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関連する概念動画

The Hall Effect01:30

The Hall Effect

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Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
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Superconductor01:24

Superconductor

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A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
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Electric Field Inside a Conductor01:20

Electric Field Inside a Conductor

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When a conductor is placed in an external electric field, the free charges in the conductor redistribute and very quickly reach electrostatic equilibrium. The resulting charge distribution and its electric field have many interesting properties, which can be investigated with the help of Gauss's law.
Suppose a piece of metal is placed near a positive charge. The free electrons in the metal are attracted to the external positive charge and migrate freely toward that region. This region then...
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Electric Field at the Surface of a Conductor01:26

Electric Field at the Surface of a Conductor

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Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
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Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

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A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
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Electric Field of Parallel Conducting Plates01:16

Electric Field of Parallel Conducting Plates

1.9K
Gauss' law relates the electric flux through a closed surface to the net charge enclosed by that surface. Gauss's law can be applied to find the electric field and the charge enclosed in a region depending on its charge distribution.
Consider a cross-section of a thin, infinite conducting plate having a positive charge. For such a large thin plate, as the thickness of the plate tends to zero, the positive charges lie on the plate's two large faces. Without an external electric field, the...
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関連する実験動画

Updated: Mar 21, 2026

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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超電流は量子ハール体制で

F Amet1, C T Ke2, I V Borzenets3

  • 1Department of Physics, Duke University, Durham, NC 27708, USA. Department of Physics and Astronomy, Appalachian State University, Boone, NC 28607, USA. ametf@appstate.edu gleb@phy.duke.edu.

Science (New York, N.Y.)
|May 21, 2016
PubMed
まとめ
この要約は機械生成です。

研究者は,超伝導性とグラフェンのQH効果を組み合わせて,量子ホール (QH) 体制で超電流を観測した. この画期的な発見は 量子コンピューティングのための マジョラーナ・フェルミオンのような 異質なトポロジック刺激の探求を進めています

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

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科学分野:

  • 凝縮物質物理学
  • 量子現象について

背景:

  • 超伝導性と量子ホール効果を組み合わせることで トポロジカル状態への経路が提供されます
  • QH システムにおける超伝導性シグネチャと,QH 弱いリンクにおける超電流の観測は依然として困難である.

研究 の 目的:

  • 超電流のメカニズムを 量子ホールシステムで証明する
  • エキゾチックなトポロジカルな刺激の探求を進めるため

主な方法:

  • 封装されたグラフェンサンプルを使用した.
  • 超伝導電極と接触したサンプル
  • 磁場は2テスラまで

主要な成果:

  • QHシステム内の封装グラフェンで 明確な超電流が示されました
  • 2テスラまでの磁場で 超電流を観測しました

結論:

  • QH体制における超電流の観測は重要なステップです.
  • この発見は,誤差を許容する量子コンピューティングのためのマジョラーナフェルミオンとパラフェルミオンの探求を助けます.