Time-Resolved Measurement of Radiatively Heated Iron 2p-3d Transmission Spectra
ZHAO Yang1**, SHANG Wan-Li1, XIONG Gang1, JIN Feng-Tao2, HU Zhi-Min1, WEI Min-Xi1, YANG Guo-Hong1, ZHANG Ji-Yan1, YANG Jia-Min1
1Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900 2Department of Physics, National University of Defense Technology, Changsha 410073
Time-Resolved Measurement of Radiatively Heated Iron 2p-3d Transmission Spectra
ZHAO Yang1**, SHANG Wan-Li1, XIONG Gang1, JIN Feng-Tao2, HU Zhi-Min1, WEI Min-Xi1, YANG Guo-Hong1, ZHANG Ji-Yan1, YANG Jia-Min1
1Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900 2Department of Physics, National University of Defense Technology, Changsha 410073
摘要An experimental measurement of radiatively heated iron plasma transmission spectra was performed on Shenguang II laser facility. In the measurement, the self−emission spectrum, the backlighting spectrum, and the absorption spectrum were imaged with a flat filed grating and recorded on a gated micro channel plate detector to obtain the time-resolved transmission spectra in the range 10-20 Å (approximately 0.6-1.3 keV). Experimental results are compared with the calculation results of an unsolved transition array (UTA) code. The time-dependent relative shift in the positions of the 2p-3d transmission array is interpreted in terms of the plasma temperature variations.
Abstract:An experimental measurement of radiatively heated iron plasma transmission spectra was performed on Shenguang II laser facility. In the measurement, the self−emission spectrum, the backlighting spectrum, and the absorption spectrum were imaged with a flat filed grating and recorded on a gated micro channel plate detector to obtain the time-resolved transmission spectra in the range 10-20 Å (approximately 0.6-1.3 keV). Experimental results are compared with the calculation results of an unsolved transition array (UTA) code. The time-dependent relative shift in the positions of the 2p-3d transmission array is interpreted in terms of the plasma temperature variations.
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