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A Gibbs energy view of double hysteresis in ZrO_2 and Si-doped HfO_2

机译:ZrO_2和Si-掺杂HFO_2中双滞后的GIBBS能量观

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摘要

The Gibbs energy can yield fundamental insight into the material properties of ferroelectrics such as energy barriers and phase transitions. Particularly for newly emerging classes of ferroelectric and antiferroelectric materials, such as fluorite-structured HfO_2 and Zr0O_2, the Gibbs energy can bridge theoretical calculations with experimental observations. Experimentally observed dynamic double hysteresis loops in thin film ZrO_2 and Si-doped HfO_2 capacitors are used to obtain a solution to the Gibbs energy by calculating the internal electric field with depolarization. By accounting for dipole-field interaction energies and static energies in the solution of the Gibbs energy of double-hysteresis ZrO_2 and Si-doped HfO_2, a characteristic triple-well with two polar and one nonpolar energy minima emerges. Macroscopic metastable polar and nonpolar phases close in free energy are shown to be in agreement with first-order phase transitions underlying double hysteresis in ZrO_2 and Si-doped HfO_2. The application of an external field is demonstrated to lower the free energy minimum of the polar phase below the nonpolar phase, providing macroscopic support that a first-order phase transition driven by an electric field is responsible for antiferroelectric behavior in doped HfO_2 and ZrO_2. Energy barriers for the nonpolar → polar phase transition from 0.75 to 4.3 meV per formula unit are calculated for ZrO_2 and Si-doped HfO_2. The macroscopic Gibbs energy profiles obtained through experimental measurements and device modeling connect the fundamental phenomenology of ferroelectrics and antiferroelectrics to electronic devices.
机译:GIBBS能量可以屈服于诸如能量屏障和相变的铁电性的材料特性的基础洞察。特别是对于新出现的铁电和防火电材料,例如萤石结构的HFO_2和Zr0O_2,Gibbs能量可以通过实验观察来介绍理论计算。通过计算具有去极化的内部电场,通过计算内部电场来获得薄膜ZrO_2和Si掺杂的HFO_2电容器中的实验观察到的动态双磁滞回路。通过对偶极场相互作用能量和静态能量的偶极核对双滞回ZRO_2和SI掺杂HFO_2的静态能量进行计入,具有两个极性和一个非极性能量最小值的特征三倍。宏观亚稳态和非极性阶段在自由能中闭合在Zro_2和Si掺杂HFO_2中的双滞后的一阶相转变一致。证明外部场的施加以降低非极性相下方的极性阶段的自由能量,提供宏观支撑,即由电场驱动的一阶相转变负责掺杂HFO_2和ZrO_2中的排式释放行为。对于ZrO_2和Si-掺杂的HFO_2,计算非极性→非极化→极性相位转变为0.75至4.3mEV。通过实验测量和器件建模获得的宏观GIBBS能量分布将铁电气和防火电极的基本上现象学与电子设备连接到电子设备。

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  • 来源
    《Applied Physics Letters》 |2020年第14期|142904.1-142904.5|共5页
  • 作者单位

    Nanoelectronic Materials Laboratory (NaMLab) gGmbH 01187 Dresden Germany;

    Nanoelectronic Materials Laboratory (NaMLab) gGmbH 01187 Dresden Germany;

    Nanoelectronic Materials Laboratory (NaMLab) gGmbH 01187 Dresden Germany;

    Nanoelectronic Materials Laboratory (NaMLab) gGmbH 01187 Dresden Germany;

    Nanoelectronic Materials Laboratory (NaMLab) gGmbH 01187 Dresden Germany Chair of Nanoelectronic Materials TU Dresden 01187 Dresden Germany;

    Nanoelectronic Materials Laboratory (NaMLab) gGmbH 01187 Dresden Germany;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-18 22:18:03

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