Mueller matrix spectroscopic ellipsometry based scatterometry simulations of Si and Si/SixGe1-x/Si/SixGe1-x/Si fins for sub-7nm node gate-all-around transistor metrology

S. Dey, A. Diebold, Nick Keller, M. Korde
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引用次数: 5

Abstract

In this paper, we report on Muller Matrix (MM) based scatterometry (aka. optical critical dimension or OCD) simulation strategies for two sub-7nm fin structures: one with a SixGe1-x/Si/SixGe1-x/Si/SixGe1-x/Si nanosheet structure and its comparison with a hypothetical Si-only fin structure of similar dimensions at sub-7nm semiconductor technology nodes. Si-fins are providing the performance improvements necessary for the transistors used in current generation integrated circuits. Development of sub-7nm technology nodes requires further performance improvements including advanced structures including new materials. This demand for improved performance has created the need for new fabrication processes such as extreme ultraviolet lithography, self-aligned quadruple patterning etc., along with new metrology challenges for adequately monitoring the semiconductor process control during fabrication of these advanced nanostructures.1 New materials and structures, such as, Si/Si1-xGex (0≤x≤1) stacked nanosheet structures have recently been developed as one of the potential replacement for Si-based FinFETs.2,3 We have simulated two fin structures: one with Si-fins and another with 3 alternating stacks of Si1-xGex/Si (x=0.3). We have used Rigorous Coupled Wave Approximation (RCWA) to simulate OCD spectra for 0° – 360° azimuthal angles in 10° steps by keeping the fin pitch fixed at 24nm while systematically changing (1) the fin critical dimension (CD) from 5.0–7.5nm in 0.5nm steps, (2) thickness of the Si and Si1-xGex (x=0.3) nanosheets (NST) from 8.0–1.5nm in 0.5nm steps, (3) the fin bending angle (FBA) from 0°–2.5° in 0.5° steps, and (4) the undercut angle (ED) of the Si1-xGex NSTs from 0°–10° in 2° steps. Difference in etch-rate of Si and Ge could give rise to non-zero ED during NST formation. Both the fin structures possess mirror symmetry about two orthogonal planes perpendicular to the substrate and with one of the planes along the fin long-axis. For angles 0°, 90°, 180°, and 270°, this mirror symmetry leads to absence of the cross-polarization terms in the simulated OCD spectra such that off-diagonal MM elements are zero over the simulated wavelength range. The broken mirror symmetry in other azimuthal angles leads to cross-polarization of the electrical field vectors which is seen in the off-diagonal MM elements becoming non-zero. Additionally, the off-diagonal MM elements show increased sensitivity and reduced correlation between the parameters under study which leads to a powerful metrology means for studying the critical fin-parameters for fast and reliable semiconductor process control in sub 7-nm technology nodes. All the non-zero MM-elements are found to be sensitive to changes in CD and NST with the off-diagonal elements showing greater sensitivity to the changes. At azimuthal angles <15°, MM23, MM31, and MM34 are highly sensitive to changes in etch undercut and fin bending angle defects. References: [1] D. Dixit et al., “Advanced applications of scatterometry based optical metrology,” Proc SPIE 10145, 101451H (2017). [2] N. Loubet et al., “Stacked nanosheet gate-all-around transistor to enable scaling beyond FinFET,” VLSI Technol. 2017 Symp., T230–T231, IEEE (2017). [3] R. Muthinti et al., “Advanced in-line optical metrology of sub-10nm structures for gate all around devices (GAA),” Proc SPIE 9778, 977810 (2016).
基于Mueller矩阵椭圆偏振散射法的Si和Si/SixGe1-x/Si/SixGe1-x/Si鳍片的亚7nm节点栅全能晶体管测量模拟
在本文中,我们报告了基于穆勒矩阵(MM)的散射测量法。两种亚7nm鳍片结构的光学临界尺寸(OCD)模拟策略:一种是具有SixGe1-x/Si/SixGe1-x/Si/SixGe1-x/Si纳米片结构,以及它与在亚7nm半导体技术节点上具有相似尺寸的假设的仅Si鳍片结构的比较。硅鳍为当前一代集成电路中使用的晶体管提供了必要的性能改进。亚7nm技术节点的发展需要进一步的性能改进,包括包括新材料在内的先进结构。这种对改进性能的需求创造了对新制造工艺的需求,如极紫外光刻,自对准四重图案等,以及在这些先进纳米结构制造过程中充分监测半导体工艺控制的新计量挑战新的材料和结构,如Si/Si1-xGex(0≤x≤1)堆叠纳米片结构,最近被开发为Si基finfet的潜在替代品之一。2,3我们模拟了两种翅片结构:一种是硅鳍,另一种是硅- xgex /Si (x=0.3)的3个交替堆叠。我们使用严格的耦合波近似(RCWA)为0°- 360°模拟强迫症谱方位角度在10°步骤保持鳍片固定在24海里而系统地改变(1)鳍临界尺寸(CD)从5.0 -7.5 0.5 nm的步骤,(2)如果厚度和Si1-xGex (x = 0.3) nanosheets(望远镜)从8.0 -1.5 0.5 nm的步骤,(3)鳍弯曲角(FBA)从0°-2.5°0.5°的步骤,和(4)的削弱角(ED) Si1-xGex望远镜从0°-10°在2°步骤。在NST形成过程中,Si和Ge腐蚀速率的差异会导致非零ED的产生。这两种翅片结构都具有关于垂直于基片的两个正交平面和沿鳍长轴的一个平面的镜像对称性。对于0°、90°、180°和270°的角度,这种镜面对称导致模拟OCD光谱中缺少交叉极化项,从而使非对角线MM元素在模拟波长范围内为零。其他方位角的镜面对称性的破坏导致电场矢量的交叉极化,这在非对角线MM元件中看到变为非零。此外,非对角线MM元件显示出更高的灵敏度和研究参数之间的相关性降低,这使得研究关键鳍参数在亚7纳米技术节点上快速可靠的半导体工艺控制成为一种强大的计量手段。所有非零mm单元对CD和NST的变化都很敏感,而非对角线单元对CD和NST的变化更敏感。在方位角<15°时,MM23、MM31和MM34对蚀刻下切和鳍弯曲角度缺陷的变化高度敏感。参考文献:[1]D. Dixit et al.,“基于散射测量的光学测量技术的先进应用”,中国光学工程学报,10145,101451h (2017).[1]N. Loubet et al.,“堆叠纳米片栅极全能晶体管实现超越FinFET的缩放”,VLSI technology, 2017年第1期。[j] .光学精密工程,2013 (5):442 - 442陈志强,“基于光学测量的亚10nm栅极器件(GAA)测量方法”,电子工程学报,2016,32(6)。
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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