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相关概念视频

Gauss's Law in Dielectrics01:17

Gauss's Law in Dielectrics

Consider a polar dielectric placed in an external field. In such a dielectric, opposite charges on adjacent dipoles neutralize each other, such that the net charge within the dielectric is zero. When a polar dielectric is inserted in between the capacitor plates, an electric field is generated due to the presence of net charges near the edge of the dielectric and the metal plates interface. Since the external electrical field merely aligns the dipoles, the dielectric as a whole is neutral. An...
Galvanometer01:24

Galvanometer

Common devices, including car instrument panels, battery chargers, and inexpensive electrical instruments, measure potential difference (voltage), current, or resistance using a d'Arsonval galvanometer. This electromechanical instrument is also known as a moving coil galvanometer.
The galvanometer consists of  two concave-shaped permanent magnets, providing a uniform radial magnetic field in the annular region. In the center, a pivoted coil of fine copper wire is placed in the uniform magnetic...
Potentiometer01:30

Potentiometer

Voltage and current measurements using a standard voltmeter and ammeter alter the circuit being measured either by drawing or resisting the current flow, which introduces uncertainties in the measurements. Null measurements balance the voltages so that no current flows through the measuring device and, therefore, no alterations occur in the measured circuit.
Suppose the emf of a battery needs to be measured. If the battery is directly connected to a standard voltmeter, the measured quantity is...
Biasing of P-N Junction01:16

Biasing of P-N Junction

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...
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

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...
Debye–Huckel–Onsager Conductance Equation01:28

Debye–Huckel–Onsager Conductance Equation

The Debye-Hückel-Onsager equation is a cornerstone of physical chemistry, providing a method to determine the molar conductance (Λm) and molar conductance at infinite dilution (Λ°m) for uni-univalent electrolytes.Uni-univalent electrolytes are electrolytes that dissociate in solution to produce one cation with a +1 charge and one anion with a –1 charge per formula unit.This equation addresses two crucial phenomena: the asymmetry effect and the electrophoretic effect. According to this equation,...

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相关实验视频

Updated: May 26, 2026

Design, Fabrication, and Experimental Characterization of Plasmonic Photoconductive Terahertz Emitters
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GaAs中红外电气调节的元表面

Hyun Uk Chae1, Bo Shrewsbury2, Ragib Ahsan1

  • 1Ming Hsieh Department of Electrical and Computer Engineering, University of Southern California, Los Angeles California 90089, United States.

Nano letters
|February 13, 2024
PubMed
概括
此摘要是机器生成的。

研究人员使用III-V金属-半导体-金属 (MSM) 结构开发了可调节的元表面. 这一创新允许在中红外范围内通过载波度调制进行光学调整.

关键词:
在 GaAsAs 的情况下.第三-五 薄膜薄膜表轴转移是指表轴转移.metasurface 地表的表面是什么热排放的热排放量

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科学领域:

  • 光电学是指光电子产品.
  • 超材料科学科学 超材料科学
  • 半导体物理 半导体物理

背景情况:

  • 超表面具有独特的光学特性,但往往缺乏电调性.
  • III-V 半导体对于光电子设备至关重要,但将它们集成到可调节的元表面具有挑战.

研究的目的:

  • 使用III-V金属-半导体-金属 (MSM) 结构来演示可电调的元表面.
  • 通过调节载波度,探索在中红外 (中红外) 范围内共振波长的可调性.

主要方法:

  • 通过 III-V 薄膜在金属表面上的表轴转移来制造 III-V MSM 结构.
  • 集成一个p-i-n化 (GaAs) 连接与金金属层.
  • 通过改变顶部金属格子的几何形状和通过多级偏差调节载体度来调整共振波长.

主要成果:

  • 成功实现了III-V的MSM结构,没有重度杂的半导体.
  • 通过载体度调制,在中红外范围展示系统的共振调制性.
  • 实现了具有多层偏差的元表面的电调性.

结论:

  • 开发的III-V MSM结构是电调式元表面的基本构建块.
  • 该研究有助于理解在偏差条件下的III-V材料中的光学调机制.
  • 这项工作为中红外光谱中先进的可调光学设备铺平了道路.