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PET detectors with 127 ps CTR for the Tachyon-II time-of-flight PET scanner
The signal-to-noise ratio (SNR) of the reconstructed image of Positron Emission Tomography (PET) can be improved by the timing measurement. In this article, we designed, fabricated and tested 32 time-of-flight (TOF) detectors for the second generation of Tachyon TOF-PET scanners. The detector module...
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Published in: | Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment Accelerators, spectrometers, detectors and associated equipment, 2019-07, Vol.933, p.48-55 |
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description | The signal-to-noise ratio (SNR) of the reconstructed image of Positron Emission Tomography (PET) can be improved by the timing measurement. In this article, we designed, fabricated and tested 32 time-of-flight (TOF) detectors for the second generation of Tachyon TOF-PET scanners. The detector module consists of two arrays of 2 × 12 lutetium–yttrium oxyorthosilicate (LYSO) crystal cubes of 6 ×6× 6 mm3. The discrete crystals were coupled to the 6 mm silicon photomultipliers (SiPMs) with optical glue. All the SiPM were tested for dark current. To correct the errors in the timing measurements caused by time-walk, two compensation methods (log-correction and linear-correction) based on the relationship between energy and timing information were purposed. As a comparison, the SiPM arrays coupled to 4 mm and 6 mm side crystal cube without optical glue were tested for coincidence timing resolution (CTR). The mean and standard deviations (SD) of dark current for the 1536 tested SiPMs were 12.72 +/- 1.70 μA at the bias voltage of 31.5 V and the temperature of 20 °C (±1 °C). CTR performance has increased by ∼5% within a narrow energy window, and ∼10% in a wide energy window by log-correction. The mean and SD of the CTR of 6 mm side crystal cube glue coupled was 126.9 +/- 3.6 ps for the 768 pairs of tested SiPMs. The detector is expected to provide a technical reference for the next generation of ultra-fast CTR commercial PET scanner using multilayer detectors. |
doi_str_mv | 10.1016/j.nima.2019.03.083 |
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Section A, Accelerators, spectrometers, detectors and associated equipment</title><description>The signal-to-noise ratio (SNR) of the reconstructed image of Positron Emission Tomography (PET) can be improved by the timing measurement. In this article, we designed, fabricated and tested 32 time-of-flight (TOF) detectors for the second generation of Tachyon TOF-PET scanners. The detector module consists of two arrays of 2 × 12 lutetium–yttrium oxyorthosilicate (LYSO) crystal cubes of 6 ×6× 6 mm3. The discrete crystals were coupled to the 6 mm silicon photomultipliers (SiPMs) with optical glue. All the SiPM were tested for dark current. To correct the errors in the timing measurements caused by time-walk, two compensation methods (log-correction and linear-correction) based on the relationship between energy and timing information were purposed. As a comparison, the SiPM arrays coupled to 4 mm and 6 mm side crystal cube without optical glue were tested for coincidence timing resolution (CTR). The mean and standard deviations (SD) of dark current for the 1536 tested SiPMs were 12.72 +/- 1.70 μA at the bias voltage of 31.5 V and the temperature of 20 °C (±1 °C). CTR performance has increased by ∼5% within a narrow energy window, and ∼10% in a wide energy window by log-correction. The mean and SD of the CTR of 6 mm side crystal cube glue coupled was 126.9 +/- 3.6 ps for the 768 pairs of tested SiPMs. The detector is expected to provide a technical reference for the next generation of ultra-fast CTR commercial PET scanner using multilayer detectors.