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Laser-induced carbon plasma emission spectroscopic measurements on solid targets and in gas-phase optical breakdown

机译:固体靶材和气相光学击穿中的激光诱导碳等离子体发射光谱测量

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We report measurements of time- and spatially averaged spontaneous-emission spectra following laser-induced breakdown on a solid graphite/ambient gas interface and on solid graphite in vacuum, and also emission spectra from gas-phase optical breakdown in allene C3H4 and helium, and in CO2 and helium mixtures. These emission spectra were dominated by CII (singly ionized carbon), CIII (doubly ionized carbon), hydrogen Balmer beta (Hp), and Swan C-2 band features. Using the local thermodynamic equilibrium and thin plasma assumptions, we derived electron number density and electron temperature estimates. The former was in the 10(16) cm(-3) range, while the latter was found to be near 20000 K. In addition, the vibration-rotation temperature of the Swan bands of the C-2 radical was determined to be between 4500 and 7000 K, using an exact theoretical model for simulating diatomic emission spectra. This temperature range is probably caused by the spatial inhomogeneity of the laser-induced plasma plume. Differences are pointed out in the role of ambient CO2 in a solid graphite target and in gas-phase breakdown plasma. (c) 2005 Optical Society of America.
机译:我们报告了在固体石墨/环境气体界面上以及在真空中的固体石墨上的激光诱导击穿之后的时间和空间平均自发发射光谱的测量值,以及在丙二烯C3H4和氦气中气相光学击穿的发射光谱,以及在二氧化碳和氦气混合物中。这些发射光谱主要由CII(单电离碳),CIII(双电离碳),氢巴尔默β(Hp)和Swan C-2谱带特征控制。使用局部热力学平衡和薄等离子体假设,我们得出了电子数密度和电子温度估计值。前者在10(16)cm(-3)范围内,而后者则在20000 K附近。此外,确定C-2自由基的Swan谱带的振动旋转温度为4500和7000 K,使用精确的理论模型来模拟双原子发射光谱。该温度范围可能是由激光感应等离子体羽流的空间不均匀性引起的。指出了在固态石墨靶和气相击穿等离子体中环境CO2的作用存在差异。 (c)2005年美国眼镜学会。

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