The Mechanism of the desire process

B. Roland, R. Lombaerts, F. Coopmans
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引用次数: 18

Abstract

As we enter the megabit era the demands on the performance of lithographic processes are dramatically increased. Achieving submicron resolution with sufficient line width control on substrates with reflective topography is becoming a major problem. One way of solving most of the problems that are encountered in optical submicron lithography is by so called multilayer resist techniques [1]. Although excellent results can be obtained by this method it has the serious disadvantage of being too complicated for IC production lines. It is thus not surprising that much effort has been put into the development of simpler alternatives, such as the bilayer RIE/PCM resist scheme [2], in which a silicon containing resist is used as top layer. However, the major disadvantage of these systems is that by incorporating a sufficient amount of silicon in the resist material, its physical properties tend to degrade.
欲望过程的机制
随着我们进入兆比特时代,对光刻工艺性能的要求急剧增加。在具有反射地形的基板上实现具有足够线宽控制的亚微米分辨率已成为一个主要问题。解决光学亚微米光刻中遇到的大多数问题的一种方法是采用所谓的多层抗蚀剂技术。这种方法虽然可以获得良好的效果,但对于集成电路生产线来说,其缺点是过于复杂。因此,人们投入大量精力开发更简单的替代品也就不足为奇了,比如双层RIE/PCM抗蚀剂方案[2],其中含硅抗蚀剂被用作顶层。然而,这些系统的主要缺点是,通过在抗蚀剂材料中加入足够数量的硅,其物理性能趋于退化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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