实验室空气激光点火的羟基光谱

C. Parigger
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引用次数: 1

摘要

这项工作研究了在标准环境温度和压力下实验室空气中激光等离子体中羟基的时空分布。我们感兴趣的是氢氧根的温度和密度的测定,并建立了氢氧根分子发射光谱与延时50 ~ 100 μs的阴影图的相关性,类似于以前在混合气体中氰化物、CN的阴影图和延时1 μs的发射光谱的相关性。波长和灵敏度校正的时空数据分析侧重于利用分子OH发射光谱进行温度推断。来自调q激光装置的近红外辐射在实验室空气中引发光学击穿。激光设备提供6ns,高达850毫焦耳,脉冲的波长为1064nm,聚焦辐照度范围为每平方厘米1到10太瓦。在0.1 ~ 100 μs的时间延迟范围内,利用倍频波束捕获阴影图来可视化击穿核。安装在0.64 m czerney - turner结构光谱仪出口面的强化电荷耦合器件,记录了激光等离子体在298nm ~ 321 nm波长范围内沿狭缝尺寸进行空间分辨的OH发射光谱,栅极宽度调整为10 μs。双原子OH信号是由等离子体的重组引起的,当时间延迟大于50 μs时,可以清晰地识别出来,但在等离子体衰变早期被N2的光谱所掩盖。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Hydroxyl Spectroscopy of Laboratory Air Laser-Ignition
This work investigates spatial and temporal distributions of hydroxyl, OH, in laser-plasma in laboratory air at standard ambient temperature and pressure. Of interest are determination of temperature and density of OH and establishment of a correlation of molecular OH emission spectra with shadow graphs for time delays of 50 to 100 μs, analogous to previous work on shadow graph and emission spectroscopy correlation for cyanide, CN, in gas mixtures and for time delays of the order of 1 μs. Wavelength- and sensitivity-corrected spatiotemporal data analysis focuses on temperature inferences using molecular OH emission spectroscopy. Near-IR radiation from a Q-switched laser device initiates optical breakdown in laboratory air. The laser device provides 6 ns, up to 850 milli Joule, pulses at a wavelength of 1064 nm, and focal irradiance in the range of 1 to 10 terawatt per centimeter-squared. Frequency doubled beams are utilized for capturing shadow graphs for visualization of the breakdown kernel at time delays in the range of 0.1 to 100 μs. OH emission spectra of the laser plasma, spatially resolved along the slit dimension, are recorded in the wavelength range of 298 nm to 321 nm, and with gate widths adjusted to 10 μs for the intensified charge-coupled device that is mounted at the exit plane of a 0.64 m Czerny-Turner configuration spectrometer. Diatomic OH signals occur due to recombination of the plasma and are clearly distinguishable for time delays larger than 50 μs, but are masked by spectra of N2 early in the plasma decay.
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