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Study of high-Z-coated ignition target by detailed configuration accounting atomic physics for direct-drive inertial confinement fusion

机译:通过详细配置核算原子物理研究高Z涂层点火靶,用于直接驱动惯性监禁融合

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Direct-drive is one of the key approaches in the study of inertial confinement fusion, but the laser imprinting caused by laser intensity inhomogeneities is one of the main obstacles to achieving ignition in direct-drive. It has previously been demonstrated that a thin high-Z overcoat on the laser side of the target can significantly mitigate laser imprinting (S P Obenschain et al 2002 Phys. Plasmas 9 2234). In the current work, the 1D multi-group radiation hydrodynamic code RDMG, coupled with the detailed configuration accounting non-LTE atomic physics package MBDCA (RDMG-MBDCA) was used to study a Au-coated ignition target and its implosion performances under laser direct-drive, and a bare CH target was also simulated for comparison. Our study shows that the shell compressibility in the Au-coated target is enhanced with a smaller in-flight adiabat a if and a higher neutron yield Y-id than in the bare CH target. This is because the Au coating helps to maintain a hotter CH plasma, which can ablate a wider electron conduction region with lower density leading to a weaker second shock, creating a more compressed shell and a higher yield than the bare CH target. We also compared the simulations from RDMG -MBDCA with those from RDMG-AA which is coupled with an averaged-atom (AA) non-LTE model. As a result, the shell from the AA model is less compressed with a higher alpha(if) and a lower Y-id because the AA model gives a higher inward x-ray emission during the pre-pulse than the DCA model does, which therefore drives a stronger shock and leads to a higher fuel entropy.
机译:直接驱动是惯性监禁融合研究中的关键方法之一,但激光强度不均匀引起的激光印迹是在直接驱动中实现点火的主要障碍之一。先前已经证明,目标的激光侧的薄高Z外涂层可以显着减轻激光印迹(S P Obenschain等,Phy。等离子体9 2234)。在当前工作中,使用与详细配置核算非LTE原子物理包MBDCA(RDMG-MBDCA)耦合的1D多组辐射流体动力学代码RDMG研究Au涂层点火目标及其在激光直接下的内爆性能-Drive,还模拟了裸CH目标进行比较。我们的研究表明,Au涂层靶中的壳体可压缩性增强,具有较小的飞行中的AF和更高的中子率Y-ID,而不是裸CH靶标。这是因为Au涂层有助于保持更热的CH等离子体,其可以消除具有较低密度的较宽的电子传导区域,导致第二冲击较弱,产生比裸CH靶更压缩的壳体和更高的产率。我们还将从RDMG -MBDCA的模拟与来自RDMG-AA的仿真进行了比较,其与平均原子(AA)非LTE模型耦合。结果,来自AA模型的外壳较小,具有更高的α(IF)和较低的Y-ID压缩,因为AA模型在预脉冲期间提供比DCA模型更高的向内X射线发射,这因此,驱动更强的冲击并导致更高的燃料熵。

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