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High resolution detectors for whole-body PET scanners by using dual-ended readout
BACKGROUND: Most current whole-body positron emission tomography (PET) scanners use detectors with high timing resolution to measure the time-of-flight of two 511 keV photons, improving the signal-to-noise ratio of PET images. However, almost all current whole-body PET scanners use detectors without...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Springer International Publishing
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9023628/ https://www.ncbi.nlm.nih.gov/pubmed/35445890 http://dx.doi.org/10.1186/s40658-022-00460-4 |
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author | Liu, Zheng Niu, Ming Kuang, Zhonghua Ren, Ning Wu, San Cong, Longhan Wang, Xiaohui Sang, Ziru Williams, Crispin Yang, Yongfeng |
author_facet | Liu, Zheng Niu, Ming Kuang, Zhonghua Ren, Ning Wu, San Cong, Longhan Wang, Xiaohui Sang, Ziru Williams, Crispin Yang, Yongfeng |
author_sort | Liu, Zheng |
collection | PubMed |
description | BACKGROUND: Most current whole-body positron emission tomography (PET) scanners use detectors with high timing resolution to measure the time-of-flight of two 511 keV photons, improving the signal-to-noise ratio of PET images. However, almost all current whole-body PET scanners use detectors without depth-encoding capability; therefore, their spatial resolution can be affected by the parallax effect. METHODS: In this work, four depth-encoding detectors consisting of LYSO arrays with crystals of 2.98 × 2.98 × 20 mm(3), 2.98 × 2.98 × 30 mm(3), 1.95 × 1.95 × 20 mm(3), and 1.95 × 1.95 × 30 mm(3), respectively, were read at both ends, with 6 × 6 mm(2) silicon photomultiplier (SiPM) pixels in a 4 × 4 array being used. The timing signals of the detectors were processed individually using an ultrafast NINO application-specific integrated circuit (ASIC) to obtain good timing resolution. The 16 energy signals of the SiPM array were read using a row and column summing circuit to obtain four position-encoding energy signals. RESULTS: The four PET detectors provided good flood histograms in which all crystals could be clearly resolved, the crystal energy resolutions measured being 10.2, 12.1, 11.4 and 11.7% full width at half maximum (FWHM), at an average crystal depth of interaction (DOI) resolution of 3.5, 3.9, 2.7, and 3.0 mm, respectively. The depth dependence of the timing of each SiPM was measured and corrected, the timing of the two SiPMs being used as the timing of the dual-ended readout detector. The four detectors provided coincidence time resolutions of 180, 214, 239, and 263 ps, respectively. CONCLUSIONS: The timing resolution of the dual-ended readout PET detector was approximately 20% better than that of the single-ended readout detector using the same LYSO array, SiPM array, and readout electronics. The detectors developed in this work used long crystals with small cross-sections and provided good flood histograms, DOI, energy, and timing resolutions, suggesting that they could be used to develop whole-body PET scanners with high sensitivity, uniform high spatial resolution, and high timing resolution. |
format | Online Article Text |
id | pubmed-9023628 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | Springer International Publishing |
record_format | MEDLINE/PubMed |
spelling | pubmed-90236282022-05-06 High resolution detectors for whole-body PET scanners by using dual-ended readout Liu, Zheng Niu, Ming Kuang, Zhonghua Ren, Ning Wu, San Cong, Longhan Wang, Xiaohui Sang, Ziru Williams, Crispin Yang, Yongfeng EJNMMI Phys Original Research BACKGROUND: Most current whole-body positron emission tomography (PET) scanners use detectors with high timing resolution to measure the time-of-flight of two 511 keV photons, improving the signal-to-noise ratio of PET images. However, almost all current whole-body PET scanners use detectors without depth-encoding capability; therefore, their spatial resolution can be affected by the parallax effect. METHODS: In this work, four depth-encoding detectors consisting of LYSO arrays with crystals of 2.98 × 2.98 × 20 mm(3), 2.98 × 2.98 × 30 mm(3), 1.95 × 1.95 × 20 mm(3), and 1.95 × 1.95 × 30 mm(3), respectively, were read at both ends, with 6 × 6 mm(2) silicon photomultiplier (SiPM) pixels in a 4 × 4 array being used. The timing signals of the detectors were processed individually using an ultrafast NINO application-specific integrated circuit (ASIC) to obtain good timing resolution. The 16 energy signals of the SiPM array were read using a row and column summing circuit to obtain four position-encoding energy signals. RESULTS: The four PET detectors provided good flood histograms in which all crystals could be clearly resolved, the crystal energy resolutions measured being 10.2, 12.1, 11.4 and 11.7% full width at half maximum (FWHM), at an average crystal depth of interaction (DOI) resolution of 3.5, 3.9, 2.7, and 3.0 mm, respectively. The depth dependence of the timing of each SiPM was measured and corrected, the timing of the two SiPMs being used as the timing of the dual-ended readout detector. The four detectors provided coincidence time resolutions of 180, 214, 239, and 263 ps, respectively. CONCLUSIONS: The timing resolution of the dual-ended readout PET detector was approximately 20% better than that of the single-ended readout detector using the same LYSO array, SiPM array, and readout electronics. The detectors developed in this work used long crystals with small cross-sections and provided good flood histograms, DOI, energy, and timing resolutions, suggesting that they could be used to develop whole-body PET scanners with high sensitivity, uniform high spatial resolution, and high timing resolution. Springer International Publishing 2022-04-21 /pmc/articles/PMC9023628/ /pubmed/35445890 http://dx.doi.org/10.1186/s40658-022-00460-4 Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visithttp://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Original Research Liu, Zheng Niu, Ming Kuang, Zhonghua Ren, Ning Wu, San Cong, Longhan Wang, Xiaohui Sang, Ziru Williams, Crispin Yang, Yongfeng High resolution detectors for whole-body PET scanners by using dual-ended readout |
title | High resolution detectors for whole-body PET scanners by using dual-ended readout |
title_full | High resolution detectors for whole-body PET scanners by using dual-ended readout |
title_fullStr | High resolution detectors for whole-body PET scanners by using dual-ended readout |
title_full_unstemmed | High resolution detectors for whole-body PET scanners by using dual-ended readout |
title_short | High resolution detectors for whole-body PET scanners by using dual-ended readout |
title_sort | high resolution detectors for whole-body pet scanners by using dual-ended readout |
topic | Original Research |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9023628/ https://www.ncbi.nlm.nih.gov/pubmed/35445890 http://dx.doi.org/10.1186/s40658-022-00460-4 |
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