在WSe2单层中,p型导电性的起源
Yu-Zhou Zhang1,2, Guo-Jun Zhu1,2, Ji-Hui Yang1,2
1Department of Physics, Key Laboratory for Computational Science (MOE), State Key Laboratory of Surface Physics, Fudan University, Shanghai 200432, China. jhyang04@fudan.edu.cn.
Nanoscale
|July 10, 2023
概括
化 (WSe2) 单层中的缺陷会影响电子性能. 氧杂质形成复合物与空位 (nOSe + VW) 被确定为WSe2.2中p型导电的来源.
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
- 固态化学 固态化学
背景情况:
- 过渡金属二化物 (TMD) 对于先进的电子和光电子技术至关重要.
- 了解WSe2单层中的缺陷是优化其性能的关键.
- 在WSe2单层中报告的p型导电性缺乏最终的解释.
研究的目的:
- 系统地调查WSe2单层中的点缺陷.
- 为了确定p型导电性在WSe2.2中的来源.
- 探索先天缺陷和补充剂的作用.
主要方法:
- 使用了第一原则计算.
- 系统地调查WSe2单层中的点缺陷.
- 对内在点缺陷,间隙和氧取代的分析.
主要成果:
- 没有内在点缺陷可以解释p型兴奋剂.
- 间位子 (Hi) 可以导致n型导电性.
- 氧取代 (OSe) 促进空缺 (VW),形成浅层受体复合体 (nOSe + VW).
结论:
- 缺陷复合体nOSe + VW被确定为p型导电的起源,在无意中添加WSe2单层中.
- 在合成过程中氧气的存在对于这种p型行为至关重要.
- 这一发现澄清了WSe2研究中长期存在的团.
相关概念视频
Types of Semiconductors
666
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...
666
P-N junction
585
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
585
Metal-Semiconductor Junctions
395
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...
395
Fermi Level
668
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
668


