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Positron emission tomography detector performance with different crystal pitches
Aims: In this work, we evaluated the performance of three pitches positron emission tomography (PET) detectors for building a high-resolution small-animal PET imaging experimental platform. Methods: The evaluation of PET detectors includes two-dimensional crystal identification, energy resolution, a...
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Published in: | Radiation detection technology and methods 2017-12, Vol.1 (2), Article 24 |
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container_title | Radiation detection technology and methods |
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creator | Tong, LinGe Fan, YaMing Dong, Ming Zhao, Liang Li, ZhongXing Li, YingGuo Wang, TianQuan Yin, YongZhi Chen, XiMeng |
description | Aims:
In this work, we evaluated the performance of three pitches positron emission tomography (PET) detectors for building a high-resolution small-animal PET imaging experimental platform.
Methods:
The evaluation of PET detectors includes two-dimensional crystal identification, energy resolution, and crystal look-up table. The nuclear instrumentation module and PXI data acquisition (DAQ) system were both used to obtain flood images. The energy spectrum of the Na-22 source was measured. PET detectors of 2.0 and 1.6 mm pitches used in our present experiment were composed of lutetium yttrium oxyorthosilicate (LYSO) crystals directly coupled to position-sensitive photomultiplier tubes (PSPMTs). The 1.3-mm pitch detector comprises a LYSO crystal, a tapered light-guide, and a PSPMT. The crystal sizes of the detectors were a
10
×
10
array of
2.0
×
2.0
×
10
mm
3
crystals, a
10
×
10
array of
1.6
×
1.6
×
10
mm
3
crystals, and an
18
×
18
array of
1.3
×
1.3
×
10
mm
3
crystals, respectively. Due to the lower sampling frequency of the DAQ system, a spline interpolation algorithm was introduced in the signal waveform to reconstruct the peak values.
Results:
The experimental results indicated that all three PET detector crystals could be clearly identified. A detailed analysis demonstrated that the key characteristic full width at half maximum (FWHM) values of the crystals profile could reach
0.46
±
0.03
,
0.32
±
0.03
, and
0.21
±
0.02
mm
, while the crystal average energy resolutions were
16.8
%
±
1.76
%
,
20.1
%
±
2.24
%
, and
31.5
%
±
3.76
%
, which correspond to pitches of 2.0-, 1.6-, and 1.3-mm, respectively.
Conclusions:
The PET detector modules of LYSO crystal arrays could be potentially used in the small-animal PET imaging applications and are promising to achieve sub-millimeter PET images. |
doi_str_mv | 10.1007/s41605-017-0026-y |
format | article |
fullrecord | <record><control><sourceid>crossref_sprin</sourceid><recordid>TN_cdi_crossref_primary_10_1007_s41605_017_0026_y</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1007_s41605_017_0026_y</sourcerecordid><originalsourceid>FETCH-LOGICAL-c288t-f1325c8f245d137ee6536b485bcfd0090be3f336d6f4197d90e87b57fffb68ed3</originalsourceid><addsrcrecordid>eNp9kMtqwzAQRUVpoSHNB3SnH1A7sizJXpbQFwSaRbsWtjxKFGLLSCrFf1-HlC6zmru45zIcQu45PHAA_ZhKrkAy4JoBFIpNV2RRSKhZXZf19X8WcEtWKR1gLmlRVqAXZLsNyecYBoq9T8nPIYc-7GIz7ifaYUabQ6QjRhdi3wwW6Y_Pe9p55zDikKmNU8rNkY4-2z2mO3LjmmPC1d9dkq-X58_1G9t8vL6vnzbMFlWVmeOikLZyRSk7LjSikkK1ZSVb6zqAGloUTgjVKVfyWnc1YKVbqZ1zraqwE0vCz7s2hpQiOjNG3zdxMhzMyYo5WzGzFXOyYqaZKc5MmrvDDqM5hO84zG9egH4Bpt9nww</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Positron emission tomography detector performance with different crystal pitches</title><source>Springer Nature</source><creator>Tong, LinGe ; Fan, YaMing ; Dong, Ming ; Zhao, Liang ; Li, ZhongXing ; Li, YingGuo ; Wang, TianQuan ; Yin, YongZhi ; Chen, XiMeng</creator><creatorcontrib>Tong, LinGe ; Fan, YaMing ; Dong, Ming ; Zhao, Liang ; Li, ZhongXing ; Li, YingGuo ; Wang, TianQuan ; Yin, YongZhi ; Chen, XiMeng</creatorcontrib><description>Aims:
In this work, we evaluated the performance of three pitches positron emission tomography (PET) detectors for building a high-resolution small-animal PET imaging experimental platform.
