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空间太阳极紫外三波段成像光谱仪系统设计

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太阳上层大气,即日冕、过渡区和色球,是由炽热的高度动态的磁化等离子体构成,其中高度电离的离子发射出丰富的极紫外谱线。空间太阳极紫外光谱成像观测对于捕获太阳上层大气中爆发活动的动态物理演化过程,以及实现对大气等离子体特征参数的精确测量具有重要的意义。然而现有的极紫外光谱成像仪器只能针对太阳上层大气的一个或两个目标区域进行成像观测,缺乏采用单一仪器对整个太阳上层大气区域在大空间和宽波段尺度范围内的光谱进行诊断的能力,严重制约了人们对太阳爆发活动中的能量及物质输运过程的理解。为了利用单个仪器实现对日冕、过渡区和色球的高分辨率同时诊断观测,本文提出并设计了一款同时工作在17~21nm、70~80 nm和95~105 nm三个波段的太阳极紫外成像光谱仪,该仪器基于非罗兰圆结构下的椭球面变线距(EVLS)光栅像差校正理论,采用狭缝扫描式成像光谱结构,实现了具有大离轴狭缝视场的高空间、高光谱分辨的消像散光谱成像。基于蒙特卡罗统计模拟方法对太阳极紫外三波段成像光谱仪的最优模型开展光线追迹仿真实验,仿真结果表明,所设计的成像光谱仪取得了良好的光栅像差校正效果,系统空间分辨率优于0。6",光谱分辨率在17~21 nm波段优于0。006 nm,在70~80 nm和95~105 nm波段优于0。008 nm。本文研究对我国未来的太阳极紫外光谱成像仪器的发展和研制具有重要的理论意义,对我国未来的太阳空间探测任务的型号遴选具有重要的参考价值。
System Design of Space Solar Extreme Ultraviolet Three-Waveband Imaging Spectrometer
Objective The solar upper atmosphere including the corona,transition region,and chromosphere is composed of hot and highly dynamic magnetized plasma,from which highly ionized ions emit abundant extreme ultraviolet(EUV)spectral lines.Existing EUV imaging spectrometers can only conduct imaging on one or two target regions of the solar upper atmosphere but cannot diagnose the whole region in a wide spectral and spatial scale using a single instrument.This severely restricts our understanding of the energy and material transport processes in solar eruptive activities.Therefore,we propose and design a solar EUV three-waveband imaging spectrometer with an elliptical varied line-space(EVLS)grating that operates at non-Rowland circle mounting.This innovative solar EUV imaging spectrometer boasts exceptional spectral imaging performance in an extremely large off-axis slit field of view(FOV)while maintaining a compact instrument package.Furthermore,it provides excellent grating aberration correction even at very high spectrograph magnifications and beam speeds.We hope that our spectral imaging strategy and instrument system design will be instrumental in the simultaneous observation of the solar corona,transition region,and chromosphere in the near future.Methods The instrument utilizes an EVLS grating as the diffraction spectroscopic element.To achieve simultaneous correction of aberrations and free-astigmatism in all three spectral bands,we analyze the grating for aberrations by employing the optical path function and Fermat's principle.The correction condition of off-axis aberrations for the grating is obtained by optimizing the elliptical base shape parameters,line-space parameters,and structure parameters of the EVLS grating,with the grating's spectral focusing formula and spatial focusing curve formula considered.The global optimal solution for the instrument is then obtained via the simulated annealing algorithm and computer-aided design method to build the optimal model of the solar EUV three-waveband imaging spectrometer.Finally,the Monte Carlo method is adopted to non-sequentially trace different spectral line pairs in the target spectral band to verify the spectral imaging performance of the designed system.Results and Discussions Figure 3 shows the final optimized optical system layout of the designed solar EUV three-waveband imaging spectrometer.The working wavelengths of 17-21 nm,70-80 nm,and 95-105 nm are respectively utilized for observing the solar corona,transition region,and chromosphere.The detector for the 17-21 nm band adopts the charge-coupled device(CCD)structure of e2v technology with a pixel size of 13.5 μm,while the detectors for the 70-80 nm and 95-105 nm bands