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X-ray conversion efficiency of high-Z hohlraum wall materials for indirect drive ignition

机译:间接驱动点火的高Z霍尔姆壁材料的X射线转换效率

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The conversion efficiency of 351 nm laser light to soft x rays (0.1-5 keV) was measured for Au, U, and high Z mixture "cocktails" used as hohlraum wall materials in indirect drive fusion experiments. For the spherical targets in a direct drive geometry, flattop laser pulses and laser smoothing with phase plates are employed to achieve constant and uniform laser intensities of 10(14) and 10(15) W/cm(2) over the target surface that are relevant for the future ignition experiments at the National Ignition Facility [G. H. Miller, E. I. Moses, and C. R. Wuest, Nucl. Fusion 44, 228 (2004)]. The absolute time and spectrally resolved radiation flux is measured with a multichannel soft x-ray power diagnostic. The conversion efficiency is then calculated by dividing the measured x-ray power by the incident laser power from which the measured laser backscattering losses are subtracted. After similar to 0.5 ns, the time resolved x-ray conversion efficiency reaches a slowly increasing plateau of 95% at 10(14) W/cm(2) laser intensity and of 80% at 10(15) W/cm(2). The M-band flux (2-5 keV) is negligible at 10(14) W/cm(2) reaching similar to 1% of the total x-ray flux for all target materials. In contrast, the M-band flux is significant and depends on the target material at 10(15) W/cm(2) laser intensity, reaching values between 10% of the total flux for U and 27% for Au. LASNEX simulations [G. B. Zimmerman and W. L. Kruer, Comm. Plasma Phys. Contr. Fusion 2, 51 (1975)] show good agreement in conversion efficiency and radiated spectra with data when using XSN atomic physics model and a flux limiter of 0.15, but they underestimate the generated M-band flux. (c) 2008 American Institute of Physics.
机译:对于在间接驱动聚变实验中用作ho壁材料的金,铀和高Z混合物“鸡尾酒”,测量了351 nm激光到软X射线(0.1-5 keV)的转换效率。对于直接驱动几何中的球形目标,采用平顶激光脉冲和相位板进行激光平滑,以在目标表面上获得恒定且均匀的10(14)和10(15)W / cm(2)的激光强度。与国家点火设施的未来点火实验有关[G. H. Miller,E。I. Moses和C. R. Wuest,Nucl。融合44,228(2004)]。绝对时间和光谱分辨辐射通量通过多通道软X射线功率诊断仪进行测量。然后通过将测量的X射线功率除以入射激光功率来计算转换效率,从中减去测量的激光反向散射损耗。经过约0.5 ns后,时间分辨的X射线转换效率在10(14)W / cm(2)的激光强度下达到95%的缓慢增加的平台,而在10(15)W / cm(2)的情况下达到80%的缓慢增加的平台。 。 M波段通量(2-5 keV)在10(14)W / cm(2)时可以忽略不计,达到所有目标材料的总X射线通量的1%。相反,M波段通量很大,并且取决于目标材料在10(15)W / cm(2)的激光强度下,其值介于U的总通量的10%和Au的总通量的27%之间。 LASNEX模拟[G. B.Zimmerman和W.L.Kruer,通讯。等离子物理控制Fusion 2,51(1975)]在使用XSN原子物理模型和通量限制器0.15的情况下,在转换效率和辐射光谱方面与数据显示出良好的一致性,但它们低估了所产生的M波段通量。 (c)2008年美国物理研究所。

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