三种 MHCD 配置中的绝对原子氮密度空间分布图

A. Remigy, Belkacem Menacer, Konstantinos Kourtzanidis, Odyssea Gazeli, K. Gazeli, G. Lombardi, C. Lazzaroni
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引用次数: 0

摘要

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。
Absolute atomic nitrogen density spatial mapping in three MHCD configurations
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.
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