阿哈罗诺夫-博姆干扰和在拓绝缘环中的相一致表面状态传输
Gerrit Behner1,2, Abdur Rehman Jalil1,2, Dennis Heffels1,2
1Peter Grünberg Institut (PGI-9), Forschungszentrum Jülich, 52425 Jülich, Germany.
Nano letters
|July 3, 2023
概括
拓绝缘环表现出Aharonov-Bohm振荡,这是由于其表面状态中的相连贯传输. 这些拓的表面状态保持弹道运输,即使在扩散散散货运船.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 量子现象是一种量子现象.
背景情况:
- 拓绝缘器 (TI) 具有独特的表面状态,有可能用于新的电子应用.
- 了解TI纳米结构中的相连贯性对于利用它们的量子性质至关重要.
研究的目的:
- 为了研究基于甲 (Sb2Te3) 的拓绝缘体环结构中的相连贯传输.
- 阐明阿哈罗诺夫-博姆振荡的起源及其与拓表面状态的关系.
主要方法:
- 在Sb2Te3拓绝缘环上进行低温磁传输测量.
- 对导电率振荡及其温度依赖性的分析.
- 与Aharonov-Bohm型振荡在拓绝缘器纳米丝带中的比较.
主要成果:
- 在TI环的导电性中观察到明显的阿哈罗诺夫-博姆振荡,表明相连贯运输.
- 振荡幅度的温度依赖性表明环臂沿着弹道运输,归因于拓表面状态.
- 在拓表面状态中,相位连贯性在长距离上保持,即使使用扩散散散载体.
结论:
- 在Sb2Te3环中的拓表面状态支持远程相连贯弹道运输.
- 阿哈罗诺夫-博姆振荡是这种拓表面状态运输的明确标志.
- 这些发现突显了拓绝缘体在强大的量子电子设备中的潜力.
相关概念视频
Electric Field at the Surface of a Conductor
4.7K
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...
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...
4.7K
π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds
1.2K
In aromatic compounds, such as benzene, the circulation of (4n + 2) π-electrons sets up a diamagnetic or diatropic ring current around the perimeter of the molecule. This current induces a magnetic field that opposes the external field inside the ring and reinforces it on the outside. The protons in benzene are deshielded and exhibit high chemical shifts in the range 6.5–8.5 ppm. The shielding effect at the center of the ring is evident in complex aromatic molecules, such as...
1.2K
Equipotential Surfaces and Conductors
3.5K
For a conductor in which all charges are at rest, the conductor's surface is equipotential. The electric field is always perpendicular to equipotential surfaces. Therefore, in a conductor with static charges, the electric field just outside the conductor is always perpendicular to the conductor's surface. Any tangential component of the electric field will cause charges to move inside the conductor, which will violate the electrostatic nature of the system. In an electrostatic...
3.5K
Interference: Path Lengths
1.3K
Consider two sources of sound, that may or may not be in phase, emitting waves at a single frequency, and consider the frequencies to be the same.
Two special sources may be considered when they are in phase. This can be easily achieved by feeding the two sources from the same source. An example would be synchronizing the two speakers by feeding them with the same source, such as the sound waves produced by a tuning fork. This setup ensures that the two sources have the same frequency and are...
Two special sources may be considered when they are in phase. This can be easily achieved by feeding the two sources from the same source. An example would be synchronizing the two speakers by feeding them with the same source, such as the sound waves produced by a tuning fork. This setup ensures that the two sources have the same frequency and are...
1.3K
Phase Transitions
19.2K
Whether solid, liquid, or gas, a substance's state depends on the order and arrangement of its particles (atoms, molecules, or ions). Particles in the solid pack closely together, generally in a pattern. The particles vibrate about their fixed positions but do not move or squeeze past their neighbors. In liquids, although the particles are closely spaced, they are randomly arranged. The position of the particles are not fixed—that is, they are free to move past their neighbors to...
19.2K
The de Broglie Wavelength
26.0K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
26.0K