leverage an active pixel sensor(APS)structure with micro-channel plate(MCP)technology,and the pixel size is 20 μm.The entire instrument has an optical envelope volume of 1700 mmX370 mm× 100 mm,and the slit has five different widths to adapt to different spatial and temporal scales of solar eruption activities.High-resolution spectral imaging of the two-dimensional solar disk with an FOV of 9.6'X 5.0'can be achieved by stepwise rotation of the off-axis primary mirror.The instrument exhibits excellent imaging performance.The root mean square(RMS)radii at 17-21 nm are all less than 6 μm,while the RMS radii at 70-80 nm and 95-105 nm are mostly less than 10 μm.As the FOV increases,the radius of the diffractive spot RMS changes smoothly[Figs.5(d)-5(f)],which indicates good correction of off-axis aberrations.At 19 nm,the modulation transfer function values at the Nyquist spatial frequency(37 lp/mm)are all greater than 0.6[Fig.6(a)],and the geometric encircled energy within a single pixel size(13.5 μm)is better than 82.5%[Fig.7(a)].At 75 nm and 100 nm,the modulation transfer function values at the Nyquist spatial frequency(25 lp/mm)are both greater than 0.4[Figs.6(b)-6(c)],and the geometric encircled energy within a single pixel size is 80.5%and 85.9%[Figs.7(b)-7(c)]for each.Generally,the spatial resolution of the system is better than 0.6".The simulation results of non-sequential ray tracing show that the slit image length is 19.67 mm,which is consistent with the theoretically calculated value of 19.60 mm[Fig.8(b)].The slit images of the spectral lines with their respective calculated ideal spectral resolution intervals at the three center wavelengths of 19,75,and 100 nm are separated[Fig.8(a)].Therefore,the spectral resolution of the imaging spectrometer system is better than 0.006 nm in the 17-21 nm band and better than 0.008 nm in the 70-80 nm and 95-105 nm bands.Conclusions We propose an innovative slit-scanning spectral imaging architecture that operates at 17-21 nm,70-80 nm,and 95-105 nm.It can simultaneously diagnose and observe important plasma spectral lines in the solar corona,transition region,and chromosphere.Meanwhile,the theory of correcting the image aberrations caused by EVLS grating operating at non-Rowland circle mounting is studied.This structure can correct off-axis grating aberrations in a relatively compact design to achieve high-resolution spectroscopic imaging with broadband and large off-axis FOV.The ray tracing simulation experimental results reveal that the system's spatial resolution is better than 0.6",and its spectral resolution is better than 0.006 nm at 17-21 nm,and better than 0.008 nm at 70-80 nm and 95-105 nm respectively.The advanced design research of this instrument has theoretical significance for the development and research of China's solar EUV imaging spectrometers in the near future and provides references for the model selection of China's future solar space exploration missions.

solar space explorationsolar extreme ultravioletimaging spectrometergrating aberration correctionray tracing

段紫雯、邢阳光、彭吉龙、代树武、王颖、朱成林、闫雷、黄一帆、刘越、李林

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北京理工大学光电学院,北京 100081

北京卫星环境工程研究所,北京 100094

北京空间飞行器总体设计部,北京 100094

北京宇航系统工程研究所,北京 100076

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太阳空间探测 太阳极紫外 成像光谱仪 光栅像差校正 光线追迹

国家自然科学基金国家自然科学基金中国科学院战略性先导科技专项

6220502742274208XDA15018300

2024

光学学报
中国光学学会 中国科学院上海光学精密机械研究所

光学学报

CSTPCD北大核心
影响因子:1.931
ISSN:0253-2239
年,卷(期):2024.44(6)
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