Related Experiment Video
Updated: Aug 7, 2025

09:06
Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
8.2K
Inhomogeneous Superconductivity Onset in FeSe Studied by Transport Properties
Pavel D Grigoriev1,2,3, Vladislav D Kochev2, Andrey P Orlov4,5
1L.D. Landau Institute for Theoretical Physics, 142432 Chernogolovka, Russia.
Materials (Basel, Switzerland)
|March 11, 2023
Summary
Superconductivity in iron selenide (FeSe) shows a higher transition temperature (Tc) as sample thickness decreases. This study reveals insights into superconducting domain structure and size in thin FeSe films.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Superconductivity
Background:
- Heterogeneous superconductivity onset is typical in high-temperature superconductors.
- Superconductivity often initiates as isolated domains in anisotropic materials like FeSe.
- Transport measurements reveal SC domain structure and size.
Purpose of the Study:
- Investigate the impact of sample thickness on superconductivity in FeSe.
- Determine the aspect ratio and size of superconducting domains.
- Develop a method to estimate SC domain aspect ratio from Tc anisotropy.
Main Methods:
- Fabrication of FeSe mesa structures using focused ion beam (FIB) for interlayer resistivity measurements.
- Temperature-dependent measurement of both interlayer and intralayer resistivity.
- Analytical and numerical calculations to analyze experimental data.
Main Results:
- Superconducting transition temperature (Tc) increases from 8 K in bulk FeSe to 12 K in ~40 nm thick microbridges.
- SC domain aspect ratio and size are consistent with resistivity and diamagnetic response measurements.
- A method for estimating SC domain aspect ratio from Tc anisotropy in thin samples was proposed.
Conclusions:
- Sample thickness significantly influences the superconducting transition temperature in FeSe.
- The study provides a method for characterizing SC domains in anisotropic superconductors.
- Discusses the relationship between nematic and superconducting domains in FeSe.
Related Concept Videos
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
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
2.4K
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
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
Magnetic Susceptibility and Permeability
1.3K
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...
1.3K
Fermi Level
713
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,...
713

