一种散装形式的基于Cu的铁磁半导体 (La,Ba) ((Cu,Mn) SO,其基里温度高达170K
Jinou Dong1, Cui Ding1, Xueqin Zhao1
1Zhejiang Province Key Laboratory of Quantum Technology and Device and School of Physics, Zhejiang University, Hangzhou, 310027, China.
Scientific reports
|September 5, 2023
概括
研究人员在一个新的基于铜的磁性半导体中发现了铁磁性, (La,Ba) ((Cu,Mn) SO.SO. 这种材料表现出由载体介导的远程铁磁排序,达到高达170K的基里温度.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学是一种材料科学.
- 磁力学 磁力学 是一种
背景情况:
- 原型的基于铁的1111型超导体LaFeAsO作为结构参考.
- LaCuSO是开发新型磁性半导体的原始化合物.
- 引入载体和旋转对于实现磁性排序至关重要.
研究的目的:
- 为了研究基于Cu的磁性半导体 (La,Ba) 的新型散装 (Cu,Mn) SO.SO.中的铁磁性.
- 探索载体度,旋转兴奋剂和磁性排序之间的关系.
- 了解化学压力对铁磁性质的影响.
主要方法:
- 合成具有不同兴奋剂水平的 (La,Ba) ((Cu,Mn) SO化合物.
- 结构特征证实与1111型超导体的同结构关系.
- 测量磁性特性以确定基里温度和排序类型.
主要成果:
- 在 (La,Ba) ((Cu,Mn) SO.SO中成功诱导了铁磁性.
- 观察到远距离的铁磁顺序,由载体介导.
- 在10%的Ba和5%的Mn兴奋剂下,达到170K的最大基里温度.
- 通过对 (La,Sr) ((Cu,Mn) SO) 的Sr兴奋剂诱导的负化学压力被证明可以抑制铁磁性.
结论:
- 这项研究表明,通过载体和旋转兴奋剂,在基于Cu的材料中实现铁磁性的可行途径.
- (La,Ba) ((Cu,Mn) SO代表了一类新的磁性半导体,具有潜在的应用.
- 化学压力在调整这些材料中的磁性秩序方面发挥着重要作用.
相关概念视频
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
Fermi Level
654
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,...
654
Magnetostatic Boundary Conditions
994
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
994
Theory of Metallic Conduction
1.4K
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,...
1.4K
Types Of Superconductors
1.0K
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...
1.0K
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


