在异质连接中建立多个顺序的内置电场,以实现光载体空间分离
Sikang Xue1,2, Hao Tang1, Min Shen1
1State Key Laboratory of Photocatalysis on Energy and Environment, College of Chemistry, Fuzhou University, Fuzhou, 350116, P. R. China.
Advanced materials (Deerfield Beach, Fla.)
|January 8, 2024
概括
研究人员创建了具有内置电场 (BIEF) 的新氧化/硫化异质连接,以实现高效的二氧化碳 (CO2) 光还原. 这种设计增强了电荷分离,提高了二氧化碳转化为一氧化碳的性能.
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
- 表面化学 表面化学
背景情况:
- 在异质连接接口上构建内置电场 (BIEF) 对光催化中的电荷分离至关重要.
- 低维材料中的单向BIEF限制了光生成载体分离.
- 有效的二氧化碳 (CO2) 光降解需要优化电荷载体动力学.
研究的目的:
- 为了制造Z-方案ZnO/ZnS异质连接,具有多个顺序的BIEF,用于增强CO2光降解.
- 为了研究ZnO/ZnS异质连接的界面结构和BIEF方向.
- 阐明BIEF在促进光生成载体分离和二氧化碳转化中的作用.
主要方法:
- 通过硫化 ZnO 纳米盘制造 ZnO/ZnS 异质连接.
- 使用阴极光发光2D映射进行表征.
- 使用密度函数理论 (DFT) 的计算分析.
主要成果:
- 观察到具有两个半连贯相位边界的明显界面结构.
- 证实了从ZnS到ZnO跨越的多级BIEF.
- 获得了3811.7μmol h−1 g−1的增强的CO2到一氧化碳光降解性能.
结论:
- 新型ZnO/ZnS异质连接有效地利用多次 BIEF 实现更优质的电荷分离.
- 从ZnS到ZnO的定向BIEF促进了电子和孔的空间分离.
- 这项研究为设计用于光催化应用的异质连接中的BIEF提供了一种新策略.
相关概念视频
Carrier Generation and Recombination
577
Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
577
P-N junction
536
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...
536
Induced Electric Fields: Applications
1.6K
An important distinction exists between the electric field induced by a changing magnetic field and the electrostatic field produced by a fixed charge distribution. Specifically, the induced electric field is nonconservative because it does not work in moving a charge over a closed path. In contrast, the electrostatic field is conservative and does no net work over a closed path. Hence, electric potential can be associated with the electrostatic field but not the induced field. The following...
1.6K
Electric Field of Two Equal and Opposite Charges
5.9K
Atoms generally contain the same number of positively and negatively charged particles, protons, and electrons. Hence, they are electrically neutral. However, the centers of the positive and negative charges do not always coincide. In such a scenario, the electric field of an atom may not be zero.
A separation of the positive and negative charges can lead to a weak, remnant effect of the positive and negative charges. The expectation is that the more the distance between the positive and...
A separation of the positive and negative charges can lead to a weak, remnant effect of the positive and negative charges. The expectation is that the more the distance between the positive and...
5.9K
Induced Electric Dipoles
4.2K
A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
4.2K
Carrier Transport
446
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:
446


