Observation of surface superconductivity in a three-dimensional Dirac material
arXiv:2206.03405 · doi:10.1002/adfm.202208616
Abstract
Superconductivity becomes more interesting when it encounters dimensional constraint or topology, because it is of importance for exploring exotic quantum phenomena or developing superconducting electronics. Here we report the coexistence of naturally formed surface superconducting state and three-dimensional topological Dirac state in single crystals of BaMgBi. The electronic structure obtained from the first-principles calculations demonstrates that BaMgBi is an ideal Dirac material, in which the Dirac point is very close to the Fermi level and no other energy band crosses the Fermi level. Superconductivity up to 4.77 K can be observed under ambient pressure in the measurements of resistivity. The angle dependent magnetoresistance reveals the two-dimensional characteristic of superconductivity, indicating that superconductivity occurs on the surface of the sample and is absent in the bulk state. Our study not only provides BaMgBi as a suitable platform to study the interplay between superconductivity and topological Dirac state, but also indicates that MgBi-based materials may be a promising system for exploring new superconductors.
References in corpus (6)
- Superconducting proximity effect and Majorana fermions at the surface of a topological insulator
- Superconductivity in single-layer films of FeSe with a transition temperature above 100 K
- Highly crystalline 2D superconductors
- Two-dimensional superconductivity at the surfaces of KTaO3 gated with ionic liquid
- Tip induced unconventional superconductivity on Weyl semimetal TaAs
- Quasi 1D topological nodal vortex line phase in doped superconducting 3D Dirac Semimetals
Cited by in corpus (5)
- Atomic Visualization of Bulk and Surface Superconductivity in Weyl Semimetal γ-PtBi2
- Uncovering surface states of the Dirac semimetal BaMg2Bi2
- Emergence of Double-Dome Superconductivity in the Pressurized Dirac Semimetal BaMg2Bi2
- Surface Functional Renormalization Group for Layered Quantum Materials
- Topological materials with extensive flat-band surface states