Preliminary study of depth of interaction measurement for a PET detector
In this work we studied the feasibility of detecting the depth of interaction (DOI) with two layers of crystal arrays of LYSO and BGO scintillators coupled to a position-sensitive photomultiplier tube (PS-PMT) R8900-C12. A front-end electronics was designed, with which we got different pulse shapes...
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| Published in | Chinese physics C Vol. 35; no. 11; pp. 1070 - 1073 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
IOP Publishing
01.11.2011
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| Subjects | |
| Online Access | Get full text |
| ISSN | 1674-1137 0254-3052 2058-6132 |
| DOI | 10.1088/1674-1137/35/11/017 |
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| Summary: | In this work we studied the feasibility of detecting the depth of interaction (DOI) with two layers of crystal arrays of LYSO and BGO scintillators coupled to a position-sensitive photomultiplier tube (PS-PMT) R8900-C12. A front-end electronics was designed, with which we got different pulse shapes for different crystals to obtain depth information. With the double integration method, we got the DOI histogram of a divided integration ratio of two crystals as the standard to determine the layer-of-interaction. The DOI accuracy, measured by scanning a 22Na slit source along the side of the module, was 98% for the LYSO layer and 95% for the BGO layer. The energy resolution at 511keV was 13.1% for LYSO and 17.1% for BGO. We obtained good crystal separation in 2D position histograms of both layers. These results could be useful in the manufacture of PET scanners with high spatial resolutions. |
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| Bibliography: | In this work we studied the feasibility of detecting the depth of interaction (DOI) with two layers of crystal arrays of LYSO and BGO scintillators coupled to a position-sensitive photomultiplier tube (PS-PMT) R8900-C12. A front-end electronics was designed, with which we got different pulse shapes for different crystals to obtain depth information. With the double integration method, we got the DOI histogram of a divided integration ratio of two crystals as the standard to determine the layer-of-interaction. The DOI accuracy, measured by scanning a 22Na slit source along the side of the module, was 98% for the LYSO layer and 95% for the BGO layer. The energy resolution at 511keV was 13.1% for LYSO and 17.1% for BGO. We obtained good crystal separation in 2D position histograms of both layers. These results could be useful in the manufacture of PET scanners with high spatial resolutions. 11-5641/O4 PET; detector; DOI; spatial resolution LIAO Yan-Fei 1,2,3 ZHANG Zhi-Ming 1,2 LI Dao-Wu 1,2 SHUAI Lei 1,2 SHAN Bao-Ci1,2 HUANG Xian-Chao 1,2,3 LIU Jun-Hui 1,2,3 CHEN Yan 1,2,3 WANG Ying-Jie 1,2,3 LIU Shuang-Quan 1,2,3 WANG Pei-Lin 1,2,3 WEI Shu-Jun1,2 WEI Long1,2;1) 1 Key Laboratory of Nuclear Analysis Techniques, Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China 2 Beijing Engineering Research Center of Radiographic Techniques and Equipment, Beijing 100049, China 3 Graduate University of Chinese Academy of Sciences, Beijing 100049, China ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
| ISSN: | 1674-1137 0254-3052 2058-6132 |
| DOI: | 10.1088/1674-1137/35/11/017 |