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 inChinese physics C Vol. 35; no. 11; pp. 1070 - 1073
Main Author 廖燕飞 章志明 李道武 帅磊 单保慈 黄先超 刘军辉 陈研 王英杰 刘双全 王培林 魏书军 魏龙
Format Journal Article
LanguageEnglish
Published IOP Publishing 01.11.2011
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ISSN1674-1137
0254-3052
2058-6132
DOI10.1088/1674-1137/35/11/017

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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.
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
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ISSN:1674-1137
0254-3052
2058-6132
DOI:10.1088/1674-1137/35/11/017