在石异构结构中的近距离铁电
Chloe H Skidmore1, R Jackson Spurling1, John Hayden1
1Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA, USA.
在石异构中观察到近距离铁电,使非铁电材料的极化反转. 这种接口现象在没有化学干扰的情况下发生,为铁电应用开辟了新的途径.
科学领域:
- 材料科学
- 凝聚物质物理学
- 固态化学
背景情况:
- 近距离铁电是一种接口现象,相邻的铁电材料会诱导非铁电材料的极化反转.
- 由于其独特的晶体结构,石材料为探索接口驱动的现象提供了一个独特的平台.
研究的目的:
- 在石铁电异构结构中展示和研究近距离铁电.
- 阐明这些材料接口的极化逆转的潜在物理机制.
主要方法:
- 化物-化物,氧化物-氧化物和化物-氧化物异构的制造.
- 多模特特征包括偏振歇斯底里,压缩反应力显微镜和扫描传输电子显微镜.
- 密度函数理论计算以建模切换障碍和域壁能.
主要成果:
- 在非铁电AlN和ZnO层中通过相邻的铁电AlBN,AlScN和ZnMgO层成功诱导了近距离铁电.
- 提出了一个物理切换模型,涉及反极核的传播和界面场效应,减少切换障碍.
- 实验验证证了两层在各种异构结构中的铁电切换.
结论:
- 在不依赖元素替代的情况下,可以在石异构中实现近距离铁电.
- 这项工作扩大了基于接口的铁电及其对新型电子设备的潜力.
更多相关视频
08:00Chemical Synthesis of Porous Barium Titanate Thin Film and Thermal Stabilization of Ferroelectric Phase by Porosity-Induced Strain
Published on: March 27, 2018
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
相关概念视频
Ferromagnetism
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Trends in Lattice Energy: Ion Size and Charge
Fermi Level Dynamics
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Crystal Field Theory - Tetrahedral and Square Planar Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
