下一代半导体制造面临的等离子蚀刻挑战

V. Rastogi, P. Ventzek, A. Ranjan
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引用次数: 1

摘要

在光刻工艺中,将必要的掩模布局印刷到聚合物层中。反过来,这一层被转移到底层的无机/有机材料层上,用于制造3D半导体和大批量集成芯片。摩尔定律描述了一种趋势,这种趋势在1965年首次被观察到,即这些布局中的模式尺寸每两年缩小一次,使微芯片上的晶体管数量增加一倍。光学光刻技术早已达到其物理极限(即印刷特征尺寸低于40nm),并且已经评估了许多替代印刷/材料沉积方案,以用于低于该极限的使用(见图1),以保持缩放的经济性。在这些方案中,等离子蚀刻(通过引发化学反应将印刷的掩模布局转移到底层)被广泛应用于工业。等离子体是部分电离的气体(即含有气体原子/分子、活化自由基和离子)。干等离子体蚀刻过程涉及自由基和暴露表面之间的相互作用,通过高能离子轰击导致活化/修饰层的去除/挥发。为了优化蚀刻工艺,可以通过调整适当的调谐旋钮来修改压力、气体流量/流量比、射频功率和衬底温度。当这些调谐旋钮中的一个被调整时,在多个等离子体参数(即自由基通量、离子通量、离子能量和离子能量分布)中触发变化。在连续等离子体蚀刻过程中,表面改性(活化)和高能材料去除(解吸)同时发生。然而,并发是有问题的,因为改变等离子体参数来改善印刷掩模传输的一个方面可能会降低图1。能够实现小于40nm特征尺寸的备选图纹方案:193nm浸没光刻结合自校准多重图纹;极紫外光刻;和定向自组装(DSA)。每种颜色代表不同的材料层。自对齐双图案。SAQP:自对齐四重图案。自对齐的八组模式
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Plasma etch challenges for next-generation semiconductor manufacturing
In the photolithography process, a requisite mask layout is printed into a polymer layer. This layer, in turn, is transferred onto underlying inorganic/organic material layers for the fabrication of 3D semiconductors, and for high-volume integrated-chip manufacturing. Moore’s law describes a trend, first observed in 1965, in which the dimension of patterns in these layouts shrinks every two years, doubling the number of transistors on the microchip. Optical lithography has long since reached its physical limit (i.e., printing feature sizes below 40nm), and a number of alternative printing/material deposition schemes have been evaluated for use below this limit (see Figure 1) to maintain the economy of scaling. Among these schemes, plasma etching (which transfers the printed mask layout onto underlying layers by initiating chemical reactions) is employed industrywide. Plasma is partially ionized gas (i.e., which contains gas atoms/molecules, activated radicals, and ions). The dry plasma etching process involves interactions—between radicals and the exposed surface—which lead to the removal/volatilization of the activated/modified layer via energetic ion bombardment. To optimize the etch process, the pressure, gas flow/flow ratios, radio frequency power, and substrate temperature can be modified by adjusting the appropriate tuning knobs. When one of these tuning knobs is adjusted, change is triggered in more than one of the plasma parameters (i.e., the radical flux, ion flux, ion energy, and ion energy distribution). In a continuous plasma-etch process, surface modification (activation) and energetic material removal (desorption) occur concurrently. Concurrence is problematic, however, because changing plasma parameters to improve one aspect of the printed mask transfer may degrade Figure 1. Alternative patterning schemes able to achieve feature sizes of less than 40nm: 193nm immersion lithography combined with selfaligned multiple patterning; extreme UV (EUV) lithography; and directed self-assembly (DSA). Each color represents a different material layer. SADP: Self-aligned double patterning. SAQP: Self-aligned quadruple patterning. SAOP: Self-aligned octuple patterning.1
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