Hongwei Xie, Jinchuan Chen, Q. Yi, Faqiang Zhang, Linbo Li
{"title":"影响伽玛射线相机空间分辨率的主要因素评价","authors":"Hongwei Xie, Jinchuan Chen, Q. Yi, Faqiang Zhang, Linbo Li","doi":"10.4236/JASMI.2013.34029","DOIUrl":null,"url":null,"abstract":"The spatial resolution of the \ngamma-rays camera was measured on a60Co gamma-rays source with edge \nmethod. The gamma-rays camera is consisting with rays-fluorescence convertor, \noptical imaging system, MCP image intensifier, CCD camera, electronic control \nsystem and other devices, and is mainly used in the image diagnostics of the \nintense pulse radiation sources [1]. Due to the relatively big quantum \ndetective efficiency (DQE) and quantum gain of the gamma-rays, etc., the \nexperimental data were processed by averaging multiple images and fitting \ncurves. According to the experimental results, the spatial resolution MTF \n(modulation transfer function) at the 10% intensity was about 2lp/mm. Meanwhile, because of the relatively \nbig dispersion effects of the fluorescence transmissions in the scintillator \nand the optical imaging system, the maximal single-noise ratio (SNR) of the \ncamera was found to be about 5:1. In addition, the spatial resolution of the camera \nwas measured with pulse X-rays with 0.3MeV in average energy and exclusion of \nthe effects of secondary electrons from consideration. Accordingly, the spatial \nresolution MTF at the 10% intensity was about 5lp/mm. This could be an additional \nevidence to verify the effects of secondary electrons induced by the 1.25MeV gamma-rays in the scintillator \nupon the spatial resolution. Based on our analysis, the dispersion sizes of the \nsecondary electrons in the scintillator are about 0.4mm-0.6mm. Comparatively, as indicated by the \ndetailed analysis of the spatial resolutions of the MCP image intensifier and \nCCD devices, both of them have little effect on the spatial resolution of the \ngamma-rays camera that could be well neglected.","PeriodicalId":274168,"journal":{"name":"Image Quality and System Performance","volume":"73 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2013-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Evaluation of Major Factors Affecting Spatial Resolution of Gamma-Rays Camera\",\"authors\":\"Hongwei Xie, Jinchuan Chen, Q. Yi, Faqiang Zhang, Linbo Li\",\"doi\":\"10.4236/JASMI.2013.34029\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The spatial resolution of the \\ngamma-rays camera was measured on a60Co gamma-rays source with edge \\nmethod. The gamma-rays camera is consisting with rays-fluorescence convertor, \\noptical imaging system, MCP image intensifier, CCD camera, electronic control \\nsystem and other devices, and is mainly used in the image diagnostics of the \\nintense pulse radiation sources [1]. Due to the relatively big quantum \\ndetective efficiency (DQE) and quantum gain of the gamma-rays, etc., the \\nexperimental data were processed by averaging multiple images and fitting \\ncurves. According to the experimental results, the spatial resolution MTF \\n(modulation transfer function) at the 10% intensity was about 2lp/mm. Meanwhile, because of the relatively \\nbig dispersion effects of the fluorescence transmissions in the scintillator \\nand the optical imaging system, the maximal single-noise ratio (SNR) of the \\ncamera was found to be about 5:1. In addition, the spatial resolution of the camera \\nwas measured with pulse X-rays with 0.3MeV in average energy and exclusion of \\nthe effects of secondary electrons from consideration. Accordingly, the spatial \\nresolution MTF at the 10% intensity was about 5lp/mm. This could be an additional \\nevidence to verify the effects of secondary electrons induced by the 1.25MeV gamma-rays in the scintillator \\nupon the spatial resolution. Based on our analysis, the dispersion sizes of the \\nsecondary electrons in the scintillator are about 0.4mm-0.6mm. Comparatively, as indicated by the \\ndetailed analysis of the spatial resolutions of the MCP image intensifier and \\nCCD devices, both of them have little effect on the spatial resolution of the \\ngamma-rays camera that could be well neglected.\",\"PeriodicalId\":274168,\"journal\":{\"name\":\"Image Quality and System Performance\",\"volume\":\"73 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2013-10-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Image Quality and System Performance\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.4236/JASMI.2013.34029\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Image Quality and System Performance","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.4236/JASMI.2013.34029","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Evaluation of Major Factors Affecting Spatial Resolution of Gamma-Rays Camera
The spatial resolution of the
gamma-rays camera was measured on a60Co gamma-rays source with edge
method. The gamma-rays camera is consisting with rays-fluorescence convertor,
optical imaging system, MCP image intensifier, CCD camera, electronic control
system and other devices, and is mainly used in the image diagnostics of the
intense pulse radiation sources [1]. Due to the relatively big quantum
detective efficiency (DQE) and quantum gain of the gamma-rays, etc., the
experimental data were processed by averaging multiple images and fitting
curves. According to the experimental results, the spatial resolution MTF
(modulation transfer function) at the 10% intensity was about 2lp/mm. Meanwhile, because of the relatively
big dispersion effects of the fluorescence transmissions in the scintillator
and the optical imaging system, the maximal single-noise ratio (SNR) of the
camera was found to be about 5:1. In addition, the spatial resolution of the camera
was measured with pulse X-rays with 0.3MeV in average energy and exclusion of
the effects of secondary electrons from consideration. Accordingly, the spatial
resolution MTF at the 10% intensity was about 5lp/mm. This could be an additional
evidence to verify the effects of secondary electrons induced by the 1.25MeV gamma-rays in the scintillator
upon the spatial resolution. Based on our analysis, the dispersion sizes of the
secondary electrons in the scintillator are about 0.4mm-0.6mm. Comparatively, as indicated by the
detailed analysis of the spatial resolutions of the MCP image intensifier and
CCD devices, both of them have little effect on the spatial resolution of the
gamma-rays camera that could be well neglected.