High Power Laser Science and Engineering, 2016, 4 (1): 010000e2, Published Online: Oct. 25, 2016  

Hard x-ray transmission curved crystal spectrometers (10–100 keV) for laser fusion experiments at the ShenGuang-III laser facility Download: 828次

Author Affiliations
1 Department of Modern Physics & CAS Key Laboratory of Geospace Environment, University of Science and Technology of China, Hefei, Anhui 230026, China
2 Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900, China
3 National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China
Figures & Tables

Fig. 1. Cauchois-geometry optics of a symmetry transmission cylindrical curved crystal.

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Fig. 2. (Solid lines) the position of the slit $f$ versus the detecting distance $s$ (the source-to-crystal distance) of the 17.48 keV Mo K${\it\alpha}_{1}$ x-ray. (Dash lines) the position of the slit $f$ versus the x-ray photon energy at a fixed detecting distance, $s$, of 500 mm. The crystals’ curvature radii are 150 and 300 mm.

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Fig. 3. The lateral distance of the 10 keV x-ray footprint on the crystal (Point C in Figure 1) versus the crystal’s curvature radius. The detecting distances $s$ are 200 mm (dash line) and 1500 mm (solid line).

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Fig. 4. Theoretical spectral sensitivities of the transmission curved crystal spectrometers LCCS and HCCS. Insert is the sensitivity curve of Fujifilm™ image plates SR.

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Fig. 5. Spectral resolution of the LCCS and HCCS spectrometers at detecting distances of 200 and 1500 mm. The working distance of the recording medium is fixed at $d_{0}=22~\text{mm}$.

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Fig. 6. The energy-dependent integrated reflectivity of the curved crystals. The ${\it\alpha}$-quartz (10–11) crystals’ curvature radii are 300 mm (HCCS) and 150 mm (LCCS).

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Fig. 7. Schematic diagram of the HCCS spectrometer.

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Fig. 8. Experimental spectral images of a Mo anode x-ray source measured by (a) LCCS and (b) HCCS. Details of K lines are shown in (c) and (d), for LCCS and HCCS, respectively. The exposure times are 60 s for LCCS and 30 s for HCCS.

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Fig. 9. Spectral images of the Mo anode x-ray source obtained by LCCS with various working distances $d_{\text{0}}$. (a) $d_{\text{0}}=7~\text{mm}$; (b) $d_{\text{0}}=22~\text{mm}$; (c) $d_{\text{0}}=52~\text{mm}$. The abscissa represents the distance from the left side of image.

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Fig. 10. Experimentally measured and theoretically calculated spectral resolution at various working distances.

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Fig. 11. Ag spectral images recorded using the HCCS at the XGIII laser facility (a), the detail characteristic K lines of Ag (b, c).

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Table1. Design parameters of the Curved Crystal Spectrometers (CCS).

LCCS HCCS
Crystal${\it\alpha}$-quartz (10–11) 70 mm ($L$) $\times$ 12 mm ($W$) $\times$ 0.27 mm ($T$)
Curvature radius (mm) 150 300
Energy range (keV) 10–56 17–100
Detecting distance (mm)200–1500 200–1500
Resolution $(E/{\rm\Delta}E)$331-57327-54
Recording mediumFujifilm BAS-SR IPs 74 mm ($L$) $\times$ 20 mm ($W$)

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Ming-hai Yu, Guang-yue Hu, Ning An, Feng Qian, Yu-chi Wu, Xiao-ding Zhang, Yu-qiu Gu, Qiu-ping Wang, Jian Zheng. Hard x-ray transmission curved crystal spectrometers (10–100 keV) for laser fusion experiments at the ShenGuang-III laser facility[J]. High Power Laser Science and Engineering, 2016, 4(1): 010000e2.

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