在高温超导体中,超导性和反铁磁性不能混合
I Bozovic1, G Logvenov, M A J Verhoeven
1Oxxel GmbH, Technologiepark Universitaet, Bremen 28359, Germany. ibozovic@pacbell.net
Nature
|April 25, 2003
概括
高温超导理论受到挑战:抗铁磁和超导状态不混合,即使在薄层中. 兴奋剂似乎在带隙内创造了新的电子状态.
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
- 量子力学就是量子力学.
背景情况:
- 高温超导理论通常将其与反铁磁联系起来.
- 一个常见的假设是,兴奋剂会在母化合物的价值带中产生洞,从而导致超导.
- 这些模型预测由于类似的能量状态,反铁磁和超导相混合.
研究的目的:
- 研究超薄材料层中反铁磁性和超导性之间的关系.
- 为了测试高温超导的现有模型.
- 为了确定反铁磁和超导相是否在纳米尺度上混合.
主要方法:
- 制造一个单元细胞厚的La2CuO4 (抗铁磁) 和La1.85Sr0.15CuO4 (超导) 层.
- 测量超电流通过La2CuO4屏障的流量.
- 描述La1.85Sr0.15CuO4层的超导性能.
主要成果:
- 抗铁磁La2CuO4层仍然具有绝缘性,并完全阻断超电流,衰变长度为1 Å.
- 超导的La1.85Sr0.15CuO4层单独表现出超导性.
- 这些发现表明,在这种尺度上,反铁磁和超导之间缺乏相位混合.
结论:
- 实验结果与目前大多数关于高温超导的理论相矛盾.
- 缺少相位混合表明,反铁磁性和超导性可能比以前认为的更明显.
- 兴奋剂可能会在带隙内诱导新的电子状态,而不是简单地在价值带中创建洞.
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
04:51Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
Published on: July 8, 2021
相关概念视频
Superconductor
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...
Types Of Superconductors
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...
Ferromagnetism
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...
Paramagnetism
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...
Theory of Metallic Conduction
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,...
Magnetostatic Boundary Conditions
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...
