The shape dependency of two-dimensional magnetic field dependence of a Josephson junction

Abstract

Modulation characteristics of a Josephson current are usually measured by applying the external magnetic field parallel to the junction plane from one direction, and uniformity in tunnel barrier is discussed. So far, we have measured two-dimensional magnetic field dependence of a square Josephson junction by independently scanning the magnetic field (Hx,Hy) parallel to the junction plane from two directions. We can get a lot of information about spatial critical current distribution in a Josephson junction by observing the magnetic field dependence of a Josephson junction in two dimensions. This time, we have fabricated the different-shaped Josephson junctions and investigated the shape dependency of two-dimensional magnetic field dependence of a Josephson junction. We observed the Ic-(Hx,Hy) characteristics of triangular, hexagonal, and circular Josephson junctions quite different from the Ic-(Hx,Hy), characteristics of a square Josephson junction. Furthermore, we simulated two-dimensional magnetic field dependence of a Josephson junction by calculating the superconducting current density distribution in each magnetic field. The simulation results agreed well with experimental results.

The field-free Josephson diode in a van der Waals heterostructure

“…In addition, from the theory, the ideal Fraunhofer pattern requires a uniform current profile (rectangular junction area shape and magnetic field parallel with either side of the rectangle). Therefore, the junction shape and magnetic field direction can also lead to a non-ideal Fraunhofer pattern, even in a high-quality junction with high-quality interfaces 44 .…”

Two-dimensional magnetic field dependence of Josephson current and resonant current steps at finite voltage of square shape superconducting tunnel junctions

“…7 We have also obtained the I c -H (H x , H y ) characteristics by two dimensional (2-D) scanning of the external magnetic field H using two pairs of the Helmholtz coils. [8][9][10][11][12] In the I c -H (H x , H y ) dependence of square shape junction, sub peaks were observed in the directions of 0 , 90 , 180 , 270 in the H x ÀH y plane. 8 In triangle and hexagonal shape junctions, sub peaks were observed in the directions of 0 , 60 120 , 180 , 240 , 300 in the H x ÀH y plane.…”