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首页> 外文期刊>Spectrochimica Acta, Part B. Atomic Spectroscopy >Comparative study on contribution of charge-transfer collision to excitations of iron ion between argon radio-frequency inductively-coupled plasma and nitrogen microwave induced plasma
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Comparative study on contribution of charge-transfer collision to excitations of iron ion between argon radio-frequency inductively-coupled plasma and nitrogen microwave induced plasma

机译:氩射频感应耦合等离子体与氮气微波诱导等离子体之间电荷转移碰撞对铁离子激发贡献的比较研究

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摘要

This paper describes an ionization/excitation phenomenon of singly-ionized iron occurring in an Okamoto-cavity microwave induced plasma (MIP) as well as an argon radio-frequency inductively-coupled plasma (ICP), by comparing the Boltzmann distribution among iron ionic lines (Fe II) having a wide range of the excitation energy from 4.76 to 9.01 eV. It indicated in both the plasmas that plots of Fe II lines having lower excitation energies (4.76 to 5.88 eV) were fitted on each linear relationship, implying that their excitations were caused by a dominant thermal process such as collision with energetic electron. However, Fe II lines having higher excitation energies (more than 7.55 eV) had a different behavior from each other. In the ICP, Boltzmann plots of Fe II lines assigned to the higher excited levels also followed the normal Boltzmann relationship among the low-lying excited levels, even including a deviation from it in particular excited levels having an excitation energy of ca. 7.8 eV. This deviation can be attributed to a charge-transfer collision with argon ion, which results in the overpopulation of these excited levels, but the contribution is small. On the other hand, the distribution of the high-lying excited levels was non-thermal in the Okamoto-cavity MIP, which did not follow the normal Boltzmann relationship among the low-lying excited levels. A probable reason for the non-thermal characteristics in the MIP is that a charge-transfer collision with nitrogen molecule ion having many vibrational/rotational levels could work for populating the 3d(6)4p (3d(5)4s4p) excited levels of iron ion broadly over an energy range of 7.6-9.0 eV, while collisional excitation by energetic electron would occur insufficiently to excite these high-energy levels. (C) 2015 Elsevier B.V. All rights reserved.
机译:本文通过比较铁离子线之间的玻尔兹曼分布,描述了在冈本腔微波感应等离子体(MIP)和氩气射频感应耦合等离子体(ICP)中发生的单电离铁的电离/激发现象。 (Fe II)的激发能范围从4.76到9.01 eV。在两个等离子体中都表明,具有较低激发能(4.76至5.88 eV)的Fe II线的图线符合每个线性关系,这表明它们的激发是由主要的热过程(例如与高能电子碰撞)引起的。然而,具有较高激发能(大于7.55 eV)的Fe II线具有彼此不同的行为。在ICP中,分配给较高激发能级的Fe II谱线的Boltzmann图也遵循低层激发能级之间的正常Boltzmann关系,甚至包括与它的偏差,特别是激发能为ca的激发能级。 7.8 eV。该偏差可归因于与氩离子的电荷转移碰撞,这导致这些激发能级的过度聚集,但贡献很小。另一方面,在冈本空洞MIP中,高激发水平的分布是非热的,这与低激发水平之间的正常玻耳兹曼关系不符。 MIP中非热特性的可能原因是,与具有许多振动/旋转能级的氮分子离子发生电荷转移碰撞可能会产生铁的3d(6)4p(3d(5)4s4p)激发能级离子在7.6-9.0 eV的能量范围内广泛传播,而高能电子的碰撞激发将不足以激发这些高能级。 (C)2015 Elsevier B.V.保留所有权利。

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