在单个纳米板Cu1.81S-CdS异构结构中,可见光诱导的孔转移
Chang Wang1, Zhaozhe Chen1, Si Xiao1
1Hunan Key Laboratory of Nanophotonics and Devices, School of Physics, Central South University, Changsha 410083, China. sixiao@csu.edu.cn.
Nanoscale
|February 20, 2024
概括
研究人员合成了硫化铜-硫化 (Cu1.81S-CdS) 异质连接. 过渡吸收光谱显示光生成孔从CdS转移到Cu1.81S,增强光催化.
科学领域:
- 材料科学 材料科学 材料科学
- 光催化作用的光催化
- 频谱学是一种光谱学.
背景情况:
- 半导体中有效的电荷分离和转移对于光电子设备和光催化剂至关重要.
- 短暂吸收光谱是研究光生成载体动态的一个关键技术.
研究的目的:
- 合成Cu1.81S-CdS异质连接并研究它们的载体动态.
- 为了探索这些异质连接中光生成载体转移的方向.
- 了解可见光诱导的孔运输的机制.
主要方法:
- 通过热注射合成Cu1.81S纳米板.
- 使用阴子交换制备Cu1.81S-CdS异质连接和CdS纳米板.
- 使用短暂吸收光谱学进行载体动态调查.
- 使用密度函数理论 (DFT) 计算的理论解释.
主要成果:
- 高质量的Cu1.81S纳米板已经成功合成.
- 在Cu1.81S-CdS异质连接中,通过离子交换进行了制备.
- 过渡吸收光谱显示光生成孔在400nm激发下从CdS转移到Cu1.81S.
- 这种孔转移方向与近红外局部表面等离子体共振诱导的转移在硫化铜异构结构中观察到的方向相反.
- DFT计算支持可见光诱导的孔输送机制.
结论:
- 这项研究表明,在Cu1.81S-CdS异质连接处,有一种新的光生成孔转移途径.
- 这种相反方向的孔转移机制有可能提高气生产率.
- 催化剂的增强光稳定性是这种异构结构设计的另一个潜在好处.
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
7.6K
12:21Close-Space Sublimation-Deposited Ultra-Thin CdSeTe/CdTe Solar Cells for Enhanced Short-Circuit Current Density and Photoluminescence
Published on: March 6, 2020
8.2K
相关概念视频
Metal-Semiconductor Junctions
350
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...
350
P-N junction
531
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...
531
