology, University of Chinese Academy of Sciences, Beijing 100049, People's Republic of China
- Jinan Laboratory of Applied Nuclear Science, Jinan 250131, People's Republic of China
- CAEA Centre of Excellence on Nuclear Technology Applications for Nuclear Detection and Imaging, Beijing 100049, People's Republic of China
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Gonzalez AJ, Berr SS, Cañizares G, Gonzalez-Montoro A, Orero A, Correcher C, Rezaei A, Nuyts J, Sanchez F, Majewski S, Benlloch JM. Feasibility Study of a Small Animal PET Insert Based on a Single LYSO Monolithic Tube. Front Med (Lausanne) 2018; 5:328. [PMID: 30547030 PMCID: PMC6279866 DOI: 10.3389/fmed.2018.00328] [Citation(s) in RCA: 16] [Impact Index Per Article: 2.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/03/2018] [Accepted: 11/09/2018] [Indexed: 11/26/2022] Open
Abstract
There are drawbacks with using a Positron Emission Tomography (PET) scanner design employing the traditional arrangement of multiple detectors in an array format. Typically PET systems are constructed with many regular gaps between the detector modules in a ring or box configuration, with additional axial gaps between the rings. Although this has been significantly reduced with the use of the compact high granularity SiPM photodetector technology, such a scanner design leads to a decrease in the number of annihilation photons that are detected causing lower scanner sensitivity. Moreover, the ability to precisely determine the line of response (LOR) along which the positron annihilated is diminished closer to the detector edges because the spatial resolution there is degraded due to edge effects. This happens for both monolithic based designs, caused by the truncation of the scintillation light distribution, but also for detector blocks that use crystal arrays with a number of elements that are larger than the number of photosensors and, therefore, make use of the light sharing principle. In this report we present a design for a small-animal PET scanner based on a single monolithic annulus-like scintillator that can be used as a PET insert in high-field Magnetic Resonance systems. We provide real data showing the performance improvement when edge-less modules are used. We also describe the specific proposed design for a rodent scanner that employs facetted outside faces in a single LYSO tube. In a further step, in order to support and prove the proposed edgeless geometry, simulations of that scanner have been performed and lately reconstructed showing the advantages of the design.
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Affiliation(s)
- Antonio J. Gonzalez
- Detector for Molecular Imaging Lab (DMIL), Instituto de Instrumentacion para Imagen Molecular (i3M), Centro Mixto CSIC - Universitat Politècnica de València, Valencia, Spain
| | - Stuart S. Berr
- Department of Radiology and Medical Imaging, University of Virginia, Charlottesville, VA, United States
| | - Gabriel Cañizares
- Detector for Molecular Imaging Lab (DMIL), Instituto de Instrumentacion para Imagen Molecular (i3M), Centro Mixto CSIC - Universitat Politècnica de València, Valencia, Spain
| | - Andrea Gonzalez-Montoro
- Detector for Molecular Imaging Lab (DMIL), Instituto de Instrumentacion para Imagen Molecular (i3M), Centro Mixto CSIC - Universitat Politècnica de València, Valencia, Spain
| | | | | | - Ahmadreza Rezaei
- Nuclear Medicine and Medical Imaging Research CenterKU Leuven, Leuven, Belgium
| | - Johan Nuyts
- Nuclear Medicine and Medical Imaging Research CenterKU Leuven, Leuven, Belgium
- MoSAIC, Molecular Small Animal Imaging Center, KU Leuven – University of LeuvenLeuven, Belgium
| | - Filomeno Sanchez
- Detector for Molecular Imaging Lab (DMIL), Instituto de Instrumentacion para Imagen Molecular (i3M), Centro Mixto CSIC - Universitat Politècnica de València, Valencia, Spain
| | - Stan Majewski
- Department of Radiology and Medical Imaging, University of Virginia, Charlottesville, VA, United States
| | - Jose M. Benlloch
- Detector for Molecular Imaging Lab (DMIL), Instituto de Instrumentacion para Imagen Molecular (i3M), Centro Mixto CSIC - Universitat Politècnica de València, Valencia, Spain
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