TY - JOUR
T1 - Asymmetric Little–Parks oscillations in full shell double nanowires
AU - Vekris, Alexandros
AU - Estrada Saldaña, Juan Carlos
AU - de Bruijckere, Joeri
AU - Lorić , Sara
AU - Kanne, Thomas
AU - Marnauza, Mikelis
AU - Olsteins, Dags
AU - Nygård, Jesper
AU - Grove-Rasmussen, Kasper
PY - 2021
Y1 - 2021
N2 - Little–Parks oscillations of a hollow superconducting cylinder are of interest for flux-driven topological superconductivity in single Rashba nanowires. The oscillations are typically symmetric in the orientation of the applied magnetic flux. Using double InAs nanowires coated by an epitaxial superconducting Al shell which, despite the non-centro-symmetric geometry, behaves effectively as one hollow cylinder, we demonstrate that a small misalignment of the applied parallel field with respect to the axis of the nanowires can produce field-asymmetric Little–Parks oscillations. These are revealed by the simultaneous application of a magnetic field perpendicular to the misaligned parallel field direction. The asymmetry occurs in both the destructive regime, in which superconductivity is destroyed for half-integer quanta of flux through the shell, and in the non-destructive regime, where superconductivity is depressed but not fully destroyed at these flux values.
AB - Little–Parks oscillations of a hollow superconducting cylinder are of interest for flux-driven topological superconductivity in single Rashba nanowires. The oscillations are typically symmetric in the orientation of the applied magnetic flux. Using double InAs nanowires coated by an epitaxial superconducting Al shell which, despite the non-centro-symmetric geometry, behaves effectively as one hollow cylinder, we demonstrate that a small misalignment of the applied parallel field with respect to the axis of the nanowires can produce field-asymmetric Little–Parks oscillations. These are revealed by the simultaneous application of a magnetic field perpendicular to the misaligned parallel field direction. The asymmetry occurs in both the destructive regime, in which superconductivity is destroyed for half-integer quanta of flux through the shell, and in the non-destructive regime, where superconductivity is depressed but not fully destroyed at these flux values.
U2 - 10.1038/s41598-021-97780-9
DO - 10.1038/s41598-021-97780-9
M3 - Journal article
C2 - 34561484
VL - 11
JO - Scientific Reports
JF - Scientific Reports
SN - 2045-2322
M1 - 19034
ER -