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Spatially and Temporally Resolved Electron and Atom Concentrations in an Afterglow Gas Discharge

机译:余辉气体放电中的空间和时间分辨的电子和原子浓度

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The use of a modified laser interferometer to measure the temporal and spatial behavior of a medium density (1013–1014 electrons/cc) afterglow plasma is described. In the work described here, the plasma to be studied is located inside the laser cavity. The presence of the plasma changes the laser frequency (within the Doppler‐broadened transition) and this frequency shift is determined by coupling an external cavity to the laser. This modification of the interferometer preserves the high sensitivity of using the transverse modes in the external cavity and has a spatial resolution in the medium being studied of less than 1 mm2. Two optical wavelengths, λ0=0.6328 μ and λ0=1.1523 μ, and two microwave wavelengths, λ=4, 8 mm, are used in this study and excellent agreement is obtained between measurements. It is shown that there is a strong migration of the gas atoms away from the discharge vessel axis due to the localized heating during the active discharge. Electron loss processes in such plasmas are discussed. Because of the excellent spatial resolution, the rate of loss of electrons by diffusion can be measured directly, and hence the electron temperature can be estimated. Electron temperatures obtained in this manner agree to within a factor of two with that obtained by the double‐probe technique.
机译:描述了使用改进的激光干涉仪测量中等密度(1013–1014电子/ cc)余辉等离子体的时间和空间行为。在这里描述的工作中,要研究的等离子体位于激光腔内部。等离子体的存在改变了激光频率(在多普勒扩展的过渡范围内),并且该频移是通过将外部腔体耦合到激光器来确定的。干涉仪的这种修改保留了在外腔中使用横向模式的高灵敏度,并且在所研究的介质中具有小于1 mm2的空间分辨率。在这项研究中,使用了两个光学波长λ0= 0.6328μ和λ0= 1.1523μ,以及两个微波波长λ= 4、8 mm,并且两次测量之间获得了极好的一致性。结果表明,由于主动放电过程中的局部加热,气体原子有很强的迁移作用,使其远离放电管轴线。讨论了这种等离子体中的电子损失过程。由于出色的空间分辨率,可以直接测量电子因扩散而损失的速率,因此可以估算电子温度。以这种方式获得的电子温度与通过双探针技术获得的电子温度相差约两倍。

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    《Journal of Applied Physics 》 |1965年第11期| 共9页
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  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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