接口极性对GaN/AlN接口的基底位移的影响
Yuming Yang1,2, Xuemei Zhang3, Mi Qin1,2
1Key Laboratory of Materials Physics, Institute of Solid State Physics, HFIPS, Chinese Academy of Sciences, Hefei 230031, China.
Physical chemistry chemical physics : PCCP
|December 6, 2024
概括
高密度位移在化 (GaN) 冲击装置的性能. 这项研究侧重于基底位移,发现N极化 (AlN) 基板在1900K产生高质量的GaN,缺陷较少.
科学领域:
- 材料科学 材料科学 材料科学
- 固态物理 固态物理
- 半导体物理 半导体物理
背景情况:
- 高密度的化 (GaN) 失调严重阻碍了基于GaN的电子设备的功能.
- 现有的研究主要研究大量GaN内部的线程位移,忽视实验观察到的基底位移.
研究的目的:
- 为了研究在AlN上生长的GaN中基础位的形成机制和特征.
- 探索基质极性和生长温度对脱位密度和GaN晶体质量的影响.
主要方法:
- 密度函数理论 (DFT) 的计算被用来分析原子相互作用和结合.
- 经验分子动力学 (MD) 模拟被用于模拟在AlN上GaN生长期间的脱位行为.
主要成果:
- 阿尔极性GaN/AlN接口有利于形成Shockley部分位移,这是线程边缘位移的前体.
- GaN生长温度显著影响脱位密度和局部原子排列.
- 在1900K的N极性AlN基质促进了GaN的生长,增强了石结构和减少了位含量.
结论:
- 基底位移,特别是肖克利局部位移,在AlN上GaN增长的早期阶段起着至关重要的作用.
- 优化基质极性 (N-极性AlN) 和生长温度 (1900K) 对于最大限度地减少位移和实现高质量的GaN薄膜至关重要.
更多相关视频
06:57Theoretical Calculation and Experimental Verification for Dislocation Reduction in Germanium Epitaxial Layers with Semicylindrical Voids on Silicon
Published on: July 17, 2020
2.2K
07:50Electron Channeling Contrast Imaging for Rapid III-V Heteroepitaxial Characterization
Published on: July 17, 2015
11.0K
相关概念视频
Biasing of P-N Junction
422
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
422
P-N junction
466
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...
466
Biasing of Metal-Semiconductor Junctions
215
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...
215
Metal-Semiconductor Junctions
296
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...
296
Magnetostatic Boundary Conditions
874
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
874
Types of Semiconductors
530
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...
530
