西南科技大学学报
西南科技大學學報
서남과기대학학보
Journal of Southwest University of Science and Technology
2015年
3期
94-98
,共5页
王树青%廖鹏%彭丽%杨超%印茂伟
王樹青%廖鵬%彭麗%楊超%印茂偉
왕수청%료붕%팽려%양초%인무위
介质壁加速器%电磁粒子模拟%质子治疗
介質壁加速器%電磁粒子模擬%質子治療
개질벽가속기%전자입자모의%질자치료
Dielectric wall accelerator%Particle-in-cell simulation%Proton therapy
采用自主开发的电磁粒子模拟软件对中国工程物理研究院研制的1 MeV介质壁质子加速器进行数值仿真,并对影响介质壁加速器的主要参数进行了系统分析,得到了可靠的优化方案. 模拟结果显示:保持加速梯度20 MV/m的情况下,HGI越厚,得到的束流能量峰值越高,束流值越大,需综合考虑加速器尺寸和所需的束流和束能,以选取合适的HGI厚度;峰值电流随加速梯度的减小而增大,即在特定要求,可以通过损失部分加速梯度得到更大的输出电流;输出束流峰值随输入电流大小线性增长,且输入束流每增加3 mA,对应输出峰值增加0.12 A,增长比率为1:40;输出束流峰值随输入束流半径的增加而减少,随法兰内半径的增大而增加;随着延时间距的增大,束流先增大后减小,最佳延时为21,21.5,21.7 ns,且电流值为不考虑延时的1.73倍.
採用自主開髮的電磁粒子模擬軟件對中國工程物理研究院研製的1 MeV介質壁質子加速器進行數值倣真,併對影響介質壁加速器的主要參數進行瞭繫統分析,得到瞭可靠的優化方案. 模擬結果顯示:保持加速梯度20 MV/m的情況下,HGI越厚,得到的束流能量峰值越高,束流值越大,需綜閤攷慮加速器呎吋和所需的束流和束能,以選取閤適的HGI厚度;峰值電流隨加速梯度的減小而增大,即在特定要求,可以通過損失部分加速梯度得到更大的輸齣電流;輸齣束流峰值隨輸入電流大小線性增長,且輸入束流每增加3 mA,對應輸齣峰值增加0.12 A,增長比率為1:40;輸齣束流峰值隨輸入束流半徑的增加而減少,隨法蘭內半徑的增大而增加;隨著延時間距的增大,束流先增大後減小,最佳延時為21,21.5,21.7 ns,且電流值為不攷慮延時的1.73倍.
채용자주개발적전자입자모의연건대중국공정물리연구원연제적1 MeV개질벽질자가속기진행수치방진,병대영향개질벽가속기적주요삼수진행료계통분석,득도료가고적우화방안. 모의결과현시:보지가속제도20 MV/m적정황하,HGI월후,득도적속류능량봉치월고,속류치월대,수종합고필가속기척촌화소수적속류화속능,이선취합괄적HGI후도;봉치전류수가속제도적감소이증대,즉재특정요구,가이통과손실부분가속제도득도경대적수출전류;수출속류봉치수수입전류대소선성증장,차수입속류매증가3 mA,대응수출봉치증가0.12 A,증장비솔위1:40;수출속류봉치수수입속류반경적증가이감소,수법란내반경적증대이증가;수착연시간거적증대,속류선증대후감소,최가연시위21,21.5,21.7 ns,차전류치위불고필연시적1.73배.
In this paper , 1 MeV dielectric wall proton accelerator which is developed by China Academy of Engineering Physics was numerically simulated by the self -developed electromagnetic particle simulation software .A reliable optimization scheme was obtained after the system analyzing of its major parameters . The simulation results are the following:With the accelerating gradient of 20 MV/m, the thicker the HGI is, the higher beam energy peak and beam value become .Accelerator's size, the needed beam and beam energy should be considered synthetically in order to choose a suitable thick of HGI .The peak current in-creases with the accelerating gradient decreasing , which means larger output current would be obtained by losing part of accelerating gradient in the specific requirements .The output beam peak grows linearly with the input current and when the input current increases by every 3 mA, the output beam peak increases by 0.12 A, in which growth rate is 1:40.The output beam peak decreases with the input beam radius in-creasing and increases with the flange inner radius increasing .With the rise of delay interval , the beam current increases first and then decreases .The optimal delay are 21, 21.5, 21.7 ns and the current is 1.73 times the value of the one without considering the delay .