Methods:
The evaluation of PET detectors includes two-dimensional crystal identification, energy resolution, and crystal look-up table. The nuclear instrumentation module and PXI data acquisition (DAQ) system were both used to obtain flood images. The energy spectrum of the Na-22 source was measured. PET detectors of 2.0 and 1.6 mm pitches used in our present experiment were composed of lutetium yttrium oxyorthosilicate (LYSO) crystals directly coupled to position-sensitive photomultiplier tubes (PSPMTs). The 1.3-mm pitch detector comprises a LYSO crystal, a tapered light-guide, and a PSPMT. The crystal sizes of the detectors were a
10
×
10
array of
2.0
×
2.0
×
10
mm
3
crystals, a
10
×
10
array of
1.6
×
1.6
×
10
mm
3
crystals, and an
18
×
18
array of
1.3
×
1.3
×
10
mm
3
crystals, respectively. Due to the lower sampling frequency of the DAQ system, a spline interpolation algorithm was introduced in the signal waveform to reconstruct the peak values.
Results:
The experimental results indicated that all three PET detector crystals could be clearly identified. A detailed analysis demonstrated that the key characteristic full width at half maximum (FWHM) values of the crystals profile could reach
0.46
±
0.03
,
0.32
±
0.03
, and
0.21
±
0.02
mm
, while the crystal average energy resolutions were
16.8
%
±
1.76
%
,
20.1
%
±
2.24
%
, and
31.5
%
±
3.76
%
, which correspond to pitches of 2.0-, 1.6-, and 1.3-mm, respectively.
Conclusions:
The PET detector modules of LYSO crystal arrays could be potentially used in the small-animal PET imaging applications and are promising to achieve sub-millimeter PET images.</description><identifier>ISSN: 2509-9930</identifier><identifier>EISSN: 2509-9949</identifier><identifier>DOI: 10.1007/s41605-017-0026-y</identifier><language>eng</language><publisher>Singapore: Springer Singapore</publisher><subject>Beam Physics ; Hadrons ; Heavy Ions ; Nuclear Energy ; Nuclear Physics ; Original Paper ; Particle Acceleration and Detection ; Physics ; Physics and Astronomy</subject><ispartof>Radiation detection technology and methods, 2017-12, Vol.1 (2), Article 24</ispartof><rights>Institute of High Energy Physics, Chinese Academy of Sciences; China Nuclear Electronics and Nuclear Detection Society and Springer Nature Singapore Pte Ltd. 2017</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c288t-f1325c8f245d137ee6536b485bcfd0090be3f336d6f4197d90e87b57fffb68ed3</citedby><cites>FETCH-LOGICAL-c288t-f1325c8f245d137ee6536b485bcfd0090be3f336d6f4197d90e87b57fffb68ed3</cites><orcidid>0000-0002-1101-8121</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Tong, LinGe</creatorcontrib><creatorcontrib>Fan, YaMing</creatorcontrib><creatorcontrib>Dong, Ming</creatorcontrib><creatorcontrib>Zhao, Liang</creatorcontrib><creatorcontrib>Li, ZhongXing</creatorcontrib><creatorcontrib>Li, YingGuo</creatorcontrib><creatorcontrib>Wang, TianQuan</creatorcontrib><creatorcontrib>Yin, YongZhi</creatorcontrib><creatorcontrib>Chen, XiMeng</creatorcontrib><title>Positron emission tomography detector performance with different crystal pitches</title><title>Radiation detection technology and methods</title><addtitle>Radiat Detect Technol Methods</addtitle><description>Aims:
In this work, we evaluated the performance of three pitches positron emission tomography (PET) detectors for building a high-resolution small-animal PET imaging experimental platform.
