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Spin-triplet supercurrent in Josephson junctions containing a synthetic antiferromagnet with perpendicular magnetic anisotropy

Published 19 Oct 2017 in cond-mat.supr-con | (1710.07247v1)

Abstract: We present measurements of Josephson junctions containing three magnetic layers with noncolinear magnetizations. The junctions are of the form S/F<sup>′/N/F/N/F<sup>′</sup></sup>′/SS/F<sup>{\prime}/N/F/N/F<sup>{\prime</sup></sup> \prime}/S, where SS is superconducting Nb, F<sup>′F<sup>\prime is either a thin Ni or Permalloy layer with in-plane magnetization, NN is the normal metal Cu, FF is a synthetic antiferromagnet (SAF) with magnetization perpendicular to the plane, composed of Pd/Co multilayers on either side of a thin Ru spacer, and F<sup>′</sup>′F<sup>{\prime</sup> \prime} is a thin Ni layer with in-plane magnetization. The supercurrent in these junctions decays more slowly as a function of the FF-layer thickness than for similar spin-singlet junctions not containing the F<sup>′F<sup>\prime and F<sup>′</sup>′F<sup>{\prime</sup> \prime} layers. The slower decay is the prime signature that the supercurrent in the central part of these junctions is carried by spin-triplet pairs. The junctions containing F<sup>′=F<sup>{\prime}= Permalloy are suitable for future experiments where either the amplitude of the critical current or the ground-state phase difference across the junction is controlled by changing the relative orientations of the magnetizations of the F<sup>′F<sup>{\prime} and F<sup>′</sup>′F<sup>{\prime</sup> \prime} layers.

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