离子注入诱导的 ALD TiO2 薄膜带隙改变

Shahbaz Afzal, Muhammad Usman, Aamenah Siddiqui, R. Y. Khosa, Anders Hallén
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摘要

原子层沉积(ALD)二氧化钛层被植入氮、氧和氩离子,以减小带隙,从而提高其在可见光区域的吸收率。植入是用 40 keV 氮离子、45 keV 氧离子和 110 keV 氩离子在 1 × 1015 至 5.6 × 1016 离子 cm-2 的通量范围内完成的。每个入射离子的能量都是通过物质中离子的停止和范围(SRIM)来调整的,以便在相同的投射范围内产生缺陷。通过 X 射线衍射(XRD)、扫描电子显微镜(SEM)、卢瑟福反向散射(RBS)和飞行时间弹性反冲探测分析(ToF-ERDA)对沉积薄膜进行结构分析。利用漫反射光谱(DRS)和傅立叶变换红外光谱(FTIR)对植入层进行表征,以研究薄膜的光学和振动特性。结果表明,氮植入 TiO2 后,反射率从 43.52% 降至 26.31%,带隙从 2.68 eV 降至 2.61 eV,使其成为太阳能电池应用中一种很有前途的带隙工程材料。在 1 × 1016 离子 cm-2 (N-16) 的条件下,40 keV 氮离子植入薄膜的折射率从≈2.8 增加到≈2.95。OPAL2 太阳能电池模拟显示,N-16 植入 TiO2 减反射涂层(ARC)可将吸收的光电流提高 7.3%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Ion Implantation‐Induced Bandgap Modifications in the ALD TiO2 Thin Films
Atomic layer deposited (ALD) TiO2 layers are implanted with N, O, and Ar ions to reduce the bandgap, thereby increasing its absorbance in the visible region. The implantation is accomplished with 40 keV nitrogen, 45 keV oxygen, and 110 keV argon ions in the fluence range 1 × 1015 to 5.6 × 1016 ions cm−2. The energy of each incident ion is tuned using stopping and range of ions in matter (SRIM) to produce defects around the same projected range. The structural analysis of the as‐deposited film is performed through X‐ray diffraction (XRD), scanning electron microscopy (SEM), Rutherford backscattering (RBS), and time of flight elastic recoil detection analysis (ToF‐ERDA). The implanted layers are characterized using diffuse reflectance spectroscopy (DRS) and Fourier transform infrared spectroscopy (FTIR) to study the optical and vibrational properties of the films. The results demonstrate that nitrogen implantation in TiO2 reduces the reflectance from 43.52% to 26.31% and bandgap from 2.68 to 2.61 eV, making it a promising bandgap‐engineered material for capping layers in solar cell applications. The refractive index of the 40 keV nitrogen ion implanted film at 1 × 1016 ions cm−2 (N‐16) increases from ≈2.8 to ≈2.95. OPAL2 solar cell simulations show that the N‐16 implanted TiO2 anti‐reflective coatings (ARC) can enhance the absorbed photocurrent by 7.3%.
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