在中镜环中的波动超导性
Nicholas C Koshnick1, Hendrik Bluhm, Martin E Huber
1Department of Applied Physics, Stanford University, Stanford, CA 94305, USA.
概括
研究人员研究了超导环中的热波动,发现单个参数解释了它们在相位过渡附近的行为. 这项工作验证了这些引人入胜的中视系统的现有理论.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子现象是一种量子现象.
背景情况:
- 阶段过渡表现出显著的波动,具有挑战性的定量描述.
- 介光环中的超导性显示了依赖磁场的临界温度,使其成为一个独特的系统.
- 现有的理论准确地描述了一维超导环中的热波动.
研究的目的:
- 量化研究介质超导环中的热波动.
- 为了验证模型系统中热波动的确切理论.
- 为了确定与临界温度抑制相关的波动重要性的参数.
主要方法:
- 使用扫描超导量子干扰装置 (SQUID) 进行高灵敏度磁性测量.
- 测量了单个中距离超导环的磁性易感性.
- 在应用的流量中隔离了极小的磁信号.
主要成果:
- 实验结果与超导环的既定波动理论一致.
- 证明单个参数有效地描述波动的影响.
- 确定了特定的磁场范围,其中波动显著影响临界温度.
结论:
- 热波动的确切理论准确地描述了介面层超导环中的实验数据.
- 一个单一的统一参数决定了波动的重要性,特别是当临界温度被抑制时.
- 介光超导环作为一个优秀的模型系统,用于研究相位过渡附近的量子波动.
更多相关视频
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
08:55Methods of Ex Situ and In Situ Investigations of Structural Transformations: The Case of Crystallization of Metallic Glasses
Published on: June 7, 2018
相关概念视频
Theory of Metallic Conduction
The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the theory of metallic conduction.
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
Types Of Superconductors
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...
Superconductor
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...
Ferromagnetism
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...
Biasing of Metal-Semiconductor Junctions
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Magnetic Field Due To A Thin Straight Wire
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.
