TY - JOUR
T1 - Andreev rectifier
T2 - A nonlocal conductance signature of topological phase transitions
AU - Rosdahl, T. O.
AU - Vuik, A.
AU - Kjaergaard, M.
AU - Akhmerov, A. R.
PY - 2018
Y1 - 2018
N2 - The proximity effect in hybrid superconductor-semiconductor structures, crucial for realizing Majorana edge modes, is complicated to control due to its dependence on many unknown microscopic parameters. In addition, defects can spoil the induced superconductivity locally in the proximitized system, which complicates measuring global properties with a local probe. We show how to use the nonlocal conductance between two spatially separated leads to probe three global properties of a proximitized system: the bulk superconducting gap, the induced gap, and the induced coherence length. Unlike local conductance spectroscopy, nonlocal conductance measurements distinguish between nontopological zero-energy modes localized around potential inhomogeneities, and true Majorana edge modes that emerge in the topological phase. In addition, we find that the nonlocal conductance is an odd function of bias at the topological phase transition, acting as a current rectifier in the low-bias limit. More generally, we identify conditions for crossed Andreev reflection to dominate the nonlocal conductance and show how to design a Cooper pair splitter in the open regime.
AB - The proximity effect in hybrid superconductor-semiconductor structures, crucial for realizing Majorana edge modes, is complicated to control due to its dependence on many unknown microscopic parameters. In addition, defects can spoil the induced superconductivity locally in the proximitized system, which complicates measuring global properties with a local probe. We show how to use the nonlocal conductance between two spatially separated leads to probe three global properties of a proximitized system: the bulk superconducting gap, the induced gap, and the induced coherence length. Unlike local conductance spectroscopy, nonlocal conductance measurements distinguish between nontopological zero-energy modes localized around potential inhomogeneities, and true Majorana edge modes that emerge in the topological phase. In addition, we find that the nonlocal conductance is an odd function of bias at the topological phase transition, acting as a current rectifier in the low-bias limit. More generally, we identify conditions for crossed Andreev reflection to dominate the nonlocal conductance and show how to design a Cooper pair splitter in the open regime.
UR - http://resolver.tudelft.nl/uuid:47c8939a-0b09-484b-9e34-c5f7bdeeecaf
UR - http://www.scopus.com/inward/record.url?scp=85041036861&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.97.045421
DO - 10.1103/PhysRevB.97.045421
M3 - Article
AN - SCOPUS:85041036861
SN - 2469-9950
VL - 97
JO - Physical Review B
JF - Physical Review B
IS - 4
M1 - 045421
ER -