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中国科学院 西安光学精密机械研究所,陕西 西安,710119
收稿日期:2012-07-04,
修回日期:2012-09-25,
纸质出版日期:2012-11-10
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闫亚东, 何俊华. 聚变反应速率测量光学系统设计[J]. 光学精密工程, 2012,20(11): 2389-2394
YAN Ya-dong, HE Jun-hua. Design of optical system for fusion reaction-rate measurement[J]. Editorial Office of Optics and Precision Engineering, 2012,20(11): 2389-2394
闫亚东, 何俊华. 聚变反应速率测量光学系统设计[J]. 光学精密工程, 2012,20(11): 2389-2394 DOI: 10.3788/OPE.20122011.2389.
YAN Ya-dong, HE Jun-hua. Design of optical system for fusion reaction-rate measurement[J]. Editorial Office of Optics and Precision Engineering, 2012,20(11): 2389-2394 DOI: 10.3788/OPE.20122011.2389.
基于塑料闪烁体和条纹相机设计了聚变反应速率测量系统
论述了测量光学系统的工作原理和设计方法。通过设置防辐射石英玻璃窗
防止了光学元件受强X射线辐射而变暗;采用晶体等紫外透过率高的光学材料
满足了光学系统对透过率的要求;光学系统像面与条纹相机的阴极面直接对接
解决了条纹相机孔径不匹配的问题;最后在一次像面设置场镜
大幅缩小了光学元件的口径。设计的光学系统总长为2 660 mm
放大倍率为1/3
像方
F
/#数达到0.667
系统透过率达到67%
时间弥散小于7.3 ps。这些结果能够适应不同中子产额的实验需求
在激光打靶实验中取得了较好的实验效果。
Based on a plastic scintillator and an optic streak camera
a measuring system for fusion reaction-rate was designed
then the working princile and design method of the measuring system were addressed in detail. A piece of fused silica window was set just behind the plastic scintillator to protect optical elements from darkening after a long time exposure in scatted X rays and the ultraviolet crystals and other ultraviolet glass were selected to ensure the high system transmission. Furthermore
the image plane of the optical system was put onto a photocathode of the streak camera directly to remove the aperture non-matching of input optic system of the streak camera. Finally
a field mirror was put on the first image plane to reduce the max diameter of optical element from 160 mm to 120 mm. The designed optical system has a total length of 2 660 mm
magnification of 3∶1 and its final lens is
F
/0.667 and transmission is 67%. Moreover
the time dispersion of the optical system is less than 7.3 ps. These results meet the experimental needs of different neutron yields and good experimental results have been obtained in a laser targeting experiment.
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