Tracing optimized condition for electron beam metrology of EUV photoresist pattern using low-landing energy

抵抗 极紫外光刻 收缩率 计量学 平版印刷术 光刻胶 电子束光刻 材料科学 光学 X射线光刻 临界尺寸 光刻 扫描电子显微镜 下一代光刻 极端紫外线 光电子学 纳米技术 物理 复合材料 激光器 图层(电子)
作者
Woo‐Sik Jung,Jong-Hoi Cho,SungHun Lim,TaeSeop Lee,Daeyoung Choi,Jong-Hyun Seo,Seung–Hyun Lee,JunKyoung Lee,You Jin Kim,Jeong Ho Yeo,Alex Brikker,Roi Meir,Ran Alkoken,Kyeongju Han,Seung Woon Lim,KyungJae Choi,Chanhee Kwak,Hyeon Sang Shin
标识
DOI:10.1117/12.2660114
摘要

With the extreme ultraviolet (EUV) lithography and its pitch scaling, the resist shrinkage from electron beam has returned to an important critical dimension (CD) control issue—unlike multi-patterning where the smallest CD is larger than 40nm. The resist height reduces to maintain the aspect ratio below 2:1 which is critical factor for the prevention of the resist collapse. This leads to huge challenges to minimize the shrinkage of resist during the scanning electron microscope (SEM) measurement. Accurate and precise metrology of chemically amplified resist (CAR) type EUV photoresist processed pattern utilizing classical beam energy for lithography pattern such as 500V is great challenging as electron beam exposure of 1st measurement already fully shrunk the pattern. Moreover, occurrence of carbonization along with shrinkage hinders finding best conditions for not only metrology optimization but also minimized process impact. In this work, we evaluated the magnitude of shrinkage of CAR type EUV photoresists with several approaches including 0th and 1st shrinkage estimation utilizing line & space pattern and contact hole pattern as a function of landing energy dose and static/dynamic repeatability method to distinguish behaviors of shrinkage and carbonization by controlling interaction time of photoresist to its environment. One approach to trace minimized 0th shrinkage and metrology uncertainty in lithography process is utilizing 1st shrinkage (1st CD – 2nd CD) analysis together with plotting absolute value of the 1st CD as a function of dose. The other approach to trace optimization condition was comparing exposed area with electron beam and non-exposed area achieved by comparing litho/etch consecutive process on the same area. Furthermore, model fits, a simulation study were also performed.
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