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METHOD TO MEASURE SPATIAL DISTRIBUTION OF ION TEMPERATURE OF HYDROGEN PLASM

机译:测量氢等离子体温度的空间分布方法

摘要

FIELD: instrumentation.;SUBSTANCE: to each registered atom an electric pulse at an analyser outlet corresponds, and simultaneously photons are registered with a spectral selective device (SSD), having a common input collimator with the analyser. At the same time atoms are registered with energy Ei by i channel of the analyser, and photons are registered with wave length λ0-Δλ by i channel of the SSD, where λ0 - wave length of a hydrogen line, emitted by a dormant atom, and Δλ - wave length shift specified by Doppler effect for energy Ei. Occurred electric pulses from the outlet of a coincidence detector are sent to a pulse counter and by the ratio of quantity of pulses registered in different channels of the analyser, they determine energy distribution of recharging atoms and accordingly ion temperature Tion in this LMA. Then they produce values Tion(j) for j local areas of measurement and dependence Tion(L), where L - coordinate along the observation line, i.e. spatial distribution of ion temperature.;EFFECT: provision of possibility of measurements without use of probing atom bundles, increased validity and accuracy of measurements.;3 dwg
机译:领域:仪器;物质:分析器出口处的每个脉冲对应一个注册的原子,同时光子通过光谱选择装置(SSD)进行注册,该光谱选择装置具有与分析仪共用的输入准直仪。同时原子通过分析器的i通道以能量E i 进行配准,光子通过SSD的i通道以波长λ 0 -Δλ进行配准,其中λ 0 -休眠原子发射的氢线的波长,而Δλ-多普勒效应为能量E i 指定的波长偏移。来自一致性检测器出口的电脉冲被发送到脉冲计数器,并通过在分析仪的不同通道中记录的脉冲数量的比率来确定再充电原子的能量分布,并由此确定离子温度T ion 。然后,它们为j个局部测量区域生成值T ion (j)并依赖T ion (L),其中L-沿观察线协调,即离子温度;效果:不使用探测原子束就可以进行测量,提高了测量的有效性和准确性。; 3 dwg

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