相关实验视频
Updated: Jan 16, 2026

06:53
Scanning SQUID Study of Vortex Manipulation by Local Contact
Published on: February 1, 2017
7.3K
用扫描量子显微镜探测二维超导体中的旋动力学
Sreehari Jayaram1, Malik Lenger1, Dong Zhao2,3,4
1University of Stuttgart, 3rd Institute of Physics, Allmandring 13, Stuttgart 70569, Germany.
Physical review letters
|October 5, 2025
概括
研究人员使用单旋显微镜研究2D超导体中的磁动力学. 他们发现了低于临界温度的意外磁噪声,表明超导材料的内在波动.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 纳米技术 纳米技术
- 量子科学 是一个量子科学.
背景情况:
- 了解纳米级磁力动力学是超导体行为的关键.
- 2D超导体中的旋转动力学是复杂的,并未完全理解.
研究的目的:
- 用单旋扫描量子显微镜探测二维超导体NbSe2中的动力学.
- 研究2D超导体中低于临界温度的磁噪声和波动的性质.
主要方法:
- 使用单旋扫描量子显微镜测量磁力学动力学.
- 通过旋转脱凝度测量分析了形配置和磁噪声.
主要成果:
- 观察到一个混乱的旋转玻璃相,在临界温度附近融化.
- 在Tc以下检测到持续的磁噪声,在较低的温度下增加.
- 有证据表明,由于超电流密度和热波动竞争,噪声的内在来源.
结论:
- 单旋显微镜是研究二维超导体波动的强大工具.
- 这些发现挑战了对超导体中低于Tc的磁性行为的传统预期.
- 这项研究为驱动2D超导系统中的磁噪声的内在机制提供了新的见解.
相关概念视频
Overview of Microscopy Techniques
14.8K
The early pioneers of microscopy opened a window into the invisible world of microorganisms. In 1830, Joseph Jackson Lister created an essentially modern light microscope. The 20th century saw the development of microscopes that leveraged nonvisible light, such as fluorescence microscopy that uses an ultraviolet light source and electron microscopy that uses short-wavelength electron beams. These advances significantly improved magnification, image resolution, and contrast. By comparison, the...
14.8K
Atomic Force Microscopy
4.4K
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...
4.4K
Magnetic Field due to Moving Charges
11.5K
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...
11.5K
Magnetic Field Of A Current Loop
6.2K
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.
6.2K
Electric Field at the Surface of a Conductor
5.2K
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...
5.2K
Electric Field Inside a Conductor
7.2K
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...
7.2K

