在混合Au/YBa2Cu3O7-x电极上诱导的超导性
Irina Gundareva1,2, Jose Martinez-Castro3,2,4, Frank Stefan Tautz3,2,5
1Peter Grünberg Institute (PGI-9), Forschungszentrum Jülich, 52425, Jülich, Germany.
Scientific reports
|September 1, 2025
概括
我们使用黄金和铜氧化物 (YBCO) 制造了新的超导混合电极. 这些电极在黄金中表现出强大的超导能量缺口,使高温约瑟夫森装置成为可能.
科学领域:
- 凝聚物质物理学
- 材料科学
- 量子技术
背景情况:
- 超导电极对于量子技术中的混合Josephson连接至关重要.
- 传统的Au/YBCO电极在能量差值和变化方面存在限制.
研究的目的:
- 在附近基板上制造和描述新的超导 Au/YBa2Cu3O7-x (YBCO) 电极.
- 调查黄金中诱导的超导能量缺口的起源和特性.
主要方法:
- 使用面向金膜的CuO2平面制造Au/YBCO异构结构.
- 在现场沉积在YBCO膜上的薄金层.
- 扫描道显微镜 (STM) 来测量能量间隙.
- 制造用于电传输测量的纳米收缩.
主要成果:
- 在混合电极的金面上观察到10-17 meV的能量差距.
- 通过纳米收缩的多个Andreev反射, 证明了黄金的超导性.
- 与传统电极相比,实现更高的诱导能量差值.
结论:
- 制造的Au/YBCO电极为高温混合Josephson设备提供了一个有前途的平台.
- YBCO薄膜的方向对混合界面的超导特性产生重大影响.
- 这项工作促进了超导电子和量子信息处理材料的开发.
更多相关视频
06:49Radio Frequency Magnetron Sputtering of GdBa2Cu3O7âˆ'ÃŽ ´/ La0.67Sr0.33MnO3 Quasi-bilayer Films on SrTiO3 STO Single-crystal Substrates
Published on: April 12, 2019
7.7K
07:13High Temperature Fabrication of Nanostructured Yttria-Stabilized-Zirconia YSZ Scaffolds by In Situ Carbon Templating Xerogels
Published on: April 16, 2017
10.9K
相关概念视频
Types Of Superconductors
1.1K
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...
1.1K
Superconductor
1.2K
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...
1.2K
Charging Conductors By Induction
8.2K
The Earth is a good conductor of electricity, and it is so big that it can be considered an infinite source or sink of charges. It can easily exchange charges with any matter.
Generally, conductors like metals do not allow any excess charge to be present on them. Any excess charge added to metals easily flows away, for example, when a metal is placed on the Earth. This process is called earthing.
However, conductors can be charged by a process called induction. For example, consider charging a...
Generally, conductors like metals do not allow any excess charge to be present on them. Any excess charge added to metals easily flows away, for example, when a metal is placed on the Earth. This process is called earthing.
However, conductors can be charged by a process called induction. For example, consider charging a...
8.2K
Ferromagnetism
2.5K
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...
2.5K
Induced Electric Fields: Applications
1.9K
An important distinction exists between the electric field induced by a changing magnetic field and the electrostatic field produced by a fixed charge distribution. Specifically, the induced electric field is nonconservative because it does not work in moving a charge over a closed path. In contrast, the electrostatic field is conservative and does no net work over a closed path. Hence, electric potential can be associated with the electrostatic field but not the induced field. The following...
1.9K
Induced Electric Dipoles
4.4K
A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
4.4K
