Erosion of focus rings in capacitively coupled plasma etching reactors

薄脆饼 蚀刻(微加工) 等离子体 材料科学 离子 GSM演进的增强数据速率 反应离子刻蚀 等离子体刻蚀 电介质 电容 光电子学 电压 原子物理学 纳米技术 化学 电气工程 物理 图层(电子) 电极 工程类 核物理学 物理化学 电信 有机化学
作者
Xifeng Wang,Hyunjae Lee,Sang Ki Nam,Mark J. Kushner
出处
期刊:Journal of vacuum science & technology [American Institute of Physics]
卷期号:39 (6) 被引量:9
标识
DOI:10.1116/6.0001225
摘要

In plasma etching reactors, the structure surrounding the wafer, often called a focus ring (FR), plays an important role in maintaining uniform fluxes of reactants across the wafer. The FR is typically made of dielectric materials. During the plasma etching process, the sheath that forms over the wafer to accelerate ions anisotropically into the surface extends over the FR. Electrical charging of the FR modifies the sheath relative to that over the wafer. On the one hand, one wants the sheath to be uniform across the wafer-FR boundary to enable uniform fluxes to the edge of the wafer. On the other hand, maintaining a high voltage sheath over the FR will erode the FR, which is undesirable as the FR is a consumable component that must be periodically replaced in high volume manufacturing. In this work, we computationally investigated the consequences of dielectric constant ɛr of the FR materials on erosion of the FR. The series capacitance of the FR and its underlying structure is typically smaller than that of the wafer and its underlying structure. As a result, the FR charges quickly relative to the wafer, which then reduces the voltage across the sheath on top of the FR. The ion energy and angular distributions (IEADs) striking the FR are, therefore, generally lower in energy with a broader angular distribution. With ɛr = 2, the ion energies striking the middle to the outer edge of the FR are 30–180 eV, whereas for ɛr = 100, the ion energies are 120–380 eV. At the transition between the wafer and the FR, there is a skew in the IEAD as large as 15° that results from the difference in sheath thickness above the wafer and the FR. This skew and the erosion rate across the FR are functions of the dielectric constant of the FR material. With low ɛr, the FR charges quickly, less plasma is produced above the FR, and there is less voltage across the sheath that results in less FR erosion. Increasing ɛr of the FR produces a higher sheath voltage as well as higher ion fluxes over the FR, which increases erosion, while the skew at the edge of the wafer is less severe. The material of the subsurface portion of the FR, which dominates its capacitance, is an important consideration in the design of the substrate assembly.
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