从DFT计算中,单层石墨烯中电子和孔兴奋剂的理论极限
Dawid Ciszewski1, Wojciech Grochala1
1Centre of New Technologies, University of Warsaw, Banacha 2C St., 02-097 Warsaw, Poland. d.ciszewski@cent.uw.edu.pl.
概括
单层石墨烯在兴奋剂中表现出显著的不对称性,支持比孔兴奋剂更高的电子兴奋剂. 电子兴奋剂显示出超导的潜力,临界温度在特定的兴奋剂水平达到峰值.
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
- 计算化学计算化学
背景情况:
- 单层石墨烯是一种具有独特电子特性的新材料.
- 了解兴奋剂效应对于定制石墨烯的功能至关重要.
- 电荷载体兴奋剂中的不对称性可以显著影响材料的行为.
研究的目的:
- 为了研究单层石墨烯的兴奋剂不对称性.
- 为了确定孔和电子兴奋剂的稳定性极限.
- 为了探索电子合石墨烯的超导性潜力.
主要方法:
- 使用密度函数理论 (DFT) 的计算.
- 进行了Phonon稳定性分析.
- 麦克米伦的公式被用来估计超导的临界温度.
主要成果:
- 观察到明显的不对称性,石墨烯维持更高的电子兴奋剂 (1.9电子/原子) 比洞兴奋剂 (0.1洞/原子).
- 在这些兴奋剂范围中保持了动态稳定.
- 预测了超导临界温度的两个局部最大值,用于电子合的石墨烯,与电子-声波合相关.
结论:
- 单层石墨烯显示出对电子兴奋剂的明显偏好,而不是孔兴奋剂.
- 电子合石墨烯具有高温超导的潜力.
- 电子 - 声子合强度是确定超导特性的一个关键因素.
更多相关视频
13:56Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
Published on: October 12, 2019
7.7K
11:33All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
Published on: January 19, 2018
9.9K
相关概念视频
Fermi Level
828
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,...
828
Types of Semiconductors
934
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...
934
Fermi Level Dynamics
349
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
349
Carrier Transport
571
The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
571
Metal-Semiconductor Junctions
519
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...
519
Band Theory
15.6K
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
15.6K
