Vazquez Jorge Luis, López Javier, Bohórquez Carolina, Lizarraga Eder, Blanco Eduardo, Can-Uc Bonifacio, Romo Oscar, Nedev Nicola, Farías Mario H, Tiznado Hugo
Centro de Investigación Científica y de Educación Superior de Ensenada-CICESE. Ensenada 22860, México.
Universidad Nacional Autónoma de México (UNAM), Centro de Nanociencias y Nanotecnología (CNyN), Km 107 Carretera Tijuana-Ensenada s/n, C.P. 22800, Ensenada 04510, Baja California, México.
ACS Appl Mater Interfaces. 2023 Aug 30;15(34):40942-40953. doi: 10.1021/acsami.3c07586. Epub 2023 Aug 17.
This research investigates the improvements of ozone (O) annealing on the optical and etching characteristics of TiO/AlO multilayer band-pass filters designed for potential optoelectronic applications. The band-pass filters were fabricated using atomic layer deposition (ALD), and their performance was systematically analyzed after the addition of O annealing at moderate temperatures (up to 300 °C). Results reveal that O annealing improves the optical transmittance of the multilayers by approximately 40% without significant spectral changes (∼6 nm). The observed enhancement in the transmittance is attributed to the improved stoichiometry of TiO. By filling in the oxygen vacancies created during the fabrication process, it reduces its extinction coefficient. Furthermore, the O annealing enhances the stability of TiO against wet etching, improving the uniformity of etched surfaces. Etching on the ozone-annealed multilayer was up to 8 times more homogeneous, as observed in the roughness. The relatively short duration of the O annealing process, approximately 1.6 h, makes it a cost-effective alternative compared to using ozone in the ALD process, which can last several hours for thick optical coatings.
本研究探讨了臭氧(O)退火对为潜在光电子应用设计的TiO/AlO多层带通滤波器的光学和蚀刻特性的改善情况。这些带通滤波器采用原子层沉积(ALD)制造,并在中等温度(高达300°C)下进行O退火后,系统地分析了它们的性能。结果表明,O退火可使多层膜的光学透过率提高约40%,且光谱变化不显著(约6纳米)。观察到的透过率增强归因于TiO化学计量比的改善。通过填充制造过程中产生的氧空位,降低了其消光系数。此外,O退火增强了TiO对湿法蚀刻的稳定性,改善了蚀刻表面的均匀性。如粗糙度所示,在臭氧退火的多层膜上进行蚀刻的均匀性提高了多达8倍。O退火过程持续时间相对较短,约1.6小时,与在ALD过程中使用臭氧相比,这使其成为一种经济高效的选择,后者对于厚光学涂层可能持续数小时。