在UTe_{2}中,压力诱导的多元件超导的磁性特征
Zheyu Wu1, Jiasheng Chen1, Theodore I Weinberger1
1Cavendish Laboratory, University of Cambridge, Cambridge CB3 0HE, United Kingdom.
Physical review letters
|June 27, 2025
概括
高压揭示了二化 (UTe2) 中新的超导相. 磁感应度测量显示了明显的过渡,表明在极端条件下复杂的,可能是多元件的超导.
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
- 超导性研究 超导性研究
背景情况:
- 沉重的费米离子化合物二化 (UTe2) 呈现出复杂的相图,具有多个超导相.
- 在UTe2中,一些超导相表现出暗示奇偶配对的特征.
- 了解UTe2的压力依赖性行为对于阐明其奇特的超导特性至关重要.
研究的目的:
- 研究高质量的UTe2晶体中超导过渡的压力依赖性.
- 在不同压力条件下识别超导体顺序参数的变化.
- 探索在高压下在UTe2中多元件超导的可能性.
主要方法:
- 利用磁感应度 (χ(T)) 测量来追踪超导过渡.
- 对高质量的UTe2单晶体施加水静压.
- 与之前的特定热量测量相关联的磁性敏感性数据.
主要成果:
- 在低压下 (<0.3 GPa) 观察到单个,的超导过渡.
- 检测到第二个,不同的超导过渡异常在更高的压力在磁性易感性.
- 这种异常与伦敦透深度的阶段变化有关,表明超导顺序参数的变化.
结论:
- 在UTe2中,高压超导状态在热力学上与零压状态不同.
- 新发现的低温高压超导状态与高压高温状态不同.
- 这些发现强烈表明UTe2在高压下存在多元件超导.
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
8.2K
08:42High-Sensitivity Nuclear Magnetic Resonance at Giga-Pascal Pressures: A New Tool for Probing Electronic and Chemical Properties of Condensed Matter under Extreme Conditions
Published on: October 10, 2014
11.7K
相关概念视频
Magnetic Susceptibility and Permeability
1.4K
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
1.4K
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
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
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
Magnetic Field due to Moving Charges
9.3K
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...
9.3K
Paramagnetism
2.6K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
2.6K
