首页> 外文期刊>Analytical Sciences >Deviation from Normal Boltzmann Distribution of High-lying Energy Levels of Iron Atom Excited by Okamoto-cavity Microwave-induced Plasmas Using Pure Nitrogen and Nitrogen–Oxygen Gases
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Deviation from Normal Boltzmann Distribution of High-lying Energy Levels of Iron Atom Excited by Okamoto-cavity Microwave-induced Plasmas Using Pure Nitrogen and Nitrogen–Oxygen Gases

机译:纯氮和氮氧气体激发的冈本腔微波诱导的等离子体激发的高原子能级玻尔兹曼分布的偏离

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This paper describes several interesting excitation phenomena occurring in a microwave-induced plasma (MIP) excited with Okamoto-cavity, especially when a small amount of oxygen was mixed with nitrogen matrix in the composition of the plasma gas. An ion-to-atom ratio of iron, which was estimated from the intensity ratio of ion to atomic lines having almost the same excitation energy, was reduced by adding oxygen gas to the nitrogen MIP, eventually contributing to an enhancement in the emission intensities of the atomic lines. Furthermore, Boltzmann plots for iron atomic lines were observed in a wide range of the excitation energy from 3.4 to 6.9 eV, indicating that plots of the atomic lines having lower excitation energies (3.4 to 4.8 eV) were well fitted on a straight line while those having more than 5.5 eV deviated upwards from the linear relationship. This overpopulation would result from any other excitation process in addition to the thermal excitation that principally determines the Boltzmann distribution. A Penning-type collision with excited species of nitrogen molecules probably explains this additional excitation mechanism, in which the resulting iron ions recombine with captured electrons, followed by cascade de-excitations between closely-spaced excited levels just below the ionization limit. As a result, these high-lying levels might be more populated than the low-lying levels of iron atom. The ionization of iron would be caused less actively in the nitrogen–oxygen plasma than in a pure nitrogen plasma, because excited species of nitrogen molecule, which can provide the ionization energy in a collision with iron atom, are consumed through collisions with oxygen molecules to cause their dissociation. It was also observed that the overpopulation occurred to a lesser extent when oxygen gas was added to the nitrogen plasma. The reason for this was also attributed to decreased number density of the excited nitrogen species due to collisions with oxygen molecule.
机译:本文介绍了用冈本腔激发的微波诱导等离子体(MIP)中发生的几种有趣的激发现象,特别是当等离子体气体成分中少量的氧气与氮基质混合时。通过将氧气添加到氮气MIP中,可以降低铁的离子原子比,该离子原子比是根据离子与具有几乎相同激发能的原子线的强度比估算的,最终有助于提高铁的发射强度。原子线。此外,在3.4至6.9 eV的宽激发能量范围内观察到铁原子线的Boltzmann图,这表明具有较低激发能(3.4至4.8 eV)的原子线的图很好地拟合在一条直线上,而那些大于5.5 eV时,线性关系向上偏离。除了主要确定玻尔兹曼分布的热激发之外,任何其他激发过程都可能导致这种人口过多。与氮分子的激发物种发生潘宁型碰撞可能解释了这种额外的激发机理,其中所生成的铁离子与捕获的电子重新结合,随后在刚好低于电离极限的紧密隔开的激发能级之间发生级联去激发。结果,与铁原子的低水平相比,这些高水平的位置可能更多。铁的电离在氮-氧等离子体中引起的活性要比纯氮等离子体中的少,这是因为在与铁原子碰撞时可以提供电离能的氮分子的激发态是通过与氧分子的碰撞而被消耗的。导致他们的分离。还观察到当向氮气等离子体中添加氧气时,人口过剩的发生程度较小。其原因还归因于由于与氧分子的碰撞而使被激发的氮种类的数量密度降低。

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