Abstract

We theoretically present an anomalous zero bias conductance peak (ZBCP) in graphene junctions with proximity-induced ferromagnetism and d-wave anisotropic superconducting pair symmetry (ASPS) herein. It is revealed that in the thin insulator limit, the ZBCP can be periodically recovered by adjusting the sandwiched insulating barrier strength χ regardless of exchange field h and the phase of the periodical behaviours for h larger than its Fermi energy EF (h > EF) is exactly opposite to that for h < EF. Most interestingly, in the context of h > EF, the periodic oscillation of the nonzero bias conductance located in the ZBCP versus χ, is accompanied by an explicit splitting peak. Moreover, under the situation of the insulator with finite width, the conductance exhibits a stronger damping oscillation with bias voltage eV for any h, which is also accompanied by a splitting ZBCP at h > EF. These singular features originate from ferromagnetic-modulated midgap states characteristic by the relativistic nodal fermions, which confirms the spin polarization and ASPS of the graphene, and thus will be of great interest in the designing and fabrication of graphene superconducting spintronic devices.

Highlights

  • In Particular under the case of h > EF, the periodic oscillation of the nonzero bias conductance located in the zero bias conductance peak (ZBCP) versus χ, is accompanied by an explicit splitting peak

  • The previous studies of graphene F/I/S junctions were focused on the zero-bias conductance oscillations,26–29 but here we present how the exchange field h exerts an influence on the oscillation of the whole ZBCP conductance located in the ZBCP for the graphene junctions with anisotropic d-wave superconducting pair symmetry

  • The amplitude of the pair potential disappears for α = π/4, in this context, the d-wave pair symmetry could lead to a sizable areal density of midgap states,33 which is the origin of the ZBCP observed in most high-Tc S junctions

Read more

Summary

INTRODUCTION

The so-called Kleinlike tunneling of Andreev electron-hole pairs, which carry superconducting correlations from high-Tc S YBa2Cu3O7−δ (YBCO) into graphene, was experimentally observed very recently, showing the high-Tc superconducting proximity effect in graphene.13 This confirms the conductance oscillations of a normal metal (N)/insulator (I)/d-wave S graphene junction due to the Klein tunneling.. For an incident spin-σ electron at x = 0 from the FM at an angle ασ with energy E, the wave functions in the different regions can be constructed from the linear combination of corresponding eigenfunctions, which are given by ΨF(x) = ΨFeσ+ + rNσ ΨFeσ− + rAσ ΨFhσ− ̄.

Thin I barrier limit
The effect of the finite width of the insulating region
SUMMARY
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.