Abstract

We study new types of Josephson junctions composed of helical p-wave superconductors with and -pairing symmetries using quasi-classical Green’s functions with generalized Riccati parametrization. The junctions can host rich ground states: π phase, 0 + π phase, φ0 phase and φ phase. The phase transition can be tuned by rotating the magnetization in the ferromagnetic interface. We present the phase diagrams in the parameter space formed by the orientation of the magnetization or by the magnitude of the interfacial potentials. The selection rules for the lowest order current which are responsible for the formation of the rich phases are summarized from the current-phase relations based on the numerical calculation. We construct a Ginzburg–Landau type of free energy for the junctions with d-vectors and the magnetization, which not only reveals the interaction forms of spin-triplet superconductivity and ferromagnetism, but can also directly lead to the selection rules. In addition, the energies of the Andreev bound states and the novel symmetries in the current-phase relations are also investigated. Our results are helpful both in the prediction of novel Josephson phases and in the design of quantum circuits.

Highlights

  • Josephson junctions have been subjected to continuously growing interests because of rich ground states in these systems and their potential applications in superconducting electronics [1,2,3,4,5]

  • We propose a concise scheme to realize rich ground states in Josephson junctions consisting of helical p-wave superconductors (HPSs) with paring symmetries kxx ± kyyand kyx ± kxyand a ferromagnet (F)

  • Various current-phase relations (CPRs) are found in the junctions due to the interfacial potential-dependent current which lead to rich phase diagrams

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Summary

Introduction

Josephson junctions have been subjected to continuously growing interests because of rich ground states in these systems and their potential applications in superconducting electronics [1,2,3,4,5]. The interface which is a ferromagnetic barrier or of spin-orbit coupling can lead to the Josephson current proportional to cos φ when the triplet superconductor is in the chiral p-wave state [26,27]. The dependence of CPRs on the magnetization in the barrier can bring different phases in spin-triplet Josephson junctions with p-wave paring. We propose a concise scheme to realize rich ground states in Josephson junctions consisting of helical p-wave superconductors (HPSs) with paring symmetries kxx ± kyyand kyx ± kxyand a ferromagnet (F). In order to explain the rules, we construct a Ginzburg-Landau type of free energy of the junctions with d-vectors in HPS and the magnetization in F, which reveals the interaction mechanism between the helical p-wave superconductivity and ferromagnetism.

Quasiclassical Green’s function formalism
Results and discussion
Free energy and selection rules
Conclusions

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