高速蚀刻用微波等离子体源的建模与研究

Steffen Pauly, A. Schulz, M. Walker, G. Tovar, M. Balk, Joachim Schneider, K. Baumgärtner
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摘要

该研究的目的是优化现有的微波远程等离子体源(RPS)的蚀刻速率和气体温度,并简化设置以节省生产成本。RPS如图1所示,是一种低压等离子体源,等离子体主要产生于源腔内。只有自由基迁移出RPS。这是一个重要的特点,等离子体源用于蚀刻工艺时,必须防止离子轰击和高热应变的衬底。蚀刻过程是一个化学过程,其中自由基与衬底表面原子反应形成气体分子。其优点是无损伤,干燥和清洁的基材表面。为了实现这些目标,建立了一个基于有限元的RPS模型来研究微波分布和等离子体腔内的微波耦合以及等离子体本身。本文将给出不同条件下基于有限元法的微波模拟实例及其实验验证。为了将计算得到的RPS内电场分布与实际电场分布进行比较,在源的等离子体腔内放置pmma基板。它们被电场加热,然后用红外摄像机和液晶片进行评估。实测的场分布与计算的场分布具有很好的一致性。当等离子体腔内的电场足够大时,等离子体被点燃,电子密度随之增加,介电常数和电导率也随之增加,这又改变了电场的分布。为此,fem模型被扩展为Drude模型1。该模型考虑带有电子阻尼项的运动方程,从而得到电导率的表达式。给出了不同电子密度及其对应的电场分布的结果,并与光学测量结果进行了比较。图1所示。图中显示了RPS的方案及其主要组成部分和功能。
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Modelling and Study of a Microwave Plasma Source for High-rate Etching
The aim of the study is to optimize an existing microwave powered remote plasma source (RPS) with respect to the etching rate and gas temperature and to simplify the setup to save production costs. The RPS, which is shown in figure 1, is a low-pressure plasma source where the plasma is generated and exists mainly in the chamber of the source. Only radicals migrate out of the RPS. This is one important feature, that the plasma source is used for etching processes when ion bombardment and high thermal strain of the substrate must be prevented. The etching process is a chemical process, where the radicals react with the substrate surface atoms forming gaseous molecules. The benefit is a damage-free, dry and clean substrate surface. To achieve these goals, a FEM-based model of the RPS has been developed to investigate the microwave distribution and the microwave coupling into the plasma chamber, as well as the plasma itself. In this paper different examples of FEM based microwave simulations by different conditions and their experimental validations will be presented. To compare the calculated electric field distribution in the RPS with the real field distribution, PMMA-substrates were placed inside the plasma chamber of the source. They are heated up by the electric field and evaluated with an infrared camera and liquid crystal sheets. Both the measured and the calculated field distribution show a very good conformity. When the electric field is high enough in the plasma chamber the plasma ignites, the electron density and thus the permittivity and the conductivity increase, which changes again the electric field distribution. For this purpose, the FEM-model has been extended by the Drude model1. The model considers the equation of motion with a damping term for the electrons, leading to an expression for the conductivity. Results for various electron densities as well as their corresponding electric field distributions are presented and compared with optical measurements.     Fig. 1. The figure shows the scheme of the RPS with its main components and functions.
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