在二维HgI2层中,强滑动铁电和间层滑动可控制的螺旋电子效应
Xinfeng Chen1, Xinkai Ding1,2, Gaoyang Gou1
1Frontier Institute of Science and Technology, State Key Laboratory of Electrical Insulation and Power Equipment, Xi'an Jiaotong University, Xi'an 710049, People's Republic of China.
Nano letters
|March 1, 2024
概括
研究人员发现了新的2D滑动铁电材料,HgBr2和HgI2,表现出室温铁电. 这些材料通过通过层间滑动控制电子自旋,使新型自旋电子装置成为可能.
科学领域:
- 材料科学 材料科学 材料科学
- 凝聚物质物理学 凝聚物质物理学
- 纳米技术纳米技术
背景情况:
- 开发用于先进电子应用的二维 (2D) 材料是一个关键的研究领域.
- 滑动铁电 (FE) 材料为下一代设备提供了独特的功能,但实验发现仍然具有挑战性.
- 2D"slidetronics"领域需要具有可检测铁电性的新材料和新的功能.
研究的目的:
- 识别和描述新的二维 (2D) 滑动铁电材料.
- 探索这些材料在二维自旋电子设备中的潜力.
- 为了研究层间合,铁电和旋转纹理之间的关系.
主要方法:
- 使用第一原理计算来研究范德瓦尔斯 (vdW) 层状晶体HgX2 (X = Br,I).
- 分析堆叠序列和层间合以确定铁电性质.
- 模拟电场对铁电和自旋纹理的影响.
主要成果:
- HgBr2和HgI2被确定为可合成的2D滑动铁电,在室温下具有稳定的平面外铁电.
- 2D HgI2表现出强大的滑动铁电 (高达0.16μC/cm2) 由于强大的层间合和界面电荷重排.
- 在FE-HgI2中介层滑动控制Rashba旋转纹理,使潜在的旋转电子应用成为可能.
结论:
- HgX2 (X = Br,I) 代表了一个新的二维滑动铁电材料类.
- 发现的材料显示了2D滑动电子和旋动电子的实际应用潜力.
- 在2D模式下,使用FE-HgI2层进行电子自旋检测的电控是可行的.
相关概念视频
Ferromagnetism
2.4K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.4K
Colors and Magnetism
11.7K
Color in Coordination Complexes
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
When atoms or molecules absorb light at the proper frequency, their electrons are excited to higher-energy orbitals. For many main group atoms and molecules, the absorbed photons are in the ultraviolet range of the electromagnetic spectrum, which cannot be detected by the human eye. For coordination compounds, the energy difference between the d orbitals often allows photons in the visible range to be absorbed and emitted, which is seen as colors by the human...
11.7K
Metallic Solids
18.4K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
18.4K
Types Of Superconductors
979
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
979
Trends in Lattice Energy: Ion Size and Charge
23.9K
An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid sodium chloride, the lattice energy is the enthalpy change of the process:
23.9K
The Hall Effect
2.4K
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
2.4K


