相关实验视频
Updated: Jul 2, 2025

06:53
Scanning SQUID Study of Vortex Manipulation by Local Contact
Published on: February 1, 2017
6.8K
在多频段CsV3Sb5衍生的kagome超导体中可调节的旋束状态
Zihao Huang1, Xianghe Han1, Zhen Zhao1
1Beijing National Center for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100190, China.
Science bulletin
|February 21, 2024
概括
研究人员在kagome超导体中调整了束状态 (VBSs) Cs(V$_{1-x}$Tr$_{x}$) $_{3}$Sb$_{5}$ (Tr = Ta,Ti). 兴奋剂CsV_{3}$Sb_{5}$揭示了不同的VBS行为,为超导电子特性提供了洞察力.
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
- 超导电性 超导电性 超导电性
背景情况:
- 和束状态对于理解超导体电子特性至关重要.
- 最近,在CsV_{3}$Sb_{5}$这样的kagome超导体中观察到表面依赖的旋核心状态.
- 这些材料中尖的零能量导电性峰值的起源,可能是Majorana绑定状态,尚未完全理解.
研究的目的:
- 为了研究可调节的束状态 (VBSs) 在化学合的kagome超导体 Cs(V$_{1-x}$Tr$_{x}$) $_{3}$Sb$_{5}$ (Tr = Ta,Ti).
- 探索兴奋剂对CsV_{3}$Sb_{5}$衍生材料中的超导和电荷顺序的影响.
- 阐明这些系统中零偏差导电性峰值 (ZBCPs) 的性质.
主要方法:
- 使用了低温扫描道显微镜/光谱 (STM/STS).
- 用 (Ta) 和 (Ti) 进行化学兴奋剂对 CsV$_{3}$Sb$_{5}$进行.
- 对状格子重定向和导电性峰值的空间分布的分析.
主要成果:
- 杂的Cs{(V$_{1-x}$Tr$_{x}$) $_{3}$Sb$_{5}$超导体表现出完全的间隙配对,并且缺乏远程充电顺序.
- 陶化样本显示了传统的卡罗利-德热内斯-马特里克 (CdGM) 束状态与十字形空间演变.
- Ti-doped样本显示了一个强大的,非分裂的零偏差导电性峰值 (ZBCP),在中持续存在,取决于兴奋剂度.
结论:
- 在化学杂的多频段CSV系统中观察到可调节的VBS.
- 该研究提供了关于ZBCP在kagome超导体中的起源的见解,将其与表面效应区分开来.
- 这些发现有助于理解新型超导材料中复杂的电子状态.
相关概念视频
Types Of Superconductors
980
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...
980
Magnetostatic Boundary Conditions
933
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...
933
Spin–Spin Coupling Constant: Overview
923
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
923
Superconductor
1.1K
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...
1.1K
Magnetic Field due to Moving Charges
8.7K
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...
8.7K
Standing Waves in a Cavity
920
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
920