</description><subject>Coincidence events</subject><subject>Dark current</subject><subject>Energy resolution</subject><subject>Positron emission tomography</subject><subject>Time resolution</subject><subject>TOF PET</subject><issn>0168-9002</issn><issn>1872-9576</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp9UU1r3DAQFSWl2ab9Az3pmItdfViWBCUQlm27NNBStmdhy6NYi9faSNqE_PvKbCjk0rnMYd7H8B5CnyipKaHt5309-0NXM0J1TXhNFH-DVlRJVmkh2wu0KiBVaULYJXqf0p6U0VK9Q5ecU86aVq_Qj1-bHR4gg80hJvzk84gpk_iY8Hr3G7sQcR4B7zo7Poe52m5x9geogqvc5O_HjBd-st08Q_yA3rpuSvDxZV-hP183u_X36u7nt-369q6yDWe5stSpoRGtEJz33La6Ayd612oNtG-gl1w2TBAH1krFWua4sFwNXA8coKeEX6Gbs-7x1B9gsDDn2E3mGEsa8dmEzpvXl9mP5j48Gim01IQXgesXgRgeTpCyOfhkYZq6GcIpGVa-U0I0avFiZ6iNIaUI7p8NJWZpwezN0oJZWjCEm9JCIX05k6Ck8OghmmQ9zBYGH0vQZgj-f_S_Z8qOCQ</recordid><startdate>20190721</startdate><enddate>20190721</enddate><creator>Xie, Siwei</creator><creator>Zhang, Xi</creator><creator>Peng, Hui</creator><creator>Yang, Jingwu</creator><creator>Huang, Qiu</creator><creator>Xu, Jianfeng</creator><creator>Peng, Qiyu</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>5PM</scope></search><sort><creationdate>20190721</creationdate><title>PET detectors with 127 ps CTR for the Tachyon-II time-of-flight PET scanner</title><author>Xie, Siwei ; Zhang, Xi ; Peng, Hui ; Yang, Jingwu ; Huang, Qiu ; Xu, Jianfeng ; Peng, Qiyu</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c432t-c1f8d4565533b3c69aef5bf699e1b4eb7374250fecc78262f35c38d39d3eeb103</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2019</creationdate><topic>Coincidence events</topic><topic>Dark current</topic><topic>Energy resolution</topic><topic>Positron emission tomography</topic><topic>Time resolution</topic><topic>TOF PET</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Xie, Siwei</creatorcontrib><creatorcontrib>Zhang, Xi</creatorcontrib><creatorcontrib>Peng, Hui</creatorcontrib><creatorcontrib>Yang, Jingwu</creatorcontrib><creatorcontrib>Huang, Qiu</creatorcontrib><creatorcontrib>Xu, Jianfeng</creatorcontrib><creatorcontrib>Peng, Qiyu</creatorcontrib><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Xie, Siwei</au><au>Zhang, Xi</au><au>Peng, Hui</au><au>Yang, Jingwu</au><au>Huang, Qiu</au><au>Xu, Jianfeng</au><au>Peng, Qiyu</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>PET detectors with 127 ps CTR for the Tachyon-II time-of-flight PET scanner</atitle><jtitle>Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment</jtitle><date>2019-07-21</date><risdate>2019</risdate><volume>933</volume><spage>48</spage><epage>55</epage><pages>48-55</pages><issn>0168-9002</issn><eissn>1872-9576</eissn><abstract>The signal-to-noise ratio (SNR) of the reconstructed image of Positron Emission Tomography (PET) can be improved by the timing measurement. In this article, we designed, fabricated and tested 32 time-of-flight (TOF) detectors for the second generation of Tachyon TOF-PET scanners. The detector module consists of two arrays of 2 × 12 lutetium–yttrium oxyorthosilicate (LYSO) crystal cubes of 6 ×6× 6 mm3. The discrete crystals were coupled to the 6 mm silicon photomultipliers (SiPMs) with optical glue. All the SiPM were tested for dark current. To correct the errors in the timing measurements caused by time-walk, two compensation methods (log-correction and linear-correction) based on the relationship between energy and timing information were purposed. As a comparison, the SiPM arrays coupled to 4 mm and 6 mm side crystal cube without optical glue were tested for coincidence timing resolution (CTR). The mean and standard deviations (SD) of dark current for the 1536 tested SiPMs were 12.72 +/- 1.70 μA at the bias voltage of 31.5 V and the temperature of 20 °C (±1 °C). CTR performance has increased by ∼5% within a narrow energy window, and ∼10% in a wide energy window by log-correction. The mean and SD of the CTR of 6 mm side crystal cube glue coupled was 126.9 +/- 3.6 ps for the 768 pairs of tested SiPMs. The detector is expected to provide a technical reference for the next generation of ultra-fast CTR commercial PET scanner using multilayer detectors.</abstract><pub>Elsevier B.V</pub><pmid>33132469</pmid><doi>10.1016/j.nima.2019.03.083</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Coincidence events Dark current Energy resolution Positron emission tomography Time resolution TOF PET |
title | PET detectors with 127 ps CTR for the Tachyon-II time-of-flight PET scanner |
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