丧的范德瓦尔斯异构结构
1Applied Artificial Intelligence Institute, Deakin University, Geelong, Victoria 3216, Australia. abbas@deakin.edu.au.
Nanoscale
|October 18, 2024
概括
在范德瓦尔斯的二维材料中探索了几何挫折. 研究人员使用计算方法确定了一个潜在的稳定,挫败的范德瓦尔斯异构结构.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 计算材料科学科学 计算材料科学
背景情况:
- 在密集的格子中产生冲突力的几何挫折是玻璃材料中已知的现象.
- 这项研究将几何挫折的概念扩展到范德瓦尔斯 (vdW) 二维 (2D) 材料.
研究的目的:
- 为了研究几何挫败的VDW异构结构.
- 为了确定具有这种现象的可能合成的二维材料.
主要方法:
- 使用密度函数理论 (DFT) 具有r2SCAN + rVV10交换相关性潜力.
- 采用了三个结构稳定性标准:声子分散,热力学稳定性比较 (挫折与非挫折的vdW异构结构),以及ab initio分子动力学模拟.
主要成果:
- 识别了几种具有交替应变 (应变和压缩层) 的2D异构.
- 在调查的7种挫败的VDW异构结构中,根据所应用的标准,发现一种材料具有潜在的稳定性.
结论:
- 该研究成功地应用了计算方法来探索挫败的vdW异构结构.
- 确定了对挫败的vdW异构结构的一个有希望的候选材料,并讨论了潜在的制造途径.
更多相关视频
相关概念视频
Van der Waals Interactions
63.6K
Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
63.6K
Van der Waals Equation
4.0K
The ideal gas law is an approximation that works well at high temperatures and low pressures. The van der Waals equation of state (named after the Dutch physicist Johannes van der Waals, 1837−1923) improves it by considering two factors.
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
First, the attractive forces between molecules, which are stronger at higher densities and reduce the pressure, are considered by adding to the pressure a term equal to the square of the molar density multiplied by a positive coefficient a. Second, the volume...
4.0K
Metal-Semiconductor Junctions
306
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
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...
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...
306
Valence Bond Theory
31.9K
Overview of Valence Bond Theory
31.9K
Hybridization of Atomic Orbitals I
46.6K
The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
46.6K
Biasing of Metal-Semiconductor Junctions
216
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
216


