Charged particle stopping power experiments on Orion

J. E. Coltman, W. Garbett, C. Horsfield, M. Rubery, A. Leatherland, S. Gales, A. Meadowcroft, A. Simons, V. Woolhead, S. Rice
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Abstract

The Orion laser facility provides a platform for performing direct drive capsule implosions. The predicted level of capsule performance for this type of experiment is uncertain, largely due to the reduced number of laser beams (10), compared to facilities such as OMEGA (60), which limits the drive symmetry. To this end, following a one-dimensional (1D) design study of capsule phase space, experiments have been performed to evaluate the performance of deuterium (DD)-filled targets. A thin shell “exploding pusher” (EP) design is desirable both for robustness and for future charged-particle stopping power experiments to validate current stopping power theories, important in high-energy-density physics (HEDP). Stopping power experiments require a well-known source of particles (a proton source, the EP target), a well-characterized plasma (secondary target), and an accurate measurement of the energy loss (downshift in energy of the particle traversing the plasma). DD implosions generate 3MeV protons, which will then interact with the secondary target heated isochorically by a short pulse laser to ~200–300 eV at solid density (ne ~ 2 × 1023 g/cc). The optimum EP capsule selected from the study, taking into account facility and target fabrication constraints, satisfies design criteria on the 1D clean fusion yield, capsule dynamics, and implosion time. The nominal target was a silica glass shell of radius 250 ± 10 µm and thickness 2.3 ± 0.5 µm, filled with 10 atm of DD gas. The preliminary secondary target was a plastic cuboid of ~70 × 70 × 50 µm dimensions. The work presented here focuses on the design of an optimum EP capsule and includes experimental results for comparison.The Orion laser facility provides a platform for performing direct drive capsule implosions. The predicted level of capsule performance for this type of experiment is uncertain, largely due to the reduced number of laser beams (10), compared to facilities such as OMEGA (60), which limits the drive symmetry. To this end, following a one-dimensional (1D) design study of capsule phase space, experiments have been performed to evaluate the performance of deuterium (DD)-filled targets. A thin shell “exploding pusher” (EP) design is desirable both for robustness and for future charged-particle stopping power experiments to validate current stopping power theories, important in high-energy-density physics (HEDP). Stopping power experiments require a well-known source of particles (a proton source, the EP target), a well-characterized plasma (secondary target), and an accurate measurement of the energy loss (downshift in energy of the particle traversing the plasma). DD implosions generate 3MeV protons, which wil...
猎户座上的带电粒子停止能量实验
猎户座激光设备为执行直接驱动胶囊内爆提供了一个平台。这种类型实验的胶囊性能的预测水平是不确定的,主要是因为与OMEGA(60)等设备相比,激光束的数量减少了(10),这限制了驱动器的对称性。为此,在对胶囊相空间进行一维(1D)设计研究之后,进行了实验来评估氘(DD)填充靶的性能。一种薄壳“爆炸推子”(EP)设计对于鲁棒性和未来的带电粒子停止功率实验都是理想的,以验证电流停止功率理论,这在高能量密度物理(HEDP)中很重要。停止功率实验需要一个已知的粒子源(质子源,EP靶),一个特性良好的等离子体(次级靶),以及对能量损失的精确测量(穿过等离子体的粒子的能量下降)。DD内爆产生3MeV的质子,这些质子将在固体密度(ne ~2 × 1023 g/cc)下与短脉冲激光等距加热至~ 200-300 eV的次级目标相互作用。从研究中选择的最佳EP胶囊,考虑到设施和目标制造的约束,满足一维清洁融合良率、胶囊动力学和内爆时间的设计标准。标称目标是一个半径为250±10µm,厚度为2.3±0.5µm的硅玻璃外壳,填充10atm的DD气体。初步的二次目标为~70 × 70 × 50µm尺寸的塑料长方体。本文介绍的工作重点是设计最佳的EP胶囊,并包括实验结果进行比较。猎户座激光设备为执行直接驱动胶囊内爆提供了一个平台。这种类型实验的胶囊性能的预测水平是不确定的,主要是因为与OMEGA(60)等设备相比,激光束的数量减少了(10),这限制了驱动器的对称性。为此,在对胶囊相空间进行一维(1D)设计研究之后,进行了实验来评估氘(DD)填充靶的性能。一种薄壳“爆炸推子”(EP)设计对于鲁棒性和未来的带电粒子停止功率实验都是理想的,以验证电流停止功率理论,这在高能量密度物理(HEDP)中很重要。停止功率实验需要一个已知的粒子源(质子源,EP靶),一个特性良好的等离子体(次级靶),以及对能量损失的精确测量(穿过等离子体的粒子的能量下降)。DD内爆产生3MeV的质子,这将…
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