Complexities in the growth and stabilization of polar phase in the Hf$_{0.5}$Zr$_{0.5}$O$_2$ thin films grown by Pulsed Laser Deposition

Deepak Kumar
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Abstract

After the discovery of ferroelectricity in HfO$_2$ based thin films a decade ago, ferroelectric Hf$_{0.5}$Zr$_{0.5}$O$_2$ (HZO) thin films are frequently being utilized in the CMOS (Complementary Metal- Oxide Semiconductor) and logic devices, thanks to their large remnant polarization, high retention and endurance. A great deal of effort has been made towards understanding the origin of ferroelectricity in epitaxial HZO thin films and controlling the microstructure at the atomic level which governs the ferroelectric phase. Nevertheless, the HZO films still suffer from fundamental questions, such as (1) the vagueness of interfacial mechanisms between HZO, buffer layer and the substrate which controls the polar phase; (2) the nature of the metastable polar phase responsible for the ferroelectricity, be it orthorhombic or rhombohedral; which are poorly understood. Here, we have addressed these issues by employing the in-situ reflection high energy electron diffraction -- assisted pulsed laser deposition and mapping the asymmetrical polar maps on high quality HZO films grown on functional perovskite oxide substrates. The interface between La$_{0.7}$Sr$_{0.3}$MnO$_3$ (LSMO) and the substrate is shown to be quite important, and a slightly rougher interface of the former destabilizes the ferroelectric phase of HZO irrespective of well-controlled growth of the ferroelectric layers. A rhombohedral-like symmetry of HZO unit cell is extracted through the x-ray diffraction asymmetrical polar maps. The ferroelectric measurements on a nearly 7 nm HZO film on STO(001) substrate display a remnant polarization close to 8 uC/cm$^2$. These results highlight the complexities involved at the atomic scale interface in the binary oxides thin films and can be of importance to the HfO$_2$-based ferroelectric community which is still at its infancy.
脉冲激光沉积法生长的 Hf$_{0.5}$Zr$_{0.5}$O$_2$ 薄膜中极性相的生长和稳定过程的复杂性
自十年前在基于 HfO$_2$ 的薄膜中发现铁电性后,铁电 Hf$_{0.5}$Zr$_{0.5}$O$_2$ (HZO) 薄膜因其残余极化大、保持率高和耐久性强而被频繁用于 CMOS(互补金属氧化物半导体)和逻辑器件中。为了了解外延 HZO 薄膜铁电性的起源,并在原子水平上控制其微观结构,从而控制铁电相,人们付出了巨大的努力。然而,HZO 薄膜仍然存在一些基本问题,例如:(1)HZO、缓冲层和基底之间控制极性相的界面机制不明确;(2)对铁电性负责的可转移极性相的性质(无论是正交还是斜交)不甚了解。在这里,我们利用原位反射高能电子衍射辅助脉冲激光沉积技术解决了这些问题,并绘制了生长在功能性过氧化物基底上的高质量 HZO 薄膜的非对称极性图。结果表明,La$_{0.7}$Sr$_{0.3}$MnO$_3$ (LSMO) 与基底之间的界面相当重要,前者稍粗糙的界面会破坏 HZO 铁电相的稳定性,无论铁电层的生长是否良好。通过 X 射线衍射非对称极坐标图,可以提取出 HZO 单元电池的斜方体对称性。在 STO(001)基底上对近 7 nm 的 HZO 薄膜进行的铁电测量显示,残余极化接近 8 uC/cm$^2$。这些结果凸显了二元氧化物薄膜中原子尺度界面的复杂性,对仍处于起步阶段的基于 HfO$_2$ 的铁电群体具有重要意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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