在高Si-Doped GaN中的纳米恒星
Marta Sawicka1, Henryk Turski1, Kamil Sobczak2
1Institute of High Pressure Physics, Polish Academy of Sciences, Sokołowska 29/37, 01-142 Warsaw, Poland.
Crystal growth & design
|July 10, 2023
概括
高度合化与 (GaN:Si) 形成纳米星在等离子体辅助分子束表达 (PAMBE). 这些纳米结构表现出不同的电性质和较低的含量,影响导电性.
科学领域:
- 材料科学 材料科学 材料科学
- 固态物理 固态物理
- 一个半导体的Epitaxy.
背景情况:
- 了解化与 (GaN:Si) 的表面形态和电特性之间的联系对于基础科学和应用至关重要.
- 等离子体辅助分子束表达 (PAMBE) 是种植高质量的半导体层的一个关键技术.
研究的目的:
- 为了研究PAMBE培养的高化GaN:Si层中纳米恒星的形成.
- 为了将纳米恒星表面形态与纳米尺度电性质的变化相关联.
- 阐明在蚀刻行为和导电性中观察到的差异背后的原因.
主要方法:
- 酸与 (GaN:Si) 增长的等离子辅助分子束表皮氧化 (PAMBE).
- 原子力显微镜 (AFM) 和扫描扩散电阻显微镜 (SSRM) 用于表面形态和导电性映射.
- 电化学蚀刻 (ECE) 和传输电子显微镜 (TEM) 与能量分散式X射线光谱 (EDX) 进行结构和组成分析.
主要成果:
- 纳米星的形成 (50纳米宽的血小板在六倍对称) 在高度杂的GaN:Si中 (5 × 10^19到1 × 10^20cm^-3).
- 纳米恒星在a-direction 112̅0沿线呈现增强的生长,导致不同的表面形态.
- 在纳米尺度上的电特性不均,纳米恒星具有较低的导电性和大约10%的内含量.
- 纳米星抗电化学蚀刻 (ECE),这表明补偿机制有助于降低导电性.
结论:
- 高度合的GaN:Si中的纳米恒星形成是由异性增长驱动的.
- 表面形态直接影响纳米电气性能变化.
- 较低Si含量和补偿机制的组合有助于GaN:Si中纳米恒星的独特电气特性.
相关概念视频
Biasing of Metal-Semiconductor Junctions
284
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...
284
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
MOSFET: Enhancement Mode
389
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
389
Biasing of P-N Junction
613
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...
613


