Jove
Visualize
联系我们

相关概念视频

Schottky Barrier Diode01:27

Schottky Barrier Diode

507
Schottky barrier diodes are specialized semiconductor devices characterized by their unique construction. This construction involves combining a metal layer with a moderately doped n-type semiconductor material. This combination leads to the formation of a Schottky barrier, a pivotal element that defines the diode's operational characteristics. The core functionality of Schottky barrier diodes is their capacity to allow current to flow in only one direction due to their distinctive...
507
Diode: Forward bias01:20

Diode: Forward bias

1.3K
In semiconductor devices, diodes play a crucial role in directing current flow, and its operation is primarily categorized into forward bias and reverse bias. A diode is said to be forward-biased when its p-type region is connected to the positive terminal of a battery and its n-type region is linked to the negative terminal. This configuration reduces the potential barrier within the diode, allowing current to flow easily from the p to the n-type region.
The behavior of a diode in forward bias...
1.3K
Diode: Reverse bias01:14

Diode: Reverse bias

1.0K
A diode is reverse-biased when the positive terminal of an external voltage source is connected to the n-type material and the negative terminal to the p-type material. This configuration opposes the natural direction of current flow through the diode, effectively increasing the width of the depletion region and the barrier potential. The reverse bias condition produces a minimal leakage current, primarily due to minority charge carriers. This leakage becomes significant when the reverse...
1.0K
Biasing of P-N Junction01:16

Biasing of P-N Junction

914
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...
914
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

343
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...
343
Induced Electric Fields01:23

Induced Electric Fields

3.9K
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...
3.9K

您也可能阅读

相关文章

通过共同作者、期刊和引用图与本文相关的文章。

排序
Same author

Thermoelectric Detection of Crossed Andreev Reflections in Quantum Hall/Superconductor Hybrid Structures.

Nature communications·2026
Same author

Tuning Chiral Anomaly Signature in a Dirac Semimetal via Fast-Ion Implantation.

Nano letters·2025
Same author

Chiral edge state control of thermoelectric effects.

Science advances·2025
Same author

Valence Electron Distributions from Sub-Angstrom Convergent Beam Electron Diffraction.

Nano letters·2025
Same author

Near-infrared photodetection and time-resolved photocurrents in cadmium arsenide heterojunctions.

Optics letters·2024
Same author

Tuning Displacement Fields in a Two-Dimensional Topological Insulator Using Nanopatterned Gates.

Nano letters·2024
JoVE
x logofacebook logolinkedin logoyoutube logo
关于 JoVE
概览领导团队博客JoVE 帮助中心
作者
出版流程编辑委员会范围与政策同行评审常见问题投稿
图书馆员
用户评价订阅访问资源图书馆顾问委员会常见问题
研究
JoVE JournalMethods CollectionsJoVE Encyclopedia of Experiments存档
教育
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab Manual教师资源中心教师网站
使用条款与条件
隐私政策
政策

相关实验视频

Updated: Sep 18, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
05:39

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

Published on: August 2, 2019

9.8K

自场诱导的约瑟夫森二极管效应

Arman Rashidi1, Sina Ahadi1, Susanne Stemmer1

  • 1Materials Department, University of California, Santa Barbara, California 93106-5050, United States.

Nano letters
|June 23, 2025
PubMed
概括
此摘要是机器生成的。

这项研究揭示了超电流的自我场可以在超导交点中诱导约瑟夫森二极管效应 (JDE). 这些发现对于开发先进的超导电子和量子技术至关重要.

关键词:
约瑟夫森二极管是什么意思约瑟夫森交叉口 约瑟夫森交叉口超导量子干扰是一种超导量子干扰.拓绝缘体的拓绝缘体是一个

更多相关视频

High-resolution Thermal Micro-imaging Using Europium Chelate Luminescent Coatings
09:01

High-resolution Thermal Micro-imaging Using Europium Chelate Luminescent Coatings

Published on: April 16, 2017

7.9K
Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
14:58

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping

Published on: June 3, 2015

14.9K

相关实验视频

Last Updated: Sep 18, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
05:39

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform

Published on: August 2, 2019

9.8K
High-resolution Thermal Micro-imaging Using Europium Chelate Luminescent Coatings
09:01

High-resolution Thermal Micro-imaging Using Europium Chelate Luminescent Coatings

Published on: April 16, 2017

7.9K
Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
14:58

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping

Published on: June 3, 2015

14.9K

科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 量子电子学 量子电子学
  • 材料科学 材料科学 材料科学

背景情况:

  • 约瑟夫森二极管是关键的非线性超导电路元件.
  • 应用包括固态量子比特读取和合.
  • 各种机制可以产生约瑟夫森二极管效应 (JDE).

研究的目的:

  • 调查超级电流的自我场所产生的JDE.
  • 在平面混合Josephson连接处探索JDE.
  • 了解超导器件中自场效应的作用.

主要方法:

  • 在超电流量子干扰模式中对JDE进行实验研究.
  • 使用平面混合体约瑟夫森连接与化和超导体.
  • 开发了一种包含超电流自场的模型.

主要成果:

  • 包括超电流自场在内的模型准确地描述了实验观测.
  • 在特定条件下,在平面交叉点中通常预计会发生自场诱导的JDE.
  • 即使在具有足够关键电流的对称和均交叉点中也观察到JDEs.

结论:

  • 自场诱导的JDE是平面约瑟夫森交叉点的一般现象.
  • 这些效果可以通过超电流密度和其他参数进行调整.
  • 在超导电路中实现约瑟夫森二极管的新机制.