Abstract
Topological superconductors are an intriguing and elusive quantum phase, characterized by topologically protected gapless surface/edge states residing in a bulk superconducting gap, which hosts Majorana fermions. Unfortunately, all currently known topological superconductors have a very low transition temperature, limiting experimental measurements of Majorana fermions. Here we discover the existence of a topological Dirac–nodal-line state in a well-known conventional high-temperature superconductor, MgB2. First-principles calculations show that the Dirac–nodal-line structure exhibits a unique one-dimensional dispersive Dirac–nodal line, protected by both spatial-inversion and time-reversal symmetry, which connects the electron and hole Dirac states. Most importantly, we show that the topological superconducting phase can be realized with a conventional s-wave superconducting gap, evidenced by the topological edge mode of the MgB2 thin films showing chiral edge states. Our discovery may enable the experimental measurement of Majorana fermions at high temperature.
Highlights
Superconducting and topological states are among the most fascinating quantum phenomena in nature
The first way to realize a topological superconductors (TSCs) phase is by the proximity effect via formation of a heterojunction between a topological material and a superconductor (SC).[1,2,3]
TSCs can be made by realizing superconductivity in a topological material[5,6,7,8,9,10,11] or by identifying the topological phase in a superconductor.[12,13,14,15]
Summary
Superconducting and topological states are among the most fascinating quantum phenomena in nature. Based on first-principles calculations, we demonstrate a topological Dirac nodal line (DNL)[16,17,18] structure in MgB2, exhibiting a unique combination of topological and superconducting properties.
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