Related Experiment Video
Updated: Jul 1, 2025

09:25
Fabricating van der Waals Heterostructures with Precise Rotational Alignment
Published on: July 5, 2019
9.5K
Superconductivity in a van der Waals layered quasicrystal
Yuki Tokumoto1, Kotaro Hamano2, Sunao Nakagawa2
1Institute of Industrial Science, The University of Tokyo, Tokyo, 153-8505, Japan. tokumoto@iis.u-tokyo.ac.jp.
Nature Communications
|March 1, 2024
Summary
Superconductivity was discovered in a novel van der Waals layered quasicrystal of Ta1.6Te. This finding opens new avenues for exploring physical properties of quasicrystals and advancing superconductivity research.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Solid-State Chemistry
Background:
- Van der Waals layered transition-metal chalcogenides exhibit unique physical properties.
- These materials are typically crystalline, with limited study on their quasicrystalline counterparts.
- The physical properties of van der Waals layered quasicrystals remain largely unexplored.
Purpose of the Study:
- To investigate the physical properties of van der Waals layered quasicrystals.
- To report the discovery of superconductivity in a novel van der Waals layered quasicrystal.
Main Methods:
- Synthesis and characterization of Ta1.6Te quasicrystal.
- Measurement of electrical resistivity.
- Analysis of magnetic susceptibility.
- Specific heat measurements.
Main Results:
- Discovery of bulk superconductivity in Ta1.6Te van der Waals layered quasicrystal.
- Superconducting transition temperature (Tc) observed at approximately 1 Kelvin.
- Unambiguous validation of superconductivity through multiple physical property measurements.
Conclusions:
- Superconductivity is demonstrated in a van der Waals layered quasicrystal for the first time.
- This discovery encourages research into novel van der Waals layered quasicrystals and 2D quasicrystals.
- It opens new possibilities for superconductivity in thermodynamically stable quasicrystal systems.
Related Concept Videos
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
Types Of Superconductors
979
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...
979
Metallic Solids
18.4K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
18.4K
Network Covalent Solids
13.5K
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
13.5K
Theory of Metallic Conduction
1.3K
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,...
1.3K
Van der Waals Interactions
63.9K
Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
63.9K

