Timing performance of two PET detector designs capable of time-of-flight and depth-of-interaction measurement: Phoswich and offset crystal layers

Chen-Ming Chang, C. Levin
{"title":"Timing performance of two PET detector designs capable of time-of-flight and depth-of-interaction measurement: Phoswich and offset crystal layers","authors":"Chen-Ming Chang, C. Levin","doi":"10.1109/NSSMIC.2016.8069400","DOIUrl":null,"url":null,"abstract":"PET detectors capable of measuring 511 keV photon time-of-fight (TOF) and depth-of-interaction (DOI) can improve resulting image quality and accuracy. In this work, we studied the timing performance of two TOF-DOI PET detector designs: (1) phoswich and (2) offset crystal arrays. The phoswich detector comprises a 3 × 3 × 20 mm<sup>3</sup> element made from a 3 × 3 × 10 mm<sup>3</sup> LYSO:Ce crystal with 42 ns decay time optically epoxied to a 3 × 3 × 10 mm<sup>3</sup> calcium co-doped LSO:Ce,Ca(0.4%) crystal with 33 ns decay time. The offset crystal block comprises a 4 × 4 array of 3 × 3 × 10 mm<sup>3</sup> LYSO crystals in the bottom layer and a 4 × 3 array of LYSO crystals of the same size in the top layer. The top array is offset by half pixel pitch from the bottom array. The coincidence timing resolution for photopeak events acquired by two opposing phoswich detectors ranges from 164.6 ± 0.9 ps to 183.1 ± 4.2 ps FWHM, depending on the interaction layer combinations between two identical, dual layer elements. The coincidence timing resolution for photopeak events acquired by the offset crystal layers against a reference detector comprising a single 3 × 3 × 20 mm<sup>3</sup> LYSO crystal ranges from 177.8 ps to 272.6 ps FWHM and averaged to 219.7 ± 35.5 ps FWHM. These results show that both designs are capable of TOF and DOI measurement.","PeriodicalId":184587,"journal":{"name":"2016 IEEE Nuclear Science Symposium, Medical Imaging Conference and Room-Temperature Semiconductor Detector Workshop (NSS/MIC/RTSD)","volume":"26 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2016 IEEE Nuclear Science Symposium, Medical Imaging Conference and Room-Temperature Semiconductor Detector Workshop (NSS/MIC/RTSD)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NSSMIC.2016.8069400","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

PET detectors capable of measuring 511 keV photon time-of-fight (TOF) and depth-of-interaction (DOI) can improve resulting image quality and accuracy. In this work, we studied the timing performance of two TOF-DOI PET detector designs: (1) phoswich and (2) offset crystal arrays. The phoswich detector comprises a 3 × 3 × 20 mm3 element made from a 3 × 3 × 10 mm3 LYSO:Ce crystal with 42 ns decay time optically epoxied to a 3 × 3 × 10 mm3 calcium co-doped LSO:Ce,Ca(0.4%) crystal with 33 ns decay time. The offset crystal block comprises a 4 × 4 array of 3 × 3 × 10 mm3 LYSO crystals in the bottom layer and a 4 × 3 array of LYSO crystals of the same size in the top layer. The top array is offset by half pixel pitch from the bottom array. The coincidence timing resolution for photopeak events acquired by two opposing phoswich detectors ranges from 164.6 ± 0.9 ps to 183.1 ± 4.2 ps FWHM, depending on the interaction layer combinations between two identical, dual layer elements. The coincidence timing resolution for photopeak events acquired by the offset crystal layers against a reference detector comprising a single 3 × 3 × 20 mm3 LYSO crystal ranges from 177.8 ps to 272.6 ps FWHM and averaged to 219.7 ± 35.5 ps FWHM. These results show that both designs are capable of TOF and DOI measurement.
查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
两种能够测量飞行时间和相互作用深度的PET探测器的定时性能:Phoswich和偏移晶体层
PET探测器能够测量511 keV光子的战斗时间(TOF)和相互作用深度(DOI),可以提高图像质量和精度。在这项工作中,我们研究了两种TOF-DOI PET探测器设计的时序性能:(1)光电开关和(2)偏移晶体阵列。该光电探测器由3 × 3 × 10 mm3 LYSO:Ce晶体制成的3 × 3 × 20 mm3元件组成,其衰减时间为42 ns,光学环氧化为3 × 3 × 10 mm3钙共掺杂LSO:Ce,Ca(0.4%)晶体,衰减时间为33 ns。偏移晶体块包括底层的4 × 4阵列的3 × 3 × 10 mm3 LYSO晶体和顶层相同尺寸的4 × 3 LYSO晶体。顶部数组与底部数组偏移半像素间距。两个相对的光电探测器获得的光峰事件的符合时间分辨率范围为164.6±0.9 ps至183.1±4.2 ps FWHM,这取决于两个相同的双层元件之间的相互作用层组合。偏移晶体层对由单个3 × 3 × 20 mm3 LYSO晶体组成的参考检测器获得的光峰事件的符合时间分辨率范围为177.8 ps至272.6 ps FWHM,平均为219.7±35.5 ps FWHM。这些结果表明,这两种设计都能够测量TOF和DOI。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
自引率
0.00%
发文量
0
期刊最新文献
Development of flexible, scalable, low cost readout for beam tests of the high granularity calorimeter for the CMS endcap Latest frontier technology and design of the ATLAS calorimeter trigger board dedicated to jet identification for the LHC run 3 The ATLAS tile calorimeter DCS for run 2 The phase-II ATLAS pixel tracker upgrade: Layout and mechanics Null-hypothesis testing using distance metrics for verification of arms-control treaties
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1