利用计算光刻技术集成半导体器件

Photomask Japan Pub Date : 2021-08-23 DOI:10.1117/12.2600797
Tsuyoshi Arai, S. Aihara, Yuichiro Oguchi, J. Seki, Y. Matsuoka
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引用次数: 0

摘要

压印光刻是一种有效且众所周知的纳米级特征复制技术。纳米压印(NIL)制造设备采用了一种图案化技术,该技术包括逐场沉积和通过喷射技术将低粘度抗蚀剂沉积到基板上。有图案的口罩被放入液体中,然后通过毛细管作用迅速流入口罩中的浮雕图案。在这个填充步骤之后,抗蚀剂在紫外线辐射下交联,然后去除掩模,在基材上留下图案抗蚀剂。与光刻设备相比,该技术以更高的分辨率和更大的均匀性忠实地再现图案。此外,由于该技术不需要宽直径透镜阵列和先进光刻设备所需的昂贵光源,因此NIL设备实现了更简单,更紧凑的设计,允许多个单元聚集在一起以提高生产率。先前的研究表明,NIL分辨率优于10nm,这使得该技术适用于用单个掩模打印几代关键记忆级。此外,仅在必要时应用抗蚀剂,从而消除了材料浪费。NIL的计算技术仍处于发展过程中。只有少数模拟器适用于纳米压印工艺,这些模拟器是设备制造商希望作为他们的日常工具箱的一部分。NIL过程仿真中最具挑战性的问题是系统各组成部分的尺度差异。模板图案深度和残余抗蚀剂膜厚度一般为几十纳米,而该工艺需要在整个镜头尺寸上工作,通常为10毫米见方。这相当于106数量级的比例差异。因此,为了利用传统的流体结构相互作用(FSI)模拟器计算纳米压印过程,需要大量的网格,这导致计算时间难以接受。本文介绍了一种新的工艺模拟器,它可以直接输入工艺参数,模拟整个压印过程,并对所得到的抗蚀膜的质量进行评价。为了克服尺度差异,我们的模拟器采用了解析积分表达式,减少了计算区域的尺寸。此外,该模拟器可以独立考虑液滴的位置并计算液滴的聚并,从而预测液滴之间被困气体产生的非填充区域的分布。该仿真器已应用于实际的零空系统中,并给出了一些应用实例。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
NIL integration using computational lithography for semiconductor device manufacturing
Imprint lithography is an effective and well-known technique for replication of nano-scale features. Nanoimprint lithography (NIL) manufacturing equipment utilizes a patterning technology that involves the field-by-field deposition and exposure of a low viscosity resist deposited by jetting technology onto the substrate. The patterned mask is lowered into the fluid which then quickly flows into the relief patterns in the mask by capillary action. Following this filling step, the resist is crosslinked under UV radiation, and then the mask is removed, leaving a patterned resist on the substrate. The technology faithfully reproduces patterns with a higher resolution and greater uniformity compared to those produced by photolithography equipment. Additionally, as this technology does not require an array of wide-diameter lenses and the expensive light sources necessary for advanced photolithography equipment, NIL equipment achieves a simpler, more compact design, allowing for multiple units to be clustered together for increased productivity. Previous studies have demonstrated NIL resolution better than 10nm, making the technology suitable for the printing of several generations of critical memory levels with a single mask. In addition, resist is applied only where necessary, thereby eliminating material waste. Computational technologies are still in the course of development for NIL. Only a few simulators are applicable to the nanoimprint process, and these simulators are desired by device manufacturers as part of their daily toolbox. The most challenging issue in NIL process simulation is the scale difference of each component of the system. The template pattern depth and the residual resist film thickness are generally of the order of a few tens of nanometers, while the process needs to work over the entire shot size, which is typically of the order of 10 mm square. This amounts to a scale difference of the order of 106. Therefore, in order to calculate the nanoimprint process with conventional fluid structure interaction (FSI) simulators, an enormous number of meshes is required, which results in computation times that are unacceptable. In this paper, we introduce a new process simulator which directly inputs the process parameters, simulates the whole imprinting process, and evaluates the quality of the resulting resist film. To overcome the scale differences, our simulator utilizes analytically integrated expressions which reduce the dimensions of the calculation region. In addition, the simulator can independently consider the positions of the droplets and calculate the droplet coalescence, thereby predicting the distribution of the non-fill areas which originate from the trapped gas between the droplets. The simulator has been applied to the actual NIL system and some examples of its applications are presented in this work.
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