Abstract

Following the recent synthesis of graphene–based antiferromagnetic ultrathin heterostructures made of Co and Fe, we analyse the effect of the spacer between both ferromagnetic materials. Using density functional calculations, we carried out an exhaustive study of the geometric, electronic and magnetic properties for intercalated single Co MLs on top of Ir(111) coupled to monolayered Fe through n graphene layers (n = 1, 2, 3) or monolayered h-BN. Different local atomic arrangements have been considered to model the Moiré patterns expected in these heterostructures. The magnetic exchange interactions between both ferromagnets () are computed from explicit calculations of parallel and anti-parallel Fe/Co inter–layer alignments, and discussed in the context of recent experiments. Our analysis confirms that the robust antiferromagnetic superexchange–coupling between Fe and Co layers is mediated by the graphene spacer through the hybridization of C’s orbitals with Fe and Co’s 3d states. The hybridization is substantially suppressed for multilayered graphene spacers, for which the magnetic coupling between ferromagnets is critically reduced, suggesting the need for ultrathin (monolayer) spacers in the design of synthetic graphene-based antiferromagnets. In the case of h–BN, orbitals also mediate d(Fe/Co) coupling. However, there is a larger contribution of local ferromagnetic interactions. Magnetic anisotropy energies were also calculated using a fully relativistic description, and show out–of–plane easy axis for all the configurations, with remarkable net values in the range from 1 to 4 meV.

Highlights

  • Antiferromagnetic (AFM) materials have made an appearance in the field of spintronics, where are considered as components for key active elements, rather than playing a mere supporting role

  • Among the possible materials that exhibit antiferromagnetism, there is a growing interest in the so called synthetic antiferromagnets (SAF), which can be engineered by stacking thin films of magnetic and non-magnetic materials

  • The technology has been developed since the late 1980s, but the apperance of 2D materials, mostly graphene and h-BN and dichalcogenides, has opened new exciting opportunities in spintronics, for example in magnetic tunnel junctions (MTJ) [3]

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Summary

Introduction

Antiferromagnetic (AFM) materials have made an appearance in the field of spintronics, where are considered as components for key active elements, rather than playing a mere supporting role. The Moiré superlattice means that there is a variety of local stackings for the interfacial atoms, and each of them can give different magnetic interactions, modifying the picture that model calculations can give The objective of this manuscript is to present some guidelines for the design of new synthetic magnets based on 2D materials, advancing from previous theoretical works and following recent experimental developments in the literature. We extend a previous study where we established that ultra–thin synthetic Ir(111)/Co/Gr/Fe/ films exhibit robust perpendicular AFM superexchange–coupling between Fe and Co magnetic MLs [7] Such coupling takes place throughout direct interfacial hybridisation between (Fe/Co)–3dz and C–pz states.

Methodology
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Electronic Structure and Projected DOS
Magnetic Anisotropy Energies
Structural Optimisations
Findings
Conclusions
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