グラフェン超格子におけるトポロジカル電流の検出
R V Gorbachev1, J C W Song2, G L Yu3
1Centre for Mesoscience and Nanotechnology, University of Manchester, Manchester M13 9PL, UK. School of Physics and Astronomy, University of Manchester, Oxford Road, Manchester M13 9PL, UK.
まとめ
トポロジカル・マテリアルは,磁場のない独特のホール型電流を発揮する. グラフェン超格子には,長距離,電荷中立の流れが示され,新しいバレーベースの情報処理が可能です.
科学分野:
- 凝縮物質物理学 凝縮物質物理学
- マテリアルサイエンス 材料科学
- ナノテクノロジー ナノテクノロジー
背景:
- トポロジカルな材料は,磁場なしで横断電流を生成することができる.
- 逆対称性が破られたグラフェン超網は,独特の谷間依存のトポロジカル電流を宿していることが予測されています.
研究 の 目的:
- グラフェン超格子における予測された長距離,中性電荷のトポロジカル電流を実験的に観察し,特徴づけること.
- 将来の電子アプリケーションのためのこれらのトポロジカル電流の可能性を調査する.
主な方法:
- 逆対称性が破られたグラフェン超網の製造.
- ディラック点近くの磁場ゼロにおける非局所電圧の測定.
- 電流の強度とゲート電圧制御の特徴.
主要な成果:
- 磁場ゼロにおけるトポロジカル電流を示す非ローカル電圧の観測.
- これらの電流を数ミクロメートルの範囲で検知し,遠距離輸送を証明した.
- トポロジカルな電流は,適用された電流と強さで比較可能であることが判明し,大きなバレー・ホール角を暗示しています.
結論:
- グラフェン超格子における予測されたトポロジカル電流の実験的確認.
- 長距離の電荷中性フローとトランジスタのような制御の実証.
- グラフェンの自由度渓谷を利用して,新しい情報処理装置の開発の可能性.
関連する概念動画
Mesh Analysis with Current Sources
2.4K
Mesh analysis becomes simpler when analyzing circuits with current sources, whether independent or dependent. The presence of current sources reduces the number of equations required for analysis. Two cases illustrate this:
Current Source in One Mesh: The analysis process is straightforward when a current source is found in only one mesh within the circuit. Mesh currents are assigned as usual, with the mesh containing the current source excluded from the analysis. Kirchhoff's voltage law...
Current Source in One Mesh: The analysis process is straightforward when a current source is found in only one mesh within the circuit. Mesh currents are assigned as usual, with the mesh containing the current source excluded from the analysis. Kirchhoff's voltage law...
2.4K
Magnetic Field Of A Current Loop
6.0K
Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.
6.0K
Boundary Conditions for Current Density
1.4K
Current density becomes discontinuous across an interface of materials with different electrical conductivities. The normal component of the current density is continuous across the boundary.
1.4K
Types Of Superconductors
1.6K
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
1.6K
Magnetic Field due to Moving Charges
11.2K
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...
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...
11.2K
Magnetic Force Between Two Parallel Currents
3.7K
Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the...
3.7K


