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首页> 外文期刊>Journal of Vacuum Science & Technology. B, Microelectronics and Nanometer Structures >Studies of plasma surface interactions during short time plasma etching of 193 and 248 nm photoresist materials
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Studies of plasma surface interactions during short time plasma etching of 193 and 248 nm photoresist materials

机译:在193和248 nm光刻胶材料的短时等离子体蚀刻过程中等离子体表面相互作用的研究

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摘要

As the device dimensions scale to 100 nm, the use of photoresist materials is suitable for lithographic patterning at 193 nm. The molecular structure of 193 nm photoresist materials is significantly different from that of 248 nm photoresist materials [H. Ito, IBM J. Res. Deu. 45, 683 (2001), T. Kajita et al., Proc. SPIE 4345, 712 (2001)], which leads to a number of undesirable consequences, including pronounced surface and line edge roughness during plasma etching [H. Ito, IBM J. Res. Deu. 41, 69 (1997), [E. Reichmanis et al., J. Vac. Sci. Technol. B 15, 2528 (1997), [L. Ling et al., ibid. 22, 2594 (2004)]. In this article, we present an investigation of the mechanisms for the surface/line edge roughening of photoresist materials during plasma etching using C4F8/90% Ar discharges. We emphasized in our study short exposure times (the first few seconds) of the photoresist materials and structures to the plasma, a time regime that has not been well studied. Rapid modifications were observed for both 193 and 248 nm photoresists during short time exposure. During the first seconds of plasma exposure, photoresist material densification and hydrogen depletion are important processes. It is also found that rough surfaces develop within a few seconds of exposure to the C4178/90% Ar discharges. Plasma exposure leads to the formation of rough edges on the top of trench sidewalls in photoresist trench and line structures. During prolonged exposure to the plasma, the roughness is transferred to produce striations on the sidewalls. After an initial stage, the roughening rate remains constant for 193 nm photoresist, whereas for 248 nm photoresist the roughening rate is negligible. This difference is possibly related to the preferential removal of carbonyl groups for the 193 nm photoresist material, which has been revealed by x-ray photoelectron spectroscopy and seconday ion mass spectroscopy. (c) 2006 American Vacuum Society.
机译:当器件尺寸扩展到100 nm时,使用光致抗蚀剂材料适合在193 nm处进行光刻构图。 193 nm光刻胶材料的分子结构与248 nm光刻胶材料的分子结构显着不同[H.伊藤,IBM J. Res。杜T.Kajita等人,Proc.Natl.Acad.Sci.USA,45:683(2001)。 SPIE 4345,712(2001)],这会导致许多不良后果,包括在等离子蚀刻过程中明显的表面和线边缘粗糙度[H.伊藤,IBM J. Res。杜41,69(1997),[E. Reichmanis等人,J。Vac。科学技术。 B 15,2528(1997),[L。 Ling等,同上。 22,2594(2004)]。在本文中,我们对使用C4F8 / 90%Ar放电进行等离子刻蚀期间光致抗蚀剂材料的表面/线条边缘粗糙化的机理进行了研究。我们在研究中强调了光致抗蚀剂材料和结构对等离子体的短曝光时间(前几秒钟),这种时间范围尚未得到很好的研究。在短时间曝光期间,对于193和248 nm光刻胶均观察到快速改性。在等离子暴露的最初几秒钟内,光刻胶材料的致密化和氢耗竭是重要的过程。还发现在暴露于C4178 / 90%Ar放电的几秒钟内会形成粗糙的表面。等离子体暴露导致在光致抗蚀剂沟槽和线结构中的沟槽侧壁的顶部上形成粗糙边缘。在长时间暴露于等离子体的过程中,粗糙度被转移以在侧壁上产生条纹。在初始阶段之后,对于193 nm光刻胶,粗糙化速率保持恒定,而对于248 nm光刻胶,粗糙化速率可以忽略不计。这种差异可能与193 nm光致抗蚀剂材料的羰基优先去除有关,这已通过X射线光电子能谱和二次离子质谱得到了证实。 (c)2006年美国真空学会。

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