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相关概念视频

MOSFET: Enhancement Mode01:22

MOSFET: Enhancement Mode

246
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
246
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

250
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...
250
MOSFET: Depletion Mode01:20

MOSFET: Depletion Mode

285
Depletion-mode MOSFETs represent a unique subset of MOSFET technology, functioning fundamentally differently from their enhancement-mode counterparts. Unlike enhancement MOSFETs, which require a positive gate-source voltage (Vgs) to turn on, depletion-mode MOSFETs are inherently conductive and "normally on" devices.
The primary characteristic of depletion-mode MOSFETs is their ability to conduct current between the drain and source terminals without gate bias. This inherent conductivity...
285
P-N junction01:11

P-N junction

410
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...
410
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

827
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
827
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

176
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...
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相关实验视频

Updated: May 14, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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在芯片上主动超合的拓腔.

Ridong Jia1,2, Wenhao Wang1,2, Yi Ji Tan1,2

  • 1Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore, 637371, Singapore.

Advanced materials (Deerfield Beach, Fla.)
|April 11, 2025
PubMed
概括

这项研究引入了一种用于芯片上的光子学的新型超合拓腔,可以在多个波长上激发. 这一突破克服了用于灵活芯片集成的传统 evanescent 合的局限性.

关键词:
THz在芯片上的空腔.THz拓的光子集成电路.在芯片上的特拉赫兹互连连接.光热控制的控制方法超合的腔体合特拉赫兹界面波导的波导.拓性空洞是一个拓性空洞.

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科学领域:

  • 光子学是指光子学的使用方法.
  • 集成光学 集成光学 集成光学
  • 拓式光子学 拓式光子学

背景情况:

  • 芯片上的光子共振腔对于激光,传感和光谱学至关重要.
  • 目前的激发方法依赖于 evanescent 合,限制了集成的灵活性.
  • 亚波长合距离限制了精确的芯片上设备放置.

研究的目的:

  • 为了展示一种新的芯片上超合的拓腔.
  • 为了克服短距离 evanescent 合的局限性.
  • 为了使对长距离的共振腔的激发.

主要方法:

  • 使用基于山谷流的超合机制.
  • 实现光热加热用于动态控制.
  • 在2.3波长的距离上实现关键合,激发到3.2波长.

主要成果:

  • 证明了一个超合的拓腔,具有扩展的激发范围.
  • 在2.3波长实现了临界合,在3.2波长实现了持续激发.
  • 展示了可调节的质量因素和通过光热加热通过合的动态控制.

结论:

  • 超合机制显著延长波导-波腔激发距离.
  • 这项技术为芯片上的共振器件设计打开了新的可能性.
  • 实现了先进的超合激光器,传感器和调制器,具有增强的控制.