2012/08/31 by Xiaoming Cai, Li-Jun Lang, Shu Chen +1 · 5 citations
Mathematics · Physics and Astronomy · #Advanced Condensed Matter Physics #Condensed matter physics #Fermion #Invariant (physics) #MAJORANA #Mathematics #Phase (matter) #Phase transition #Physics #Quantum #Quantum many-body systems #Quantum mechanics #Superconductivity #Topological Materials and Phenomena #Topological order #Topology (electrical circuits) #cond-mat.dis-nn #cond-mat.str-el
paper · pdf · doi:10.1103/physrevlett.110.176403
published as Phys. Rev. Lett. 110, 176403 (2013) · 5 + 4 pages, 5 +2 figures, version appeared in PRL, supplementary material included
openalex publication_date 2013/04/26 · arxiv created 2013/05/01 · arxiv updated 2015/03/20 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We study the competition of disorder and superconductivity for a one-dimensional p-wave superconductor in incommensurate potentials. With the increase in the strength of the incommensurate potential, the system undergoes a transition from a topological superconducting phase to a topologically trivial localized phase. The phase boundary is determined both numerically and analytically from various aspects and the topological superconducting phase is characterized by the presence of Majorana edge fermions in the system with open boundary conditions. We also calculate the topological Z2 invariant of the bulk system and find it can be used to distinguish the different topological phases even for a disordered system.