Related Experiment Video
Updated: Dec 8, 2025

04:51
Comparison of Two Different Synthesis Methods of Single Crystals of Superconducting Uranium Ditelluride
Published on: July 8, 2021
3.1K
Spin-Orbit-Parity-Coupled Superconductivity in Topological Monolayer WTe_{2}
Ying-Ming Xie1, Benjamin T Zhou1, K T Law1
1Department of Physics, Hong Kong University of Science and Technology, Clear Water Bay, 999077 Hong Kong, China.
Physical Review Letters
|September 21, 2020
Summary
Superconductivity in 1T^{
Area of Science:
- Condensed Matter Physics
- Materials Science
Background:
- Monolayer 1T^{'}-WTe_{2} exhibits gate-induced superconductivity and is a topological insulator.
- Observed upper critical field (B_{c2}) exceeds the Pauli paramagnetic limit (B_{p}), unexplained by conventional spin-orbit coupling.
- Inversion symmetry in centrosymmetric 1T^{'}-WTe_{2} complicates standard explanations for enhanced critical fields.
Purpose of the Study:
- To elucidate the distinctive superconducting properties of centrosymmetric 1T^{'}-WTe_{2}.
- To explain the enhanced upper critical field beyond the Pauli limit.
- To investigate the role of spin-orbit-parity coupling (SOPC) in superconductivity.
Main Methods:
- Theoretical investigation of superconducting properties in centrosymmetric 1T^{'}-WTe_{2}.
- Analysis of the interplay between spin, momentum, and band parity degrees of freedom.
- Exploration of the impact of spin-orbit-parity coupling on superconducting transitions and critical fields.
Main Results:
- A first-order superconductor-metal transition at B_{c2}, significantly above B_{p}, is predicted.
- Anisotropic spin susceptibility and potential for anisotropic B_{c2} due to SOPC.
- Strong gate dependence of B_{c2} linked to SOPC's significance near topological band crossings.
Conclusions:
- Spin-orbit-parity coupling is identified as the mechanism behind the enhanced B_{c2} in 1T^{'}-WTe_{2}.
- SOPC influences the superconducting transition order and critical field anisotropy.
- The theoretical framework is applicable to other centrosymmetric materials with topological band inversions.
Related Concept Videos
The Pauli Exclusion Principle
58.0K
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
58.0K
Types Of Superconductors
1.5K
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...
1.5K
Superconductor
1.6K
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...
1.6K
Spin–Spin Coupling: One-Bond Coupling
1.3K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.3K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
1.4K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.4K
Atomic Nuclei: Nuclear Spin State Overview
1.6K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
1.6K