Methods:
The evaluation of PET detectors includes two-dimensional crystal identification, energy resolution, and crystal look-up table. The nuclear instrumentation module and PXI data acquisition (DAQ) system were both used to obtain flood images. The energy spectrum of the Na-22 source was measured. PET detectors of 2.0 and 1.6 mm pitches used in our present experiment were composed of lutetium yttrium oxyorthosilicate (LYSO) crystals directly coupled to position-sensitive photomultiplier tubes (PSPMTs). The 1.3-mm pitch detector comprises a LYSO crystal, a tapered light-guide, and a PSPMT. The crystal sizes of the detectors were a
10
×
10
array of
2.0
×
2.0
×
10
mm
3
crystals, a
10
×
10
array of
1.6
×
1.6
×
10
mm
3
crystals, and an
18
×
18
array of
1.3
×
1.3
×
10
mm
3
crystals, respectively. Due to the lower sampling frequency of the DAQ system, a spline interpolation algorithm was introduced in the signal waveform to reconstruct the peak values.
Results:
The experimental results indicated that all three PET detector crystals could be clearly identified. A detailed analysis demonstrated that the key characteristic full width at half maximum (FWHM) values of the crystals profile could reach
0.46
±
0.03
,
0.32
±
0.03
, and
0.21
±
0.02
mm
, while the crystal average energy resolutions were
16.8
%
±
1.76
%
,
20.1
%
±
2.24
%
, and
31.5
%
±
3.76
%
, which correspond to pitches of 2.0-, 1.6-, and 1.3-mm, respectively.
Conclusions:
The PET detector modules of LYSO crystal arrays could be potentially used in the small-animal PET imaging applications and are promising to achieve sub-millimeter PET images.</description><subject>Beam Physics</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Nuclear Energy</subject><subject>Nuclear Physics</subject><subject>Original Paper</subject><subject>Particle Acceleration and Detection</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><issn>2509-9930</issn><issn>2509-9949</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNp9kMtqwzAQRUVpoSHNB3SnH1A7sizJXpbQFwSaRbsWtjxKFGLLSCrFf1-HlC6zmru45zIcQu45PHAA_ZhKrkAy4JoBFIpNV2RRSKhZXZf19X8WcEtWKR1gLmlRVqAXZLsNyecYBoq9T8nPIYc-7GIz7ifaYUabQ6QjRhdi3wwW6Y_Pe9p55zDikKmNU8rNkY4-2z2mO3LjmmPC1d9dkq-X58_1G9t8vL6vnzbMFlWVmeOikLZyRSk7LjSikkK1ZSVb6zqAGloUTgjVKVfyWnc1YKVbqZ1zraqwE0vCz7s2hpQiOjNG3zdxMhzMyYo5WzGzFXOyYqaZKc5MmrvDDqM5hO84zG9egH4Bpt9nww</recordid><startdate>20171201</startdate><enddate>20171201</enddate><creator>Tong, LinGe</creator><creator>Fan, YaMing</creator><creator>Dong, Ming</creator><creator>Zhao, Liang</creator><creator>Li, ZhongXing</creator><creator>Li, YingGuo</creator><creator>Wang, TianQuan</creator><creator>Yin, YongZhi</creator><creator>Chen, XiMeng</creator><general>Springer Singapore</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-1101-8121</orcidid></search><sort><creationdate>20171201</creationdate><title>Positron emission tomography detector performance with different crystal pitches</title><author>Tong, LinGe ; Fan, YaMing ; Dong, Ming ; Zhao, Liang ; Li, ZhongXing ; Li, YingGuo ; Wang, TianQuan ; Yin, YongZhi ; Chen, XiMeng</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c288t-f1325c8f245d137ee6536b485bcfd0090be3f336d6f4197d90e87b57fffb68ed3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Beam Physics</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Nuclear Energy</topic><topic>Nuclear Physics</topic><topic>Original Paper</topic><topic>Particle Acceleration and