Ghezzi Francesco, Pedroni Matteo, Kovač Janez, Causa Federica, Cremona Anna, Anderle Mariano, Caniello Roberto, Pietralunga Silvia M, Vassallo Espedito
Istituto per la Scienza e Tecnologia dei Plasmi CNR, Via R. Cozzi 53, Milano 20125, Italy.
Jozef Stefan Institute, Jamova cesta 39, Ljubljana 1000, Slovenia.
ACS Omega. 2022 Jul 11;7(29):25600-25612. doi: 10.1021/acsomega.2c02740. eCollection 2022 Jul 26.
The process of deep texturization of the crystalline silicon surface is intimately related to its promising diverse applications, such as bactericidal surfaces for integrated lab-on-chip devices and absorptive optical layers (black silicon-BSi). Surface structuring by a maskless texturization appeals as a cost-effective approach, which is up-scalable for large-area production. In the case of silicon, it occurs by means of reactive plasma processes (RIE-reactive-ion etching) using fluorocarbon CF and H as reaction gases, leading to self-assembled cylindrical and pyramidal nanopillars. The mechanism of silicon erosion has been widely studied and described as it is for the masked RIE process. However, the onset of the erosion and the reaction kinetics leading to defined maskless patterning have not been unraveled to date. In this work, we specifically tackle this issue by analyzing the results of three different RIE recipes, specifically designed for the purpose. The mechanism of surface self-nanopatterning is revealed by deeply investigating the physical chemistry of the etching process at the nanoscale and the evolution of surface morphology. We monitored the progress in surface patterning and the composition of the etching plasma at different times during the RIE process. We confirm that nanopattering issues from a net erosion, as contributed by chemical etching, physical sputtering, and by the synergistic plasma effect. We propose a qualitative model to explain the onset, the evolution, and the stopping of the process. As the RIE process is started, a high density of surface defects is initially created at the free silicon surface by energetic ion sputtering. Contextually, a polymeric overlayer is synthesized on the Si surface, as thick as 5 nm on average, and self-aggregates into nanoclusters. The latter phenomenon can be explained by considering that the initial creation of surface defects increases the activation energy for surface diffusion of deposited CF and CF species and prevents them from aggregating into a continuous Volmer-Weber polymeric film. The clusterization of the polymer provides the self-masking effect since the beginning, which eventually triggers surface patterning. Once started, the maskless texturing proceeds in analogy with the masked case, that is, by combined chemical etching and ion sputtering, and ceases because of the loss of ion energy. In the case of CF/H RIE processes at 10% of H and by supplying 200 W of RF power for 20 min, nanopillars of 200 nm in height and 100 nm in width were formed. We therefore propose that a precise assessment of surface defect formation and density in dependence on the initial RIE process parameters can be the key to open a full control of outcomes of maskless patterning.
晶体硅表面的深度纹理化过程与其多种有前景的应用密切相关,例如用于集成芯片实验室设备的杀菌表面和吸收性光学层(黑硅 - BSi)。通过无掩膜纹理化进行表面结构化是一种具有成本效益的方法,可扩展用于大面积生产。对于硅而言,这是通过使用碳氟化合物CF和H作为反应气体的反应性等离子体工艺(RIE - 反应离子蚀刻)来实现的,从而形成自组装的圆柱形和金字塔形纳米柱。硅侵蚀的机制已得到广泛研究,与有掩膜RIE工艺的情况类似。然而,侵蚀的起始以及导致确定的无掩膜图案化的反应动力学至今尚未阐明。在这项工作中,我们通过分析专门为此目的设计的三种不同RIE配方的结果来具体解决这个问题。通过深入研究纳米尺度蚀刻过程的物理化学以及表面形态的演变,揭示了表面自纳米图案化的机制。我们在RIE过程中的不同时间监测了表面图案化的进展以及蚀刻等离子体的成分。我们确认纳米图案化源于化学蚀刻、物理溅射以及协同等离子体效应所导致的净侵蚀。我们提出了一个定性模型来解释该过程的起始、演变和停止。随着RIE过程开始,通过高能离子溅射在自由硅表面最初产生高密度的表面缺陷。在此背景下,在硅表面合成了平均厚度达5 nm的聚合物覆盖层,并自聚集形成纳米团簇。后一种现象可以通过考虑表面缺陷的初始产生增加了沉积的CF和CF物种表面扩散的活化能,并阻止它们聚集成连续的伏默 - 韦伯聚合物膜来解释。聚合物的团簇化从一开始就提供了自掩膜效应,最终触发表面图案化。一旦开始,无掩膜纹理化的进行方式与有掩膜情况类似,即通过化学蚀刻和离子溅射相结合,并由于离子能量的损失而停止。在H含量为10%且提供200 W射频功率持续20分钟的CF/H RIE工艺中,形成了高度为200 nm、宽度为100 nm的纳米柱。因此,我们提出,根据初始RIE工艺参数精确评估表面缺陷的形成和密度可能是全面控制无掩膜图案化结果的关键。