原子能科学技术
原子能科學技術
원자능과학기술
ATOMIC ENERGY SCIENCE AND TECHNOLOGY
2014年
1期
137-141
,共5页
龙斌%吴睿%成智威%冯天成%庞璐%申茂泉
龍斌%吳睿%成智威%馮天成%龐璐%申茂泉
룡빈%오예%성지위%풍천성%방로%신무천
放射性氙测量%模拟校准%现场视察
放射性氙測量%模擬校準%現場視察
방사성선측량%모의교준%현장시찰
measurement of radio-xenon%model-based calibration%on-site inspection
基于禁核试核查现场视察的需求,研制了用于放射性氙测量的模拟气体源,实现了133 Xe 81.0 keVγ射线的效率校准。放射源基质为聚苯乙烯泡沫颗粒,母体核素为226 Ra ,采用不锈钢外壳封装,同时采用碳纤维窗以减少射线的衰减。放射源研制完成后,对其进行气密性和均匀性检验。当放射源达到平衡后,测量214 Pb的特征X射线的探测效率,然后插值计算得到133 Xe 81.0 keV γ射线的探测效率。为检验校准结果的正确性,制作了一个基质和几何尺寸均与226 Ra源相同的155 Eu放射源,并在相同测量条件进行了实验。结果表明,155 Eu 86.5 keV γ射线和214 Pb 87.3 keV X射线的探测效率之间的相对偏差小于1.0%。
基于禁覈試覈查現場視察的需求,研製瞭用于放射性氙測量的模擬氣體源,實現瞭133 Xe 81.0 keVγ射線的效率校準。放射源基質為聚苯乙烯泡沫顆粒,母體覈素為226 Ra ,採用不鏽鋼外殼封裝,同時採用碳纖維窗以減少射線的衰減。放射源研製完成後,對其進行氣密性和均勻性檢驗。噹放射源達到平衡後,測量214 Pb的特徵X射線的探測效率,然後插值計算得到133 Xe 81.0 keV γ射線的探測效率。為檢驗校準結果的正確性,製作瞭一箇基質和幾何呎吋均與226 Ra源相同的155 Eu放射源,併在相同測量條件進行瞭實驗。結果錶明,155 Eu 86.5 keV γ射線和214 Pb 87.3 keV X射線的探測效率之間的相對偏差小于1.0%。
기우금핵시핵사현장시찰적수구,연제료용우방사성선측량적모의기체원,실현료133 Xe 81.0 keVγ사선적효솔교준。방사원기질위취분을희포말과립,모체핵소위226 Ra ,채용불수강외각봉장,동시채용탄섬유창이감소사선적쇠감。방사원연제완성후,대기진행기밀성화균균성검험。당방사원체도평형후,측량214 Pb적특정X사선적탐측효솔,연후삽치계산득도133 Xe 81.0 keV γ사선적탐측효솔。위검험교준결과적정학성,제작료일개기질화궤하척촌균여226 Ra원상동적155 Eu방사원,병재상동측량조건진행료실험。결과표명,155 Eu 86.5 keV γ사선화214 Pb 87.3 keV X사선적탐측효솔지간적상대편차소우1.0%。
In order to satisfy the need of OSI (on-site inspection) ,the equivalent gas radioactive source was developed ,which was used to implement the efficiency calibration for 133 Xe 81.0 keV γ-ray .The radioactive source was composed of foam grains as matrix material and 226 Ra as parent nuclide ,and encapsulated by stainless steel and carbon fiber window to decrease the attenuation of γ-ray . The experiments on tightness and uniformity were done after the source was manufactured . When the source became equilibrium between 226 Ra and 214 Pb ,the efficiencies of X-ray of 214 Pb were measured . Then the interpolation calculation with determination values was done to obtain the efficiency of 133Xe 81.0 keV γ-ray .To verify the accuracy of calibration results ,the experiment was finished on the same measurement conditions with a 155 Eu source whose matrix and geometry dimensions were the same as 226 Ra source .The result indicates that the relative deviation of detection efficiency between 155 Eu 86.5 keV γ-ray and 214 Pb 87.3 keV X-ray is less than 1.0% .