Abstract
InxSn1−xTe is a time-reversal invariant candidate 3D topological superconductor derived from doping the topological crystalline insulator SnTe with indium. The ability to synthesize low-dimensional nanostructures of indium-doped SnTe is key for realizing the promise they hold in future spintronic and quantum information processing applications. But hitherto only bulk synthesized crystals and nanoplates have been used to study the superconducting properties. Here for the first time we synthesize InxSn1−xTe nanostructures including nanowires and nanoribbons, which show superconducting transitions. In some of the lower dimensional morphologies, we observe signs of more than one superconducting transition and the absence of complete superconductivity. We propose that material inhomogeneity, such as indium inhomogeneity and possible impurities from the metal catalyst, is amplified in the transport characteristics of the smaller nanostructures and is responsible for this mixed behavior. Our work represents the first demonstration of InxSn1−xTe nanowires with the onset of superconductivity, and points to the need for improving the material quality for future applications.
Highlights
Topological insulators (TIs)[1,2] and topological crystalline insulators[3] (TCIs) are unique states of matter with an insulating bulk and gapless surface states (SS) that are chiral and massless
Similar to TIs, topological superconductor (TSC) are time-reversal invariant and are predicted to host emergent Majorana states,[7] which are a crucial ingredient for fault tolerant quantum computing.[8]
Superconducting transition temperatures (T c) of ∼1.4-1.75 K are observed in our nanoribbons and nanowires
Summary
Topological insulators (TIs)[1,2] and topological crystalline insulators[3] (TCIs) are unique states of matter with an insulating bulk and gapless surface states (SS) that are chiral and massless. Superconducting transition temperatures (T c) of ∼1.4-1.75 K are observed in our nanoribbons and nanowires. We find that the superconducting transition varies between nanoplates, nanoribbons, and nanowires.
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