2013/03/31 by Dibyendu Roy, Nilanjan Bondyopadhaya, Sumanta Tewari · 7 citations
Physics and Astronomy · #Advanced Condensed Matter Physics #Condensed matter physics #Conductance #Dirac fermion #Fermion #MAJORANA #Magnetic field #Majorana fermion #Physics #Quantum and electron transport phenomena #Quantum mechanics #Superconductivity #Topological Materials and Phenomena #Zeeman effect #cond-mat.mes-hall #cond-mat.supr-con
paper · pdf · doi:10.1103/physrevb.88.020502
published as Phys. Rev. B 88, 020502(R) (2013)
openalex publication_date 2013/07/08 · arxiv created 2013/07/15 · arxiv updated 2015/06/15 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
We show that a topologically trivial zero-bias conductance peak is produced in semiconductor-superconductor hybrid structures due to a suppressed superconducting pair potential and/or an excess Zeeman field at the ends of the heterostructure, both of which can occur in experiments. The zero-bias peak (ZBP) (a) appears above a threshold parallel bulk Zeeman field, (b) is stable for a range of bulk field before splitting, (c) disappears with rotation of the bulk Zeeman field, and (d) is robust to weak disorder fluctuations. The topologically trivial ZBPs are also expected to produce splitting oscillations with the applied field similar to those from Majorana fermions. Because of such strong similarity with the phenomenology expected from Majorana fermions, we find that the only unambiguous way to distinguish these trivial ZBPs (of height 4e2/h) from those arising from Majorana fermions (of height 2e2/h) is by comparing the (zero-temperature) peak height and/or through an interference experiment.