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相关概念视频

Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

330
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...
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Induced Electric Fields: Applications01:27

Induced Electric Fields: Applications

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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...
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Carrier Generation and Recombination01:22

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.
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...
560
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

238
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...
238
Carrier Transport01:21

Carrier Transport

421
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:
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Induced Electric Fields01:23

Induced Electric Fields

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The fact that emfs are induced in circuits implies that work is being done on the conduction electrons in the wires. What can possibly be the source of this work? We know that it’s neither a battery nor a magnetic field, as a battery does not have to be present in a circuit where current is induced, and magnetic fields never do any work on moving charges. The source of the work is in fact an electric field that is induced in the wires. For example, if a stationary conductor is placed in a...
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Comprehensive Characterization of Extended Defects in Semiconductor Materials by a Scanning Electron Microscope
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半导体器件中电场的特征:第二波光干扰的影响.

Yuke Cao, James W Pomeroy, Martin Kuball

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    概括
    此摘要是机器生成的。

    半导体设备中的电场诱导第二和生成 (EFISHG) 测量通过将激光从基板侧聚焦来改进. 这种方法消除了背景干扰,以便在GaN PN二极管中进行准确的电场分析.

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    科学领域:

    • 半导体设备的特征表征 半导体设备的特征表征
    • 非线性光学是一种非线性光学.
    • 光子学 是一个光子学.

    背景情况:

    • 电场诱导的第二和生成 (EFISHG) 提供了先进的半导体设备设计机会.
    • 目前的EFISHG技术面临挑战,原因是背景第二和生成 (SHG) 和EFISHG信号之间的干扰.
    • 精确的电场表征对于优化半导体性能至关重要.

    研究的目的:

    • 展示一种消除EFISHG测量干扰的方法.
    • 为了在GaN PN二极管中实现简单的定量电场分析.
    • 为了调查背景SHG和EFISHG之间的不一致性.

    主要方法:

    • 从化 (GaN) PN二极管的透明基板侧聚焦激光.
    • 开发基于波浪生成和传播的模型.
    • 将基板侧测量与PN接口接口侧测量进行比较.

    主要成果:

    • 通过使用基板侧照明方法,有效消除了EFISHG测量中的干扰效应.
    • 定量电场分析是直接实现的,与接口侧测量不同.
    • 一个拟议的模型突出了背景SHG和EFISHG光线之间的不一致性.

    结论:

    • 从基板侧照明是使用GaN PN二极管进行EFISHG测量的优质方法.
    • 观察到的不一致性很可能是由于激光聚焦深度和相位不匹配.
    • 这种技术可方便精确的电场映射,从而改善半导体设备的设计.