Abstract

We present experimental data on Josephson effect in hybrid superconducting mesa-heterostructures (HSMH) with composite manganite-ruthenate interlayer. The HSMH base electrode consisted of the cuprate superconductor YBa2Cu3O7 grown epitaxially on a NdGaO substrate using laser ablation. The interlayer was composed from in-situ deposited SrRuO3 (F1) and La0.7Sr0.3MnO3 (F2) thin films, each characterized by different directions of magnetization. The top electrode was Nb/Au thin film. A superconducting current was observed when the interlayer thickness was well above the correlation length, determined by the exchange field in F1 and F2. Obtained IC(H) dependences and non-sinusoidal current-phase relation evaluated from microwave measurements are discussed in terms of generation of long-range spin triplet superconducting current component in heterostructures with interfaces of singlet superconductors and bilayer ferromagnetic materials with different spatial directions of magnetization.

Highlights

  • In superconducting heterostructures with a non-uniform magnetized ferromagnetic layer (F) between two singlet superconductors (S) a long-range triplet superconducting correlations may occur [1]

  • The superconducting current was observed in all hybrid superconducting mesa-heterostructures (HSMH) with a total thickness d of the composite Minterlayer up to 53 nm, which is much larger than the coherence lengths in F1 and F2, determined by the exchange field

  • Control measurements of the HSMH with only the LSMO [16] or the SRO interlayer, showed [22] that the critical current is absent if the SRO and LSMO films are thicker than d1=14 nm and d2=2 nm, respectively

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Summary

Introduction

In superconducting heterostructures with a non-uniform magnetized ferromagnetic layer (F) between two singlet superconductors (S) a long-range triplet superconducting correlations may occur [1]. 3. Results and discussion The superconducting current was observed in all HSMH with a total thickness d of the composite Minterlayer up to 53 nm, which is much larger than the coherence lengths in F1 and F2, determined by the exchange field.

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