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8-Layer DOI Encoding of 3-Dimensional Crystal Array
An 8-layer depth of interaction (DOI) detector was designed based on the technique we have developed for 4-layer DOI detectors. The new detector achieves 8-layer DOI encoding by pulse shape discrimination (2-layer DOI encoding) and an optimized reflector arrangement in a 3-dimensional crystal array...
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Published in: | IEEE transactions on nuclear science 2006-10, Vol.53 (5), p.2523-2528 |
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description | An 8-layer depth of interaction (DOI) detector was designed based on the technique we have developed for 4-layer DOI detectors. The new detector achieves 8-layer DOI encoding by pulse shape discrimination (2-layer DOI encoding) and an optimized reflector arrangement in a 3-dimensional crystal array (4-layer DOI encoding). Its capability was proved with an 8-layer 10times10 Gd 2 SiO 5 (GSO) crystal array coupled to a 256-channel flat panel position sensitive photomultiplier tube (256ch FP-PMT). The dimensions of each crystal element were 2.90 mmtimes2.90 mmtimes3.75 mm and the interval between 16times16 multi anodes in the 256ch FP-PMT was 3.04 mm. Two different dopant concentrations in GSO were chosen for pulse shape discrimination: GSO crystals of 0.5 mol% and 1.5 mol% Ce dopant that have 60 ns and 35 ns scintillation decay times, respectively. In the crystal array, Layer-1, the farthest from the 256ch FP-PMT, and Layers-3, -5 and -7 were composed of GSO crystals of 0.5 mol% Ce dopant. All other layers were composed of GSO crystals of 1.5 mol% Ce dopant. Performance of the 8-layer DOI detector was evaluated by irradiating with 662 keV uniform gamma-rays and the capability was judged to be good. To prove the validity of the layer encoding, a fan-beam of 662 keV gamma-rays was irradiated onto the side face of each layer. The obtained 2-dimensional position histograms showed the right structure in each corresponding layer clearly. Light output uniformity among DOI layers and energy resolutions were measured on the pulse height distributions of the central crystal in each layer. The crystals in Layer-2 and Layer-3 showed the smallest light output and their full energy peak channels were 62% to the largest peak channel of the Layer-8 crystal distribution. Energy resolutions were about 15% for all eight layers |
doi_str_mv | 10.1109/TNS.2006.882795 |
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The new detector achieves 8-layer DOI encoding by pulse shape discrimination (2-layer DOI encoding) and an optimized reflector arrangement in a 3-dimensional crystal array (4-layer DOI encoding). Its capability was proved with an 8-layer 10times10 Gd 2 SiO 5 (GSO) crystal array coupled to a 256-channel flat panel position sensitive photomultiplier tube (256ch FP-PMT). The dimensions of each crystal element were 2.90 mmtimes2.90 mmtimes3.75 mm and the interval between 16times16 multi anodes in the 256ch FP-PMT was 3.04 mm. Two different dopant concentrations in GSO were chosen for pulse shape discrimination: GSO crystals of 0.5 mol% and 1.5 mol% Ce dopant that have 60 ns and 35 ns scintillation decay times, respectively. In the crystal array, Layer-1, the farthest from the 256ch FP-PMT, and Layers-3, -5 and -7 were composed of GSO crystals of 0.5 mol% Ce dopant. All other layers were composed of GSO crystals of 1.5 mol% Ce dopant. Performance of the 8-layer DOI detector was evaluated by irradiating with 662 keV uniform gamma-rays and the capability was judged to be good. To prove the validity of the layer encoding, a fan-beam of 662 keV gamma-rays was irradiated onto the side face of each layer. The obtained 2-dimensional position histograms showed the right structure in each corresponding layer clearly. Light output uniformity among DOI layers and energy resolutions were measured on the pulse height distributions of the central crystal in each layer. The crystals in Layer-2 and Layer-3 showed the smallest light output and their full energy peak channels were 62% to the largest peak channel of the Layer-8 crystal distribution. Energy resolutions were about 15% for all eight layers</description><identifier>ISSN: 0018-9499</identifier><identifier>EISSN: 1558-1578</identifier><identifier>DOI: 10.1109/TNS.2006.882795</identifier><identifier>CODEN: IETNAE</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Anodes ; Arrays ; Channels ; Crystals ; Depth of interaction (DOI) ; Detectors ; Dopants ; Encoding ; Energy resolution ; GSO ; Photomultipliers ; positron emission tomography (PET) ; Pulse measurements ; Pulse shape ; Pulse shaping methods ; Sensor arrays ; Shape</subject><ispartof>IEEE transactions on nuclear science, 2006-10, Vol.53 (5), p.2523-2528</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2006</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c364t-4886716fdde0a6c8385899c405008c738d2dc5a47cf395dce056e581858598d33</citedby><cites>FETCH-LOGICAL-c364t-4886716fdde0a6c8385899c405008c738d2dc5a47cf395dce056e581858598d33</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1710233$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,27903,27904,54775</link.rule.ids></links><search><creatorcontrib>Inadama, N.</creatorcontrib><creatorcontrib>Murayama, H.</creatorcontrib><creatorcontrib>Hamamoto, M.</creatorcontrib><creatorcontrib>Tsuda, T.</creatorcontrib><creatorcontrib>Ono, Y.</creatorcontrib><creatorcontrib>Yamaya, T.</creatorcontrib><creatorcontrib>Yoshida, E.</creatorcontrib><creatorcontrib>Shibuya, K.</creatorcontrib><creatorcontrib>Nishikido, F.