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首页> 外文期刊>Fusion Science and Technology >Design of a 50 TW / 20 J Chirped-Pulse Amplification Laser for High-Energy-Density Plasma Physics Experiments at the Nevada Terawatt Facility of the University of Nevada
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Design of a 50 TW / 20 J Chirped-Pulse Amplification Laser for High-Energy-Density Plasma Physics Experiments at the Nevada Terawatt Facility of the University of Nevada

机译:内华达大学内华达太瓦特实验室用于高能密度等离子体物理实验的50 TW / 20 J Chi脉冲放大激光器的设计

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摘要

We have developed a conceptual design for a 50 TW / 20 J short-pulse laser for performing high-energy-density plasma physics experiments at the Nevada Terawatt Facility of the University of Nevada, Reno. The purpose of the laser is to develop proton and x-ray radiography techniques, to use these techniques to study z-pinch plasmas, and to study deposition of intense laser energy into both magnetized and unmagnetized plasmas. Our design uses a commercial diode-pumped Nd:glass oscillator to generate 3-nJ, 200-fs mode-locked pulses at 1059 nm. An all-reflective grating stretcher increases pulse duration to 1.1 ns. A two-stage chirped-pulse optical parametric amplifier (OPCPA) using BBO crystals boosts pulse energy to 12 mJ, with gain saturation increasing pulse duration and bandwidth to ~1.9 ns and ~14 nm (FWHM), respectively. A chain using mixed silicate-phosphate Nd:glass increases pulse energy to 85 J while narrowing bandwidth to 7.4 nm (FWHM). A beam splitter directs 50 J to the laser target chamber to generate plasma. The remaining energy is directed to a roof-mirror pulse compressor that uses two 21 cm x 42 cm gold gratings to recompress pulses to ~350 fs. A 30-cm-focal-length off-axis parabolic reflector (OAP) focuses ~20 J onto target, producing an irradiance of 10~(19) W/cm~2 in a 10-μm-diameter spot. This paper describes planned plasma experiments, system performance requirements, the laser design, and the target area design.
机译:我们已经开发了用于50 TW / 20 J短脉冲激光器的概念设计,以便在里诺内华达大学的内华达太瓦工厂进行高能量密度等离子体物理实验。激光的目的是发展质子和X射线射线照相技术,使用这些技术研究Z捏等离子体,并研究强激光能量在磁化和非磁化等离子体中的沉积。我们的设计使用市售的二极管泵浦Nd:玻璃振荡器在1059 nm处产生3-nJ,200-fs锁模脉冲。全反射光栅展宽器将脉冲持续时间增加到1.1 ns。使用BBO晶体的两级chi脉冲光参量放大器(OPCPA)将脉冲能量提升至12 mJ,增益饱和将脉冲持续时间和带宽分别提高至〜1.9 ns和〜14 nm(FWHM)。使用混合硅酸盐-磷酸盐Nd:玻璃的链将脉冲能量增加到85 J,同时将带宽缩小到7.4 nm(FWHM)。分束器将50 J引导至激光靶腔以产生等离子体。剩余的能量被引导到一个屋顶镜脉冲压缩机,该压缩机使用两个21 cm x 42 cm的金光栅将脉冲重新压缩到约350 fs。一个30厘米焦距的离轴抛物面反射器(OAP)将〜20 J聚焦到目标上,在直径10微米的光斑中产生10〜(19)W / cm〜2的辐照度。本文介绍了计划的等离子体实验,系统性能要求,激光器设计和目标区域设计。

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