在二维半导体中激子传输的近期进展
Hyeongwoo Lee1, Yong Bin Kim1, Jae Won Ryu1
1Department of Physics, Pohang University of Science and Technology (POSTECH), Pohang, 37673, Republic of Korea.
Nano convergence
|December 15, 2023
概括
控制二维半导体中的刺激电流是光电子学的关键. 本综述详细介绍了诸如电场和应变等方法,以克服激电传输和设备实施方面的挑战.
科学领域:
- 材料科学 材料科学 材料科学
- 凝聚物质物理学 凝聚物质物理学
- 纳米技术 纳米技术
背景情况:
- 在2D半导体中对激发性准粒子 (激发子) 的空间操纵对于先进的光电子学至关重要.
- 目前的局限性包括中性刺激子的电控制不佳,充电刺激子寿命短,以及低室温刺激子道效率.
- 这些挑战阻碍了高效的刺激传输和实际设备应用.
研究的目的:
- 审查最近在控制2D材料中的激电流方面的进展.
- 探索技术,以克服现有的挑战在刺激传输和光电子设备的实施.
- 突出各种激发性准粒子对未来技术的潜力.
主要方法:
- 专注于诱导刺激电流的四个主要控制参数:电场,应变梯度,表面等离子极子和光子腔.
- 审查每个控制方法的基本原则和最近的实验研究.
- 分析这些控制技术在可访问性,效率和功能方面的进展.
主要成果:
- 通过使用各种物理刺激来操纵刺激电流的进展.
- 突出了先进的控制技术越来越有效和更广泛的适用性.
- 提供了对激励子操纵最先进方法的综合概述.
结论:
- 通过电场,应变,等离子电流和光子空洞控制激子电流取得了重大进展.
- 克服激子传输方面的挑战对于实现实用的基于激子的光电子设备至关重要.
- 需要进一步的研究才能充分利用激发性准粒子的潜力.
相关概念视频
Carrier Transport
449
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:
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Semiconductors
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There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
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Types of Semiconductors
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The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
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The work...
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Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
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Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
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Carrier Generation and Recombination
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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.
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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...
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