</creatorcontrib><title>8-Layer DOI Encoding of 3-Dimensional Crystal Array</title><title>IEEE transactions on nuclear science</title><addtitle>TNS</addtitle><description>An 8-layer depth of interaction (DOI) detector was designed based on the technique we have developed for 4-layer DOI detectors. The new detector achieves 8-layer DOI encoding by pulse shape discrimination (2-layer DOI encoding) and an optimized reflector arrangement in a 3-dimensional crystal array (4-layer DOI encoding). Its capability was proved with an 8-layer 10times10 Gd 2 SiO 5 (GSO) crystal array coupled to a 256-channel flat panel position sensitive photomultiplier tube (256ch FP-PMT). The dimensions of each crystal element were 2.90 mmtimes2.90 mmtimes3.75 mm and the interval between 16times16 multi anodes in the 256ch FP-PMT was 3.04 mm. Two different dopant concentrations in GSO were chosen for pulse shape discrimination: GSO crystals of 0.5 mol% and 1.5 mol% Ce dopant that have 60 ns and 35 ns scintillation decay times, respectively. In the crystal array, Layer-1, the farthest from the 256ch FP-PMT, and Layers-3, -5 and -7 were composed of GSO crystals of 0.5 mol% Ce dopant. All other layers were composed of GSO crystals of 1.5 mol% Ce dopant. Performance of the 8-layer DOI detector was evaluated by irradiating with 662 keV uniform gamma-rays and the capability was judged to be good. To prove the validity of the layer encoding, a fan-beam of 662 keV gamma-rays was irradiated onto the side face of each layer. The obtained 2-dimensional position histograms showed the right structure in each corresponding layer clearly. Light output uniformity among DOI layers and energy resolutions were measured on the pulse height distributions of the central crystal in each layer. The crystals in Layer-2 and Layer-3 showed the smallest light output and their full energy peak channels were 62% to the largest peak channel of the Layer-8 crystal distribution. Energy resolutions were about 15% for all eight layers</description><subject>Anodes</subject><subject>Arrays</subject><subject>Channels</subject><subject>Crystals</subject><subject>Depth of interaction (DOI)</subject><subject>Detectors</subject><subject>Dopants</subject><subject>Encoding</subject><subject>Energy resolution</subject><subject>GSO</subject><subject>Photomultipliers</subject><subject>positron emission tomography (PET)</subject><subject>Pulse measurements</subject><subject>Pulse shape</subject><subject>Pulse shaping methods</subject><subject>Sensor arrays</subject><subject>Shape</subject><issn>0018-9499</issn><issn>1558-1578</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><recordid>eNpd0D1rwzAQBmBRWmj6MXfoYrp0cnKyJPs0hiRtA6EZms5CSHJxcKxUSgb_-8q4UOh0HDzvcbyEPFCYUgpytnv_mBYA5RSxqKS4IBMqBOZUVHhJJgAUc8mlvCY3Me7TygWICWGYb3TvQrbcrrNVZ7xtuq_M1xnLl83BdbHxnW6zRejjKc15CLq_I1e1bqO7_5235PNltVu85Zvt63ox3-SGlfyUc8SyomVtrQNdGmQoUErDQQCgqRjawhqheWVqJoU1DkTpBNLEhETL2C15Hu8eg_8-u3hShyYa17a6c_4claRS8sEn-fRP7v05pMcHVIDEgg5oNiITfIzB1eoYmoMOvaKghgpVqlANFaqxwpR4HBONc-5PVxQKxtgPnfBo9A</recordid><startdate>20061001</startdate><enddate>20061001</enddate><creator>Inadama, N.</creator><creator>Murayama, H.</creator><creator>Hamamoto, M.</creator><creator>Tsuda, T.</creator><creator>Ono, Y.</creator><creator>Yamaya, T.</creator><creator>Yoshida, E.</creator><creator>Shibuya, K.</creator><creator>Nishikido, F.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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The new detector achieves 8-layer DOI encoding by pulse shape discrimination (2-layer DOI encoding) and an optimized reflector arrangement in a 3-dimensional crystal array (4-layer DOI encoding). Its capability was proved with an 8-layer 10times10 Gd 2 SiO 5 (GSO) crystal array coupled to a 256-channel flat panel position sensitive photomultiplier tube (256ch FP-PMT). The dimensions of each crystal element were 2.90 mmtimes2.90 mmtimes3.75 mm and the interval between 16times16 multi anodes in the 256ch FP-PMT was 3.04 mm. Two different dopant concentrations in GSO were chosen for pulse shape discrimination: GSO crystals of 0.5 mol% and 1.5 mol% Ce dopant that have 60 ns and 35 ns scintillation decay times, respectively. In the crystal array, Layer-1, the farthest from the 256ch FP-PMT, and Layers-3, -5 and -7 were composed of GSO crystals of 0.5 mol% Ce dopant. All other layers were composed of GSO crystals of 1.5 mol% Ce dopant. Performance of the 8-layer DOI detector was evaluated by irradiating with 662 keV uniform gamma-rays and the capability was judged to be good. To prove the validity of the layer encoding, a fan-beam of 662 keV gamma-rays was irradiated onto the side face of each layer. The obtained 2-dimensional position histograms showed the right structure in each corresponding layer clearly. Light output uniformity among DOI layers and energy resolutions were measured on the pulse height distributions of the central crystal in each layer. The crystals in Layer-2 and Layer-3 showed the smallest light output and their full energy peak channels were 62% to the largest peak channel of the Layer-8 crystal distribution. Energy resolutions were about 15% for all eight layers</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TNS.2006.882795</doi><tpages>6</tpages></addata></record> |
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subjects | Anodes Arrays Channels Crystals Depth of interaction (DOI) Detectors Dopants Encoding Energy resolution GSO Photomultipliers positron emission tomography (PET) Pulse measurements Pulse shape Pulse shaping methods Sensor arrays Shape |
title | 8-Layer DOI Encoding of 3-Dimensional Crystal Array |
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