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First experimental comparisons of laser-plasma interactions between spherical and cylindrical hohlraums at SGIII laser facility

机译:SGIII激光设备中球形和圆柱形空穴之间的激光-等离子体相互作用的首次实验比较

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We present our recent laser-plasmas instability (LPI) comparison experiment at the SGIII laser facility between the spherical and cylindrical hohlraums. Three kinds of filling are considered: vacuum, gas-filling with or without a capsule inside. A spherical hohlraum of 3.6?mm in diameter, and a cylindrical hohlraum of 2.4?mm?×?4.3?mm are used. The capsule diameter is 0.96?mm. A flat-top laser pulse with 3?ns duration and up to 92.73?kJ energy is used. The experiment has shown that the LPI level in the spherical hohlraum is close to that of the outer beam in the cylindrical hohlraum, while much lower than that of the inner beam. The experiment is further simulated by using our 2-dimensional radiation hydrodynamic code LARED-Integration, and the laser back-scattering fraction and the stimulated Raman scatter (SRS) spectrum are post-processed by the high efficiency code of laser interaction with plasmas HLIP. According to the simulation, the plasma waves are strongly damped and the SRS is mainly developed at the plasma conditions of electron density from 0.08? n c to 0.1? n c and electron temperature from 1.5?keV to 2.0?keV inside the hohlraums. However, obvious differences between the simulation and experiment are found, such as that the SRS back-scattering is underestimated, and the numerical SRS spectrum peaks at a larger wavelength and at a later time than the data. These differences indicate that the development of a 3D radiation hydrodynamic code, with more accurate physics models, is mandatory for spherical hohlraum study.
机译:我们介绍了在球形和圆柱形的SGIII激光设备上我们最近的激光等离子体不稳定性(LPI)比较实验。考虑了三种填充:真空,内部有或没有胶囊的气体填充。使用了直径为3.6μmm的球状大球和2.4μmm××4.3μmm的圆柱状。胶囊直径为0.96mm。使用持续时间为3?ns且能量高达92.73?kJ的平顶激光脉冲。实验表明,球形圆柱体中的LPI水平与圆柱形圆柱体中的外梁接近,而远低于内梁。使用我们的二维辐射流体动力学代码LARED-Integration进一步模拟了该实验,并且通过与等离子体HLIP相互作用的高效代码对激光反向散射分数和受激拉曼散射(SRS)光谱进行了后处理。根据模拟,等离子体波被强烈衰减,并且SRS主要在电子密度从0.08?m的等离子体条件下发展。 n c到0.1? n c和电子温度从1.5?keV到2.0?keV。但是,在仿真和实验之间发现明显的差异,例如,SRS的反向散射被低估了,数字SRS光谱在比数据更大的波长和更晚的时间达到峰值。这些差异表明,开发具有更精确的物理模型的3D辐射流体力学代码对于球形球磨机研究是必不可少的。

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