No-heating deposition of ferroelectric epitaxial Hf0.5Zr0.5O2 films using a sputtering method with precise RF power density and thickness control

材料科学 正交晶系 铁电性 溅射沉积 沉积(地质) 溅射 外延 单斜晶系 光电子学 相(物质) 功率密度 Crystal(编程语言) 射频功率放大器 薄膜 腔磁控管 氧化铟锡 立方氧化锆 分析化学(期刊) 单晶
作者
Takanori Mimura,Yoshiko Nakamura,Y. Tsuchiya,K. Okamoto,Hiroshi Funakubo
出处
期刊:Journal of Materiomics [Elsevier BV]
卷期号:12 (1): 101129-101129
标识
DOI:10.1016/j.jmat.2025.101129
摘要

The no-heating deposition of (111)-oriented epitaxial (Hf 0.5 Zr 0.5 )O 2 films was successfully achieved on (111) indium tin oxide//(111) yttria-stabilized zirconia substrates using a radio-frequency (RF) magnetron sputtering method. As the RF power density was increased, the crystal phase changed sequentially from the tetragonal, the orthorhombic, and then to the monoclinic phase. A similar trend in the crystal phase was also observed with increasing film thickness. The (Hf 0.5 Zr 0.5 )O 2 film exhibited ferroelectric properties comparable to the (Y 0.07 Hf 0.93 )O 2 film previously produced via non-heating film deposition. Upon heat treatment at 1000 °C, the crystal phase of the film transitioned from the orthorhombic phase to the monoclinic phase, indicating that the stability of the orthorhombic phase is low compared with (Y 0.07 Hf 0.93 )O 2 . Therefore, precise control of the RF power density and film thickness is essential for preparing ferroelectric (Hf 0.5 Zr 0.5 )O 2 films without heating. • No-heating deposition of (111)-oriented ferroelectric (Hf 0.5 Zr 0.5 )O 2 films was achieved by RF magnetron sputtering method. • Precise control of the RF power density and film thickness was important to obtain the ferroelectric orthorhombic phase. • Ferroelectric properties of no-heating deposited (Hf 0.5 Zr 0.5 )O 2 films were comparable to those of (Y 0.07 Hf 0.93 )O 2 films.
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