Editorial: Advanced characterization methods for HfO2/ZrO2-based ferroelectrics

IF 4.1 Q2 MATERIALS SCIENCE, MULTIDISCIPLINARY Frontiers in Nanotechnology Pub Date : 2023-01-24 DOI:10.3389/fnano.2023.1114267
P. Lomenzo, U. Celano, T. Kämpfe, S. Mcmitchell
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Abstract

Ferroelectric HfO2 and ZrO2-based materials are unconventional ferroelectrics compared to historically dominant perovskite-based ferroelectrics. These differences from conventional perovskite ferroelectrics are distinctly seen in HfO2-ZrO2’s fluorite-based structure that exhibits a rich polymorphism of competing crystal phases, enhanced ferroelectric behavior when scaling film thicknesses down to 10 nm and below, and a one order of magnitude lower relative permittivity and higher coercive field. Both the complex interplay of the fluorite crystal phases, as well as the intrinsic material and/or ferroelectric properties associated with them, have made ferroelectric HfO2-ZrO2-based ferroelectrics simultaneously challenging and interesting to characterize. Due in strong part to the nanoscale thicknesses of these fluorite-based ferroelectric films, the device behavior is an inseparable combination of the ferroelectric film properties (i.e., structure, crystalline orientation, grain size) and the material stack structure that encapsulates it into a two or three terminal device (i.e., interfaces, dielectric layers, electrode materials). Each article comprising this Research Topic on advanced characterization methods for HfO2/ZrO2-based ferroelectric illustrates different ways in which the intrinsic material properties or the ferroelectric film’s interaction with the device stack can be characterized to gain physical insight into this unconventional ferroelectric material system. Surface energy effects and grain size are often attributed to the predominant stabilization of either the non-polar tetragonal, monoclinic, or the polar orthorhombic phases in polycrystalline HfO2–ZrO2 films. It is generally observed that the polar orthorhombic phase is stabilized somewhere between the non-polar tetragonal and monoclinic phase boundaries, and that these non-polar phases are very sensitive to grain size in both HfO2 and ZrO2. Since the preferred crystal phase-dependence on grain size can be sensitive to stoichiometry (for instance, in Hf1xZrxO2 or Si-doped HfO2), it can be anticipated that there may be a complex interplay between grain-size engineering and ferroelectric film composition. In “Effect of Al2O3 interlayers on the microstructure and electrical response of ferroelectric doped HfO2 thin films” by Lederer et al., the grain-size and composition dependence of ferroelectric Hf1-xZrxO2 and Si-doped HfO2 is investigated in detail in which 1, 2, and 3 Al2O3 interlayers are used to control grain size while adjusting the stoichiometry of the fluorite-structured ferroelectric films. Using a combination of structural techniques, such as grazing-incidence X-ray diffraction and Kikuchi diffraction, as OPEN ACCESS
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社论:HfO2/ZrO2基铁电体的先进表征方法
与历史上占主导地位的钙钛矿基铁电体相比,基于HfO2和ZrO2的铁电体材料是非常规铁电体。这些与传统钙钛矿铁电体的差异在HfO2-ZrO2的萤石基结构中可以清楚地看到,该结构表现出竞争晶相的丰富多态性,当将膜厚度缩小到10nm及以下时增强了铁电行为,以及一个数量级的较低相对介电常数和较高矫顽场。萤石晶相的复杂相互作用,以及与之相关的本征材料和/或铁电性质,使铁电HfO2-ZrO2基铁电体的表征同时具有挑战性和趣味性。在很大程度上,由于这些基于萤石的铁电膜的纳米级厚度,器件行为是铁电膜性质(即结构、晶体取向、晶粒尺寸)和将其封装到两个或三个端子器件中的材料堆叠结构(即界面、介电层、电极材料)的不可分割的组合。包含HfO2/ZrO2基铁电体高级表征方法研究主题的每一篇文章都说明了可以表征本征材料特性或铁电膜与器件堆叠的相互作用的不同方式,以获得对这种非常规铁电材料系统的物理见解。表面能效应和晶粒尺寸通常归因于多晶HfO2–ZrO2膜中非极性四方相、单斜相或极性正交相的主要稳定性。通常观察到,极性正交相在非极性四方和单斜相边界之间的某个地方稳定,并且这些非极性相对HfO2和ZrO2中的晶粒尺寸非常敏感。由于对晶粒尺寸的优选晶相依赖性可能对化学计量敏感(例如,在Hf1xZrxO2或Si掺杂的HfO2中),因此可以预期晶粒尺寸工程和铁电膜组成之间可能存在复杂的相互作用。在Lederer等人的“Al2O3夹层对铁电掺杂HfO2薄膜微观结构和电学响应的影响”中,并且使用3个Al2O3夹层来控制晶粒尺寸,同时调节萤石结构铁电膜的化学计量。使用结构技术的组合,如掠入射X射线衍射和菊池衍射,如OPEN ACCESS
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来源期刊
Frontiers in Nanotechnology
Frontiers in Nanotechnology Engineering-Electrical and Electronic Engineering
CiteScore
7.10
自引率
0.00%
发文量
96
审稿时长
13 weeks
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