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在星光Ⅱ激光装置上,测量了脉宽1ns、能量40-110J的527nm激光在不同条件下辐照Au盘靶、Al盘靶的背向散射能量。结果表明:激光辐照Au盘靶时.在聚焦条件下背向散射能量约占打靶激光能量的7.8%;在束匀滑条件下背向散射能量份额下降到6.2%左右,证明了束匀滑可有效抑制背向散射。对比Au盘靶、Al盘靶背反能量与打靶激光能量关系曲线,可以看出背向散射能量与打靶激光能量基本上成线性关系。 Au and Al disk target were irradiated with -1 ns, 40-110 J, 527 nm laser at Xingguang-Ⅱ facility. The backscattered lights by laser-produced plasma were studied experimentally. The results are in troduced in this paper. Backscattered light energy is 7.8% of laser energy when laser is focused on Au disk target; when laser beam is smoothed, it is 6.2%. The comparison shows that laser smoothing can restrain backscattered light efficiency. The experimental results :also show that there is a linear relation between backscattered light energy and the laser energy. 相似文献
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Research on Stimulated Raman Scattering Spectrum for Cavity Targets at the Shenguang-Ⅱ Laser Facility 下载免费PDF全文
The stimulated Raman scattering (SRS) experiments with half-cavity targets have been carried out at the Shenguang-lI laser facility. The imitative optic multiple-channel analyser (OMA) spectrograph is used to obtain the SRS experimental spectrum. We have developed a two-dimensional laser plasma interaction (LPI2D)code. The SRS spectrum for half-cavity targets is analysed theoretically and simulated numerically using the LPI2D code. These simulations quantitatively reproduce the experimental results firstly. 相似文献
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介绍了在神光Ⅱ装置上开展的长脉冲2 ns,351 nm激光与黑腔靶相互作用的实验,报道了受激Raman散射光时间分辨谱图及能量测量的实验结果。长脉冲2 ns激光注入小腔靶(Ø700 mm×1 250 mm)时,激光辐照缝靶产生的SRS光能量是激光与全腔靶作用产生的SRS光能量的1.3倍。在2 ns激光与不同尺寸黑腔靶作用的情况下,激光辐照小腔靶产生的SRS光能量比标准腔靶(Ø800 mm×1 350 mm)产生的SRS光能量高1.6倍。由于激光功率密度下降,2 ns激光打靶SRS散射光要弱于短脉冲1 ns激光打靶,但持续时间稍长。实验结果表明:长脉冲2 ns激光与标准腔靶相互作用时,等离子体“堵腔效应”比较严重,标准腔靶尺寸不再合适。 相似文献
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利用一维实验,模拟了惯性约束聚变中烧蚀层中冲击波传输和多次冲击追赶过程.针对聚苯乙烯材料(CH)容易被X射线离化的问题,通过较详细的数值模拟,分析了用Au和Cu做阻挡层对冲击波信号的影响.利用两种不同的辐射源,研究了辐射源两个台阶强度变化对两次冲击信号的影响.经过分析,使用在Al基底上面加厚度为5 μm的Au膜以挡X射线的办法,获得了单次冲击在CH材料中加载和减速的清晰条纹图.利用在Al基底上加厚度为2 μm的Au膜和厚度为3 μm的Cu膜的方法,获得了两次冲击在CH材料中加速、减速和二次加载的条纹图.实
关键词:
光学诊断
冲击波调速
离化效应 相似文献
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