来自具有不同宽度和极性量子孔的InGaN/GaN二极管的光发光和光电流
Artem Bercha1, Mikołaj Chlipała1, Mateusz Hajdel1
1Institute of High Pressure Physics, Polish Academy of Sciences, Sokołowska 29/37, 01-142 Warsaw, Poland.
Nanomaterials (Basel, Switzerland)
|January 24, 2025
概括
我们研究了具有不同层结构和宽度的InGaN量子井二极管. 反向极性,宽孔二极管表现出优越的光电效率和光发光强度,显示出稳定的发射波长.
科学领域:
- 半导体物理 半导体物理
- 光电学是指光电子产品.
- 材料科学 材料科学 材料科学
背景情况:
- 了解InGaN量子井 (QW) 属性对于光电子设备至关重要.
- 内置的电场和载体选对设备性能有很大的影响.
研究的目的:
- 为了将InGaN二极管的光学性能与标准 (nip) 和倒置 (pin) 层序列进行比较.
- 为了研究量子井宽度 (2.6 nm 和 15 nm) 对设备性能的影响.
- 分析内置的场方向和载体选对光发光和光电流的影响.
主要方法:
- 制造和表征四针二极管样本,具有不同的InGaN QW宽度和极性.
- 光发光 (PL) 和光电流 (PC) 测量作为激发功率和应用电压的函数.
主要成果:
- 由于内置场和载波选之间的相互作用,观察到光学特性中的显著差异.
- 宽井反向极性二极管在反向偏差下展示了最高的光电效率.
- 这种逆极性二极管在正偏差下也显示了最高的PL强度.
- 宽孔二极管表现出稳定的发射波长,基本上独立于偏差和激发功率.
结论:
- 设备极性和量子井宽度是优化InGaN二极管性能的关键因素.
- 具有更宽的量子井的逆极性设计显示出对高效光电子应用的前景.
- 宽孔二极管的稳定排放特性有利于设备的一致运行.
相关概念视频
Photoluminescence: Fluorescence and Phosphorescence
1.5K
Photoluminescence is a process where a molecule absorbs light energy and re-emits it in the form of light. This phenomenon occurs when a substance absorbs photons, promoting its electrons to higher energy level excited states, followed by a relaxation process in which the electrons return to their original ground state energy levels and emit light. Photoluminescence is widely observed in various materials, including semiconductors, and organic and inorganic compounds.
A pair of electrons in a...
A pair of electrons in a...
1.5K
Biasing of P-N Junction
406
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...
406
P-N junction
459
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...
459
Photoluminescence: Applications
369
Photoluminescence offers a wide range of applications due to its inherent sensitivity and selectivity. This technique allows for both direct and indirect analyses of the analyte. Direct quantitative analysis is possible when the analyte exhibits a favorable quantum yield for fluorescence or phosphorescence. However, an indirect analysis may be feasible if the analyte is not fluorescent or phosphorescent, or if the quantum yield is unfavorable. Indirect methods include reacting the analyte with...
369


