在近似一维超导体V2Ga5中的异型超导
G Lamura1, D Tay2, R Khasanov3
1CNR-SPIN, I-16152, Genova, Italy.
Scientific reports
|April 23, 2025
概括
V2Ga5,一个二进制超导体,表现出一个拓上非碎的正常状态和异构超导性. 研究人员使用磁化,核磁共振和子旋转来研究其电子性质,揭示了一个完全间隙的异性质超导状态.
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
- 超导电性 超导电性 超导电性
背景情况:
- V2Ga5是一种金属间二元超导体.
- 它具有一个近乎一维的结构.
- 最近的发现表明一个拓上非碎的正常状态,使其成为拓超导的候选者.
研究的目的:
- 研究V2Ga5在正常和超导状态中的电子特性.
- 探索异构性在其电子行为中的作用.
- 搜索拓特征和非传统的超导.
主要方法:
- 使用了优质的V2Ga5单晶.
- 使用的DC磁化测量仪.
- 进行的核磁共振 (NMR) 光谱学.
- 在不同的条件下 (温度,压力,磁场) 进行子旋转 (SR) 光谱.
主要成果:
- 在正常状态下,NMR揭示了线位移和放松率的强烈异构性.
- 磁化和SR在超导状态下证实了持续的异构性.
- 超导性被发现是完全缺口的,并且具有强烈的异构性.
- 液压压力影响了临界温度 ([公式:见文本]),但并没有影响超流体密度.
- 观察到[公式:参见文本]SR光谱中的峰值分裂,可能表明一种非常规的旋格子.
结论:
- V2Ga5是一个新的系统,在这种系统中,异构性对其电子性质至关重要.
- 该材料显示了拓超导体候选材料的特征.
- 对观察到的非常规状网和拓特征进行进一步的研究是有必要的.
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
8.0K
04:51Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
Published on: July 8, 2021
2.7K
相关概念视频
Types Of Superconductors
880
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...
880
Superconductor
1.0K
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...
1.0K
Theory of Metallic Conduction
1.3K
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,...
1.3K
Ferromagnetism
2.3K
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...
2.3K
Electric Field Inside a Conductor
5.8K
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...
5.8K
Electric Field at the Surface of a Conductor
4.5K
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...
4.5K
