2018/04/09 by C. Moore, Christopher Hudson Moore, Chuanchang Zeng +3 · 204 citations
Mathematics · Physics and Astronomy · #Advanced Condensed Matter Physics #Bound state #Charge (physics) #Condensed matter physics #Conductance #Heterojunction #MAJORANA #Mathematics #Physics #Plateau (mathematics) #Quantum #Quantum many-body systems #Quantum mechanics #Quantum tunnelling #Superconductivity #Topological Materials and Phenomena #Topology (electrical circuits) #cond-mat.mes-hall
paper · pdf · doi:10.1103/physrevb.98.155314
published in Physical review. B./Physical review. B 98(15) (American Physical Society) · 8 pages, 8 figures
arxiv created 2018/04/09 · openalex created_date 2018/04/24 · openalex publication_date 2018/10/19 · arxiv updated 2018/10/24 · openalex updated_date 2026/08/06
Recent observations of robust zero-bias quantized conductance plateaus of height 2e2/h in quantum dot-semiconductor-superconductor nanowire heterostructures have been interpreted as clear evidence for the presence of non-Abelian topologically protected Majorana zero modes (MZMs), since other sources of low-energy conductance are believed to be unable to produce such quantized plateaus. Based on extensive numerical calculations, we show that, in fact, quantized conductance plateaus of height 2e2/h can also arise as a result of partially separated Andreev bound states (ps-ABSs), in which the component Majorana bound states are somewhat shifted in space without being topological MZMs. As ps-ABSs can form rather generically in the topologically trivial phase, even in the absence of disorder, our results conclusively establish that the observation of quantized conductance plateaus of height 2e2/h does not represent sufficient evidence for the existence of topologically protected MZMs localized at the opposite ends of a wire.