在LaFeO3/SrTiO3接口上的一个二维超导电子气体.
Zhangwen Mao1,2, Dawei Qiu3, Zhihang Xu4
1National Laboratory of Solid State Microstructures, Jiangsu Key Laboratory of Artificial Functional Materials, College of Engineering and Applied Sciences, Nanjing University, Nanjing 210023, P. R. China.
Nano letters
|December 17, 2024
概括
在LaFeO3/SrTiO3接口的二维电子气体 (2DEG) 中发现了超导性,表现出可调节的特性和Berezinskii-Kosterlitz-Thouless过渡,为量子研究提供了一个新的平台.
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
- 量子现象是一种量子现象.
背景情况:
- 过渡金属氧化物接口显示出在散装材料中没有的独特特性.
- 在这些接口中,超导和磁性的共存是一个关键的研究领域.
研究的目的:
- 报告2DEG在LaFeO3/SrTiO3接口中的超导性的发现.
- 描述这种新兴超导的性质和可调性.
主要方法:
- 在LaFeO3/SrTiO3异构结构的制造.
- 电传输测量,包括电阻和磁阻.
- 低温表征以观察超导过渡和贝雷津斯基-科斯特利茨-托勒斯行为.
主要成果:
- 在2DEG中观察到的超导率在LaFeO3/SrTiO3接口,过渡温度 (Tc) 为333mK,层厚为13.7nm.
- 证据证明二维超导的证据通过Berezinskii-Kosterlitz-Thouless过渡得到证实.
- 门电压 (Vg) 对Tc的依赖性表现出圆顶形的行为,表明可调性.
- 在超导体制中观察到的歇斯底里磁电阻.
结论:
- 在LaFeO3/SrTiO3接口中,可以设置可调的二维超导状态.
- 该系统为探索氧化物接口中的量子现象提供了一个新的平台.
- 需要进一步的研究,以了解观察到的歇斯底里的磁电阻背后的机制.
相关概念视频
Types Of Superconductors
933
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...
933
Ferromagnetism
2.4K
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...
2.4K
Superconductor
1.1K
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...
1.1K
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
Fermi Level
485
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
485
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


