基于二甲的二维铁电单层分子晶体,具有很大的平面自发极化
Liang Ma1,2, Yinglu Jia1, Stephen Ducharme3
1Department of Chemistry, Nebraska Center for Materials and Nanoscience , University of Nebraska-Lincoln , Lincoln , Nebraska 68588 , United States.
Journal of the American Chemical Society
|January 12, 2019
概括
研究人员为先进的应用开发了二维 (2D) 铁电分子晶体. 这些灵活的轻质材料具有很大的自发极化 (Ps) 并在室温下保持铁电.
科学领域:
- 材料科学
- 凝聚物质物理学
- 晶体学
背景情况:
- 由于其易于加工,轻量化和机械灵活性,铁电分子晶体是理想的应用.
- 大自发极化 (Ps) 是先进铁电应用的一个关键特性.
- 现有的铁电材料在加工和机械整合方面经常面临挑战.
研究的目的:
- 理论上研究二维 (2D) 铁电分子晶体的潜力.
- 探索在二维分子晶体中实现大平面自发偏振的可行性.
- 了解键和基质支对铁电性能的作用.
主要方法:
- 为了研究二维铁电分子晶体的电子和结构性质,使用了初始计算.
- 最初的分子动力学模拟用于评估铁电秩序的热稳定性.
- 这项研究重点是基于二甲 (DIPAB) 的单层和相关的化物晶体.
主要成果:
- 基于二甲基 (DIPAB) 的二维铁电单层分子晶体在理论上以大约1.5 × 10-6μC cm-1的平面自发极化 (Ps) 实现.
- 这项研究确定了键在稳定铁电性质方面的关键作用.
- 在2DDIPAB单层中的铁电顺序在被石墨烯基底支持时在室温下稳定.
结论:
- 具有显著的平面Ps的二维全有机铁电单层单分子晶体的理论设计是可行的.
- 化分子晶体为开发下一代柔性铁电材料提供了一个有前途的平台.
- 这些发现为使用二维铁电材料的新型电子和光电子设备铺平了道路.
相关概念视频
Molecular Shape and Polarity
75.6K
Dipole Moment of a Molecule
75.6K
Spontaneity
29.8K
A spontaneous process is one that occurs naturally under certain conditions. A nonspontaneous process, on the other hand, will not take place unless it is “driven” by the continual input of energy from an external source. Processes have a natural tendency to occur in one direction under a given set of conditions. Water will naturally flow downhill (spontaneous process), but uphill flow (nonspontaneous process) requires outside intervention such as the use of a pump. Iron exposed to...
29.8K
Bond Polarity, Dipole Moment, and Percent Ionic Character
35.5K
Bond Polarity
35.5K
Group Polarization
39.2K
Group polarization is the strengthening of an original group attitude following the discussion of views within a group (Teger & Pruitt, 1967). That is, if a group initially favors a viewpoint, after discussion the group consensus is likely a stronger endorsement of the viewpoint. Conversely, if the group was initially opposed to a viewpoint, group discussion would likely lead to stronger opposition.
39.2K
Crystal Field Theory - Tetrahedral and Square Planar Complexes
48.4K
Tetrahedral 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,...
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,...
48.4K
Ionic Crystal Structures
17.0K
Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
17.0K