Detection</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tong, LinGe</creatorcontrib><creatorcontrib>Fan, YaMing</creatorcontrib><creatorcontrib>Dong, Ming</creatorcontrib><creatorcontrib>Zhao, Liang</creatorcontrib><creatorcontrib>Li, ZhongXing</creatorcontrib><creatorcontrib>Li, YingGuo</creatorcontrib><creatorcontrib>Wang, TianQuan</creatorcontrib><creatorcontrib>Yin, YongZhi</creatorcontrib><creatorcontrib>Chen, XiMeng</creatorcontrib><collection>CrossRef</collection><jtitle>Radiation detection technology and methods</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tong, LinGe</au><au>Fan, YaMing</au><au>Dong, Ming</au><au>Zhao, Liang</au><au>Li, ZhongXing</au><au>Li, YingGuo</au><au>Wang, TianQuan</au><au>Yin, YongZhi</au><au>Chen, XiMeng</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Positron emission tomography detector performance with different crystal pitches</atitle><jtitle>Radiation detection technology and methods</jtitle><stitle>Radiat Detect Technol Methods</stitle><date>2017-12-01</date><risdate>2017</risdate><volume>1</volume><issue>2</issue><artnum>24</artnum><issn>2509-9930</issn><eissn>2509-9949</eissn><abstract>Aims:
In this work, we evaluated the performance of three pitches positron emission tomography (PET) detectors for building a high-resolution small-animal PET imaging experimental platform.
Methods:
The evaluation of PET detectors includes two-dimensional crystal identification, energy resolution, and crystal look-up table. The nuclear instrumentation module and PXI data acquisition (DAQ) system were both used to obtain flood images. The energy spectrum of the Na-22 source was measured. PET detectors of 2.0 and 1.6 mm pitches used in our present experiment were composed of lutetium yttrium oxyorthosilicate (LYSO) crystals directly coupled to position-sensitive photomultiplier tubes (PSPMTs). The 1.3-mm pitch detector comprises a LYSO crystal, a tapered light-guide, and a PSPMT. The crystal sizes of the detectors were a
10
×
10
array of
2.0
×
2.0
×
10
mm
3
crystals, a
10
×
10
array of
1.6
×
1.6
×
10
mm
3
crystals, and an
18
×
18
array of
1.3
×
1.3
×
10
mm
3
crystals, respectively. Due to the lower sampling frequency of the DAQ system, a spline interpolation algorithm was introduced in the signal waveform to reconstruct the peak values.
Results:
The experimental results indicated that all three PET detector crystals could be clearly identified. A detailed analysis demonstrated that the key characteristic full width at half maximum (FWHM) values of the crystals profile could reach
0.46
±
0.03
,
0.32
±
0.03
, and
0.21
±
0.02
mm
, while the crystal average energy resolutions were
16.8
%
±
1.76
%
,
20.1
%
±
2.24
%
, and
31.5
%
±
3.76
%
, which correspond to pitches of 2.0-, 1.6-, and 1.3-mm, respectively.
Conclusions:
The PET detector modules of LYSO crystal arrays could be potentially used in the small-animal PET imaging applications and are promising to achieve sub-millimeter PET images.</abstract><cop>Singapore</cop><pub>Springer Singapore</pub><doi>10.1007/s41605-017-0026-y</doi><orcidid>https://orcid.org/0000-0002-1101-8121</orcidid></addata></record> |
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language | eng |
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source | Springer Nature |
subjects | Beam Physics Hadrons Heavy Ions Nuclear Energy Nuclear Physics Original Paper Particle Acceleration and Detection Physics Physics and Astronomy |
title | Positron emission tomography detector performance with different crystal pitches |
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