Absolute atomic nitrogen density spatial mapping in three MHCD configurations

A. Remigy, Belkacem Menacer, Konstantinos Kourtzanidis, Odyssea Gazeli, K. Gazeli, G. Lombardi, C. Lazzaroni
{"title":"Absolute atomic nitrogen density spatial mapping in three MHCD configurations","authors":"A. Remigy, Belkacem Menacer, Konstantinos Kourtzanidis, Odyssea Gazeli, K. Gazeli, G. Lombardi, C. Lazzaroni","doi":"10.1088/1361-6595/ad227b","DOIUrl":null,"url":null,"abstract":"\n In this work, nanosecond Two-photon Absorption Laser Induced Fluorescence is used to perform spatial mappings of the absolute density of nitrogen atoms generated in a micro-hollow cathode discharge (MHCD). The MHCD is operated in the normal regime, with a DC discharge current of 1.6 mA and a plasma is ignited in a 20% Ar/ 80% N2 gas mixture. A 1-inch diameter aluminum substrate acting as a third electrode (second anode) is placed further away from the MHCD to emulate a deposition substrate. The spatial profile of the N atoms is measured in three MHCD configurations. First, we study a MHCD having the same pressure (50 mbar) on both sides of the anode/cathode electrodes and the N atoms diffuse in three dimensions from the MHCD. The recorded N atoms density profile in this case satisfies our expectations, i.e., the maximal density is found at the axis of the hole, close to the MHCD. However, when we introduce a pressure differential, thus creating a plasma jet, an unexpected N atoms distribution is measured with maximum densities away from the jet axis. This behavior cannot be simply explained by the TALIF measurements. Then, as a first simplified approach in this work, we turn our attention to the role of the gas flow pattern. Compressible gas flow simulations show a correlation between the jet width and the radial distribution of the N atoms at different axial distances from the gap. Finally, a DC positive voltage is applied to the third electrode (second anode), which ignites a Micro Cathode Sustained Discharge (MCSD). The presence of the pressure differential unveils two stable working regimes depending on the current repartition between the two anodes. The MCSD enables an homogenization of the density profile along the surface of the substrate, which is suitable for nitride deposition applications.","PeriodicalId":20192,"journal":{"name":"Plasma Sources Science and Technology","volume":"121 6","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-01-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Plasma Sources Science and Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/1361-6595/ad227b","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

In this work, nanosecond Two-photon Absorption Laser Induced Fluorescence is used to perform spatial mappings of the absolute density of nitrogen atoms generated in a micro-hollow cathode discharge (MHCD). The MHCD is operated in the normal regime, with a DC discharge current of 1.6 mA and a plasma is ignited in a 20% Ar/ 80% N2 gas mixture. A 1-inch diameter aluminum substrate acting as a third electrode (second anode) is placed further away from the MHCD to emulate a deposition substrate. The spatial profile of the N atoms is measured in three MHCD configurations. First, we study a MHCD having the same pressure (50 mbar) on both sides of the anode/cathode electrodes and the N atoms diffuse in three dimensions from the MHCD. The recorded N atoms density profile in this case satisfies our expectations, i.e., the maximal density is found at the axis of the hole, close to the MHCD. However, when we introduce a pressure differential, thus creating a plasma jet, an unexpected N atoms distribution is measured with maximum densities away from the jet axis. This behavior cannot be simply explained by the TALIF measurements. Then, as a first simplified approach in this work, we turn our attention to the role of the gas flow pattern. Compressible gas flow simulations show a correlation between the jet width and the radial distribution of the N atoms at different axial distances from the gap. Finally, a DC positive voltage is applied to the third electrode (second anode), which ignites a Micro Cathode Sustained Discharge (MCSD). The presence of the pressure differential unveils two stable working regimes depending on the current repartition between the two anodes. The MCSD enables an homogenization of the density profile along the surface of the substrate, which is suitable for nitride deposition applications.
查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
三种 MHCD 配置中的绝对原子氮密度空间分布图
在这项工作中,我们利用纳秒双光子吸收激光诱导荧光对微型空心阴极放电(MHCD)中产生的氮原子绝对密度进行空间映射。微空心阴极放电在正常状态下运行,直流放电电流为 1.6 mA,在 20% Ar/80% N2 混合气体中点燃等离子体。直径为 1 英寸的铝基板作为第三电极(第二阳极)放置在离 MHCD 较远的地方,以模拟沉积基板。我们在三种 MHCD 配置中测量了 N 原子的空间分布。首先,我们研究了阳极/阴极电极两侧具有相同压力(50 毫巴)的 MHCD,N 原子从 MHCD 向三维扩散。在这种情况下记录到的 N 原子密度曲线符合我们的预期,即最大密度出现在靠近 MHCD 的孔轴线处。然而,当我们引入压差,从而产生等离子体射流时,测得的 N 原子密度分布却出乎意料地远离射流轴线。TALIF 测量无法简单地解释这种现象。然后,作为这项工作的第一种简化方法,我们将注意力转向气体流动模式的作用。可压缩气体流动模拟显示,在距离间隙不同的轴向距离上,射流宽度与 N 原子的径向分布之间存在相关性。最后,在第三个电极(第二个阳极)上施加直流正电压,点燃微阴极持续放电(MCSD)。压差的存在揭示了两种稳定的工作状态,这取决于两个阳极之间的电流分配。微阴极持续放电(MCSD)可使基底表面的密度分布均匀化,适用于氮化物沉积应用。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
自引率
0.00%
发文量
0
期刊最新文献
ThunderBoltz: an open-source direct simulation Monte Carlo Boltzmann solver for plasma transport, chemical kinetics, and 0D modeling Kinetic investigation of discharge performance for Xe, Kr, and Ar in a miniature ion thruster using a fast converging PIC-MCC-DSMC model Ground experimental study of the electron density of plasma sheath reduced by pulsed discharge Breakdown modes of capacitively coupled plasma: I. Transitions from glow discharge to multipactor Breakdown modes of capacitively coupled plasma: II. Non-self-sustained discharges
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:604180095
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1