Jove
Visualize
联系我们
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

相关概念视频

Energy Bands in Solids01:01

Energy Bands in Solids

1.2K
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.
 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...
1.2K
Fermi Level Dynamics01:12

Fermi Level Dynamics

337
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...
337
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.1K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
1.1K
Fermi Level01:18

Fermi Level

797
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
797
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

502
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...
502
Types of Semiconductors01:20

Types of Semiconductors

907
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
907

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

Large-scale analogue quantum simulation using atom dot arrays.

Nature·2026
Same author

Nonlinear transport fingerprints of tunable Fermi-arc connectivity in magnetic Weyl semimetal Co<sub>3</sub>Sn<sub>2</sub>S<sub>2</sub>.

Reports on progress in physics. Physical Society (Great Britain)·2026
Same author

Genome-wide association study on carcass traits in an indigenous yellow-feathered meat-type chicken population.

Animal : an international journal of animal bioscience·2026
Same author

An 11-qubit atom processor in silicon.

Nature·2025
Same author

A NEW-FOUND ARMC5 GERMLINE VARIANT IN PRIMARY BILATERAL MACRONODULAR ADRENAL HYPERPLASIA USING WHOLE-EXOME SEQUENCING AND PROTEIN PREDICTIVE ANALYSIS.

Acta endocrinologica (Bucharest, Romania : 2005)·2025
Same author

Genomic-based animal management in the early- and late-finishing system of Hanwoo cattle.

Animal : an international journal of animal bioscience·2025

相关实验视频

Updated: Sep 7, 2025

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
15:47

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots

Published on: November 1, 2013

16.4K

基于原子的半导体量子点的工程拓状态

M Kiczynski1,2, S K Gorman1,2, H Geng1,2

  • 1Centre of Excellence for Quantum Computation and Communication Technology, School of Physics, UNSW Sydney, Kensington, New South Wales, Australia.

Nature
|June 22, 2022
PubMed
概括
此摘要是机器生成的。

研究人员创建了一个可控制的费米子量子系统来模拟Su-Schrieffer-Heeger (SSH) 模型. 这一突破使得在量子模拟中研究拓物质和强相关的电子成为可能.

更多相关视频

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
All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

Published on: January 19, 2018

9.8K

相关实验视频

Last Updated: Sep 7, 2025

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
15:47

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots

Published on: November 1, 2013

16.4K
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
All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

Published on: January 19, 2018

9.8K

科学领域:

  • 凝聚物质物理学
  • 量子模拟
  • 拓学问题

背景情况:

  • 控制的费米子量子系统对于探索凝聚物质物理学至关重要.
  • 半导体量子点提供了量子模拟的希望,因为它们具有强大的量子相关性.
  • 模拟多体苏-施里弗-希格尔 (SSH) 模型是由于工程长距离相互作用的困难而具有挑战性.

研究的目的:

  • 使用可控制的费米子量子系统实现多体SSH模型的微不足道和拓阶段.
  • 为了证明工程量子点的能力模拟复杂的量子哈密尔顿.
  • 展示一个高度可控的量子系统,

主要方法:

  • 使用精确放置的原子,具有强大的库伦限制.
  • 设计了六个全角形的平面门来调整10个量子点的线性阵列中的能量水平.
  • 杆子子纳米精度门工程在分阶设计中控制细胞间和细胞内电子传输.

主要成果:

  • 成功实现了多体SSH模型的微不足道和拓阶段.
  • 在四分之一填充时观察到拓阶段的清晰标志,其中有两个导电性峰值.
  • 将拓阶段与微不足道阶段的十个导电峰进行对比,显示出不同的量子行为.

结论:

  • 工程量子点系统为量子模拟提供了一个高度可控的平台.
  • 这项工作克服了模拟多体SSH模型的先前挑战.
  • 这种系统对于未来的强相互作用电子和拓物质研究具有价值.