极其异构的范德瓦尔斯热导体
Shi En Kim1, Fauzia Mujid2, Akash Rai3
1Pritzker School of Molecular Engineering, University of Chicago, Chicago, IL, USA.
Nature
|September 30, 2021
概括
设计的范德瓦尔斯薄膜实现了创纪录的热异构性,使集成电路能够有效散热. 在MoS2薄膜中随机的间层旋转产生高度异性导热性,用于先进的热管理.
科学领域:
- 材料科学
- 凝聚物质物理学
- 纳米技术
背景情况:
- 集成电路 (IC) 的小型化需要先进的热管理.
- 具有高导热性和异构性质的材料对于控制热流至关重要.
- 与天然材料相比,现有的工程热导体具有有限的异构性.
研究的目的:
- 开发具有极高异构率的新型人造热导体.
- 研究范德瓦尔斯 (vdW) 薄膜中层间旋转的作用.
- 展示这些材料在电子设备中的热管理潜力.
主要方法:
- 制造大面积的vdW薄膜 (MoS2,WS2) 随机间层旋转.
- 使用专用技术测量内平面和透平面的导热率.
- 分子动力学 (MD) 模拟以阐明热传输机制.
主要成果:
- 在MoS2薄膜中实现了接近900的室温热异构比率.
- 通过平面测量的超低导热率 (MoS2: 57±3 mW m−1 K−1,WS2: 41±3 mW m−1 K−1).
- 证明了与单晶相比较的高平面导热率.
- MD模拟显示1D玻璃般的热传输在通过平面的方向.
结论:
- 具有随机层间旋转的工程VdW片提供了前所未有的热异性.
- 层间的旋转有效地阻碍了通过平面的热传输,同时保持了平面内的导电性.
- 这些异构材料有望防止纳米制造的电极和设备过热.
- 层间旋转为固态系统中的定向热传输提供了一个新的设计范式.
相关概念视频
Theory of Metallic Conduction
1.5K
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
1.5K
Types Of Superconductors
1.2K
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...
1.2K
Superconductor
1.3K
A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
1.3K
Van der Waals Equation
4.8K
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...
4.8K
Semiconductors
1.0K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.0K
Types of Semiconductors
1.0K
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
1.0K


