在室温下观察石墨烯中的电流旋
Marius L Palm1, Chaoxin Ding1, William S Huxter1
1Department of Physics, ETH Zurich, 8093 Zurich, Switzerland.
概括
研究人员在室温下观察到石墨烯中的电流, 这种用扫描磁力计可视化的现象在较大的设备中消失, 证实了水力动力学预测.
科学领域:
- 凝聚物质物理
- 中镜物理
背景情况:
- 高流动性导体中的电子相互作用可以模仿经典的水力学.
- 石墨烯是研究量子运输现象的关键材料.
研究的目的:
- 在室温下对单层石墨烯的水力动态传输特征进行成像和验证.
- 调查与设备大小和运输模式相关的电流的行为.
主要方法:
- 使用纳米扫描磁力计进行当地的电流成像.
- 具有不同特征尺寸的单层石墨烯制造和测量装置.
- 在孔主导,电子主导和双极系统中检查了传输特性.
主要成果:
- 在室温下的石墨烯中成功成像了静电,
- 随着装置大小的增加, 观察到电流的消失, 验证了水力动力学模型的预测.
- 在电子和孔运输中发现了流,但不是在双极状态中,这归因于流扩散长度的减少.
结论:
- 当地成像技术是揭示异国情调中镜运输现象的强大工具.
- 这项研究为石墨烯的液态电子行为提供了实验证据.
- 旋转的扩散长度在接近电荷中性的水力动力学效应的表现中起着关键作用.
相关概念视频
Atomic Force Microscopy
3.1K
Atomic force microscopy (AFM) is a type of scanning probe microscopy that can analyze topographic details of various specimens like ceramics, glass, polymers, and biological samples. AFM offers over 1000 times more resolution than the optical imaging system. Images generated from AFM are three-dimensional surface profiles, offering an advantage over the flat, two-dimensional images from other imaging techniques.
The AFM Probe
The probe is regarded as the heart of any AFM setup and comprises the...
The AFM Probe
The probe is regarded as the heart of any AFM setup and comprises the...
3.1K
Electric Field Inside a Conductor
6.4K
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...
6.4K
Electric Field at the Surface of a Conductor
4.6K
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...
4.6K
Magnetic Field Due To A Thin Straight Wire
5.1K
Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
5.1K
Ferromagnetism
2.8K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.8K
Atomic Spectroscopy: Effects of Temperature
1.2K
Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature...
1.2K


