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本文针对激光等离子体X射线诊断的需求,设计开发了移位双光栅X射线谱仪. 该谱仪采用高线对密度和低线对密度的两种光栅组成移位双光栅作为核心衍射组件,高密度光栅能够提高中、高能区(1000-5000 eV)的能谱分辨率,低密度光栅足够满足低能区(100-1000 eV)测量的能谱分辨率要求,控制了低能区谱线的分布空间,保证足够的测量范围. 两种光栅相互配合实现了谱仪整体性能提升. 本文提出了移位双光栅X射线谱仪结构设计方法和参数指标,完成了移位双光栅X射线谱仪的集成调试和实验应用,获得了时间分辨的X光谱实验数据,测谱范围0.1-5.0 keV,谱分辨0.04 nm,时间分辨好于30 ps. 移位双光栅X射线谱仪可以最大程度地利用记录面的长度,实现高时间分辨和宽谱X射线测量.In inertial confined fusion (ICF) experiments, the temporal evolution of X-ray spectrum can provide important diagnostic information such as electron temperature and density on laser-plasma interaction. Accurate diagnostic requires a wide range of X-ray spectrum from several hundred eV to kilo eV to be measured with high temporal resolution. For traditional single grating spectrometer coupled with streak cameras, the limited recording length of streak cameras severely restricts measured X-ray spectral range in one laser shot. Here we design a shifted dual transmission grating (SDTG) spectrometer for laser-produced plasma X-ray diagnostics in ICF experiments which can provide wide-range X-ray spectrum measurement from 100 eV to 5 keV with high temporal and spectral resolution. This SDTG spectrometer comprises two X-ray gratings: one with high line density and the other with low line density. The high line density grating is used to measure X-ray spectrum from 1000 eV to 5000 eV and the low line density grating measures X-ray spectrum from 100 eV to 1000 eV respectively. These two kinds of X-ray gratings are arranged in a plane with their centers shifted by a certain distance. A shifted double slit component is designed according to the spatial positions of the two gratings and set in front of the photocathode in the streak camera to ensure that two sets of X-ray spectra by two shifted gratings are projected on the photocathode without overlapping. This novel SDTG-based X-ray spectrometer can take the most of recording panel space, offering a path to realize a high resolution and broad spectral ranges in diagnosing soft X-rays. In this paper, the design method and the technical data of the SDTG-based X-ray spectrometer are given. The SDTG-based X-ray spectrometer is integrated, debugged and used to measure X-ray pulse at SG-III prototype facility located in Laser Fusion Research Center of Chinese Academy of Engineering Physics. The time integral results are captured by the SDTG spectrometer in the ICF fluid RT experiments and time-resolved spectra are recorded in indirect drive implosion experiment. Experimental results show the SDTG-based X-ray spectrometer can capture X-ray spectrum ranging from 0.1 keV to 5 keV, with a spectral resolution of 0.04 nm and a temporal resolution of better than 30 ps. By fully utilizing limited recording length, the SDTG-based X-ray spectrometer can realize a wide range temporal X-ray spectrum measurement with enough spectral resolution and temporal resolution. This SDTG spectrometer is a good temporal X-ray diagnostic tool for ICF experiments and other high energy density physics experiments.
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Keywords:
- shifted dual transmission grating spectrometer /
- inertial confined fusion /
- diffraction efficiency /
- time-resolved spectrum
[1] Eagleton R T, James S F 2004 Rev. Sci. Instrum. 75 3969
[2] Yang J M, Ding Y N, Zhang W H, Zhang J Y, Zheng Z J 2003 Rev. Sci. Instrum. 74 4268
[3] Kumar D, Clayton D J, Parman M, Stutman D, Tritz K 2012 Rev. Sci. Instrum. 83 10E511
[4] Wang B Q, Wang C K, Yi T, Li T S, Li J, Zhu X L, Xie C Q, Liu S Y, Jiang S E, Ding Y K 2015 Acta Phot. Sin. 44 1030003 (in Chinese) [王保清, 王传珂, 易涛, 李廷帅, 李晋, 朱效立, 谢常青, 刘慎业, 江少恩, 丁永坤 2015 光子学报 44 1030003]
[5] He K, Yi T, Liu S Y, Niu J B, Chen B Q, Zhu X L 2014 Micronanoelect. Technol. 51 381 (in Chinese) [何宽, 易涛, 刘慎业, 牛洁斌, 陈宝钦, 朱效立 2014 微纳电子技术 51 381]
[6] Ma J, Xie C Q, Ye T C, Liu M 2010 Acta Phys. Sin. 59 2564 (in Chinese) [马杰, 谢常青, 叶甜春, 刘明 2010 59 2564]
[7] Kuang L, Cao L, Zhu X, Wu S, Wang Z, Wang C, Liu S, Jiang S, Ding Y, Xie C, Zheng J 2011 J. Opt. Lett. 36 3954
[8] Wang C K, Wang B Q, Yi T, Fan Q P, Kuang L Y, Li J, Li T S, Zhu X L, Liu S Y, Jiang G 2016 J. Mod. Opt. 63 261
[9] Wang B Q, Yi T, Wang C K, Zhu X L, Li T S, Li J, Liu S Y, Jiang S E, Ding Y K 2016 Plasma Sci. Technol. 18 781
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[1] Eagleton R T, James S F 2004 Rev. Sci. Instrum. 75 3969
[2] Yang J M, Ding Y N, Zhang W H, Zhang J Y, Zheng Z J 2003 Rev. Sci. Instrum. 74 4268
[3] Kumar D, Clayton D J, Parman M, Stutman D, Tritz K 2012 Rev. Sci. Instrum. 83 10E511
[4] Wang B Q, Wang C K, Yi T, Li T S, Li J, Zhu X L, Xie C Q, Liu S Y, Jiang S E, Ding Y K 2015 Acta Phot. Sin. 44 1030003 (in Chinese) [王保清, 王传珂, 易涛, 李廷帅, 李晋, 朱效立, 谢常青, 刘慎业, 江少恩, 丁永坤 2015 光子学报 44 1030003]
[5] He K, Yi T, Liu S Y, Niu J B, Chen B Q, Zhu X L 2014 Micronanoelect. Technol. 51 381 (in Chinese) [何宽, 易涛, 刘慎业, 牛洁斌, 陈宝钦, 朱效立 2014 微纳电子技术 51 381]
[6] Ma J, Xie C Q, Ye T C, Liu M 2010 Acta Phys. Sin. 59 2564 (in Chinese) [马杰, 谢常青, 叶甜春, 刘明 2010 59 2564]
[7] Kuang L, Cao L, Zhu X, Wu S, Wang Z, Wang C, Liu S, Jiang S, Ding Y, Xie C, Zheng J 2011 J. Opt. Lett. 36 3954
[8] Wang C K, Wang B Q, Yi T, Fan Q P, Kuang L Y, Li J, Li T S, Zhu X L, Liu S Y, Jiang G 2016 J. Mod. Opt. 63 261
[9] Wang B Q, Yi T, Wang C K, Zhu X L, Li T S, Li J, Liu S Y, Jiang S E, Ding Y K 2016 Plasma Sci. Technol. 18 781
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