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Characterisation of plasma mirrors on the HELEN laser infra red CPA beam

机译:Helen激光红外线CPA光束上等离子镜的表征

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The performance of plasma mirrors has been characterised on the HELEN laser infra-red, chirped pulse amplification [CPA] beam line. This laser produced pulse energies up to 100J with pulse lengths of ~500fs. Plasma mirrors are initially low reflectance surfaces that transmit low intensity light but produce a reflecting plasma surface when exposed to high irradiance beams. Typically they are formed by transparent substrates at the laser wavelength and have been used either uncoated or with anti-reflection coatings. The coatings evaluated in these experiments were either multi-layer dielectrics or single layer sol-gel silica. Some of the fused silica substrates were coated on both faces, others were coated on the incident face only and a small number were used uncoated. The reflectance of the plasma mirrors was measured as a function of incident energy. A vacuum compatible pyro-electric sensor in conjunction with either a diffuser or neutral density filter was used to measure incident and reflected laser energy. Both the diffuser and filter could suffer laser damage at the highest incident energies available. The morphology of the damage of the different components and coating combinations was studied as a function of incident beam energy. The mirrors were being investigated to prevent pre-pulse effects in plasma physics experiments and increase the intensity contrast ratio of the laser beam incident onto solid targets. Their proximity to the laser target also allowed them to block debris and shrapnel arising from the laser matter interaction in some directions. These material emissions spread uncontrollably in the evacuated target chamber and may cause contamination of laser optics and filters or radiation diagnostic instrumentation. The plasma mirror components were operated at 45 degrees angle of incidence and an average input beam diameter of 5.5 millimetres at the mirrors with incident beam irradiances in the range 50 TW/cm~2 to 540 TW/cm~2. The reflected beams were focussed on to 10 micron thick, 10mm diameter metal foils and 3mm diameter polymer/metal targets with a thickness of 2 to 18 microns. The subsequent debris and shrapnel effects were studied using post shot microscopy and photography.
机译:等离子体镜的性能已经在Helen激光红外,啁啾脉冲放大[CPA]梁线上的特征。该激光器产生脉冲能量,高达100J,脉冲长度为〜500fs。等离子体镜是最初的低反射表面,其传输低强度光,但是在暴露于高辐照束时产生反射等离子体表面。通常,它们由激光波长的透明基板形成,并且已被未涂覆或用抗反射涂层使用。在这些实验中评价的涂层是多层电介质或单层溶胶 - 凝胶二氧化硅。将一些熔融二氧化硅底物涂覆在两个面上,其他熔合在入射面上涂覆在发生的面孔上,使用少量未涂覆。等离子体镜的反射率被测量为入射能量的函数。使用真空兼容的热电传感器与漫射器或中性密度过滤器一起使用,测量入射和反射激光能量。扩散器和过滤器都可以在可用的最高入射能中遭受激光损坏。研究了不同部件和涂层组合的损伤的形态作为入射光束能量的函数。正在研究镜子以防止血浆物理实验中的预脉冲效应,并将激光束入射到固体靶标的强度对比度增加。它们对激光靶的邻近也允许它们阻止在某些方向上从激光物质相互作用产生的碎屑和弹片。这些材料排放在抽空的目标室中无法控制地扩散,可能导致激光光学和过滤器或辐射诊断仪器的污染。等离子体镜子部件以45度的入射角和5.5毫米的平均输入光束直径在镜子中以50-Tm / cm〜2至540-t / cm〜2的入射梁辐射的镜子。将反射光束聚焦到10微米厚的10mm直径的金属箔和3mm直径的聚合物/金属靶标,厚度为2至18微米。使用后拍摄显微镜和摄影研究随后的碎片和弹片效应。

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