量子霍尔系统中的超电流
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.
概括
研究人员通过结合石墨烯中的超导和QH效应观察到量子霍尔 (QH) 模式中的超电流. 这一突破推动了对奇特的拓激发的研究,
科学领域:
- 凝聚物质物理
- 量子现象
背景情况:
- 超导和量子霍尔效应的结合提供了拓状态的途径.
- 在QH系统中观察超导特征和QH弱环中的超电流仍然具有挑战性.
研究的目的:
- 为了证明量子霍尔系统中的超流机制.
- 为了进一步寻找异国情调的拓激发.
主要方法:
- 使用封装的石墨烯样本.
- 接触过超导电极的样品
- 应用磁场高达2特斯拉.
主要成果:
- 在QH系统中成功证明了封装石墨烯的明显超电流.
- 在高达2特斯拉的磁场中观察到这种超级电流.
结论:
- 在QH系统中观察超级电流是一个重要的步骤.
- 这一发现有助于寻找Majorana费米子和对费米子用于容错量子计算.
相关概念视频
The Hall Effect
4.9K
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.
4.9K
Superconductor
2.0K
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...
2.0K
Electric Field Inside a Conductor
7.8K
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...
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...
7.8K
Electric Field at the Surface of a Conductor
5.6K
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...
5.6K
Magnetic Field due to Moving Charges
12.2K
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...
12.2K
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...
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...
1.9K


