拓学物质. 拓学物质. 在超导体上的铁磁原子链中观察Majorana子
Stevan Nadj-Perge1, Ilya K Drozdov1, Jian Li1
1Joseph Henry Laboratories and Department of Physics, Princeton University, Princeton, NJ 08544, USA.
概括
研究人员在 (Pb) 上创建了铁 (Fe) 原子链,以实现一维的拓超导体. 他们观察到Majorana铁子的证据,这些系统的边缘预计存在着异国情调的粒子.
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
- 量子物理学 量子物理学 是一种量子物理学.
背景情况:
- 拓超导体在其边缘承载着奇特的准粒子,如马约拉纳费米子.
- 这些系统对于推动量子计算和基本物理学的发展至关重要.
- 制造一维拓超导体仍然是一个重大挑战.
研究的目的:
- 实现一个一维的拓超导体.
- 为了调查工程原子链中Majorana费米子的存在.
主要方法:
- 在超导 (Pb) 基板上制造铁磁铁 (Fe) 原子链.
- 使用高分辨率光谱成像技术来探测电子属性.
- 分析状态的电子密度,并识别独特的光谱特征.
主要成果:
- 在大部分Fe原子链中诱导了超导.
- 观察到,在链条边缘出现了零能量终端状态.
- 这些终点状态为拓相形成提供了有力的证据.
结论:
- 实验设置成功地为拓超导体创造了条件.
- 检测到边缘绑定的Majorana费米子,证实了理论预测.
- 这项工作为新型量子电子设备铺平了道路.
相关概念视频
Ferromagnetism
2.8K
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...
2.8K
Types Of Superconductors
1.6K
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...
1.6K
Superconductor
1.9K
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...
1.9K
Theory of Metallic Conduction
1.9K
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,...
1.9K
Atomic Nuclei: Magnetic Resonance
1.2K
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
1.2K
Atomic Nuclei: Nuclear Relaxation Processes
1.1K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.1K


