Immersion ellipsometry for the uncorrelated determination of ultrathin film thickness and index of refraction: Theory and examples

Samira Jafari, Blaine Johs, M. Linford
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Abstract

Immersion ellipsometry can break the well-known correlation between optical constants and thicknesses of ultrathin (<5–10 nm) films, allowing both to be determined. In immersion ellipsometry, ellipsometric data is acquired in air and liquid ambients, and the data sets are combined in the analysis. The contrast in index between the liquid and film adds information to the analysis that breaks the correlation between the film thickness and refractive index that exists for air-only measurements. We describe the theory and practice of immersion ellipsometry. We also discuss the use of multiwavelength immersion ellipsometry to measure the thicknesses and optical constants of two thin films: native oxide on silicon and an alkyl monolayer on that native oxide. The average thicknesses of the native oxide and chloro(dimethyl)octadecylsilane (CDMOS) monolayer were 1.526 ± 0.027 nm and 1.968 ± 0.057 nm, and their average indices of refraction at 633 nm were 1.519 ± 0.005 and 1.471 ± 0.004, respectively. The native oxide and CDMOS monolayer were also characterized with x-ray photoelectron spectroscopy (XPS) and contact angle goniometry. Both the XPS C 1 s peak and the water contact angle increased substantially after monolayer deposition. While immersion ellipsometry has been known for decades, its use has been limited, maybe due to a lack of awareness of the technique and/or the need to immerse the sample surface in a liquid that could be destructive if the sample is not compatible with the liquid. As ultrathin films become widely used in science technology, immersion ellipsometry should increase in importance.
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用于无关联测定超薄薄膜厚度和折射率的浸入式椭偏仪:理论与实例
浸入式椭偏仪可以打破超薄(<5-10 nm)薄膜的光学常数与厚度之间众所周知的相关性,从而可以同时测定两者。在浸入式椭偏仪中,椭偏仪数据分别在空气和液体环境中采集,并将数据集合并进行分析。液体和薄膜之间的折射率对比为分析增加了信息,打破了纯空气测量中薄膜厚度和折射率之间的相关性。我们介绍了浸入式椭偏仪的理论和实践。我们还讨论了使用多波长浸入式椭偏仪测量两层薄膜的厚度和光学常数:硅上的原生氧化物和原生氧化物上的烷基单层。原生氧化物和氯(二甲基)十八烷基硅烷(CDMOS)单层的平均厚度分别为 1.526 ± 0.027 nm 和 1.968 ± 0.057 nm,它们在 633 nm 波长处的平均折射率分别为 1.519 ± 0.005 和 1.471 ± 0.004。原生氧化物和 CDMOS 单层还利用 X 射线光电子能谱(XPS)和接触角测角仪进行了表征。单层沉积后,XPS C 1 s 峰值和水接触角都大幅增加。虽然浸入式椭偏仪已经有几十年的历史,但其应用一直很有限,这可能是由于人们对该技术缺乏了解,以及/或需要将样品表面浸入液体中,如果样品与液体不兼容,就会造成破坏。随着超薄薄膜在科学技术中的广泛应用,浸入式椭偏仪的重要性应该会增加。
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