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Supercurrent in ferromagnetic Josephson junctions with heavy metal interlayers. II. Canted magnetization

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arxiv 1904.08798 v2 pith:FPHCLY4E submitted 2019-04-18 cond-mat.supr-con

classification cond-mat.supr-con
keywords ferromagneticmagnetizationsupercurrentcantedcouplingjunctionsspin-orbitweak
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abstract

It has been suggested by theoretical works that equal spin-triplet Cooper pairs can be generated in Josephson junctions containing both a ferromagnet and a source of spin-orbit coupling. Our recent experimental work suggested that spin-triplet Cooper pairs were not generated by a Pt spin-orbit coupling layer when the ferromagnetic weak link had entirely in-plane anisotropy (N. Satchell and N.O. Birge, Phys. Rev. B 97, 214509 (2018)). Here, we revisit the experiment using Pt again as a source for spin-orbit coupling and a [Co(0.4 nm)/Ni(0.4 nm)]$_{\times8}$/Co(0.4 nm) ferromagnetic weak link with both in-plane and out-of-plane magnetization components (canted magnetization). The canted magnetization more closely matches theoretical predictions than our previous experimental work. Our results suggest that there is no supercurrent contribution in our junctions from equal spin-triplets. In addition, this work includes the first systematic study of supercurrent dependence on Cu interlayer thickness, a common additional layer used to buffer the growth of the ferromagnet and which for Co may significantly improve the growth morphology. We report that the supercurrent in the [Co(0.4 nm)/Ni(0.4 nm)]$_{\times8}$/Co(0.4 nm) ferromagnetic weak links can be enhanced by over two orders of magnitude by tuning the Cu interlayer thickness. This result has important application in superconducting spintronics, where large critical currents are desirable for devices.

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  1. Switchable Josephson current in junctions with spin-orbit coupling

    cond-mat.supr-con 2019-09 accept novelty 6.0 of 10

    The long-range triplet Josephson current in diffusive lateral junctions with spin-orbit coupling can be switched between 0 and pi states by rotating the exchange field or by tuning the Rashba or Dresselhaus coupling.

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