预脉冲对激光锡等离子体极紫外转换效率的影响

J. Freeman, R. W. Coons, S. S. Harilal, S. Hassan, A. Hassanein
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引用次数: 0

摘要

极紫外(EUV)光刻技术正被考虑用于制造下一代计算机芯片。然而,必须确定一个合适的13.5 nm的EUV发射源。光源必须能够在带宽为2%的情况下提供可靠,清洁和强大的13.5 nm EUV发射,并能够满足大批量生产的需求。激光产生的等离子体(LPP)已成为极紫外光发射的一种有前景的光源,但首先必须实现更高的带内转换效率(CE)和碎片控制锡被认为是生产这种等离子体的首选材料,因为它的等离子体在EUV带内区域发射强烈,由不同的离子阶段(Sn8+ - Sn14+)贡献。然而,13.5 nm光子的净发射受到等离子体不透明度的控制,这取决于不同离子态的能级居群、电离平衡和电子密度。为了获得最高的CE,理想的等离子体温度和密度应该在尽可能长的时间内以最大的可收集尺寸产生预成型等离子体的再加热是控制密度从而优化等离子体不透明度以获得最大EUV发射的方法之一。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effects of pre-pulses on extreme ultraviolet conversion efficiency in laser-produced tin plasmas
Extreme ultraviolet (EUV) lithography is being considered for manufacturing the next generation of computer chips. However, a suitable source for EUV emission at 13.5 nm must be identified. The source must be able to provide reliable, clean, and powerful EUV emission at 13.5 nm with 2% bandwidth and be capable of meeting the demands of high volume manufacturing. Laser produced plasmas (LPP) have emerged as a promising source for EUV emission, but higher in-band conversion efficiency (CE) and debris control must first be realized.1 Tin is considered the material of choice for producing this plasma, as its plasma emits strongly in the EUV in-band region, contributed by various ionic stages (Sn8+ – Sn14+). However, the net emission of 13.5 nm photons is controlled by plasma opacity, which depends on level populations of different ionic states, ionization balance, and electron density. For obtaining the highest CE, ideal plasma temperatures and densities should be created for the longest possible period of time with the maximum collectable size.2 Reheating of a pre-formed plasma is one of the methods for controlling density and hence optimizing plasma opacity for maximum EUV emission.
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