Theoretical prediction of perfect spin filtering at interfaces between close-packed surfaces of Ni or Co and graphite or graphene

TL;DR

This paper predicts perfect spin filtering at interfaces between graphite or graphene and Ni or Co surfaces due to lattice matching and electronic structure overlap, with robustness to interface imperfections, and proposes a method to preserve graphene's electronic properties.

Contribution

It introduces a theoretical prediction of perfect spin filtering at specific metal-graphite interfaces and demonstrates how to maintain graphene's electronic structure using Cu dusting.

Findings

Perfect spin filtering predicted at Ni/Co and graphite interfaces.

Spin filtering is robust against interface roughness and disorder.

Graphene's electronic structure can be preserved with Cu dusting.

Abstract

The in-plane lattice constants of close-packed planes of fcc and hcp Ni and Co match that of graphite almost perfectly so that they share a common two dimensional reciprocal space. Their electronic structures are such that they overlap in this reciprocal space for one spin direction only allowing us to predict perfect spin filtering for interfaces between graphite and (111) fcc or (0001) hcp Ni or Co. First-principles calculations of the scattering matrix show that the spin filtering is quite insensitive to amounts of interface roughness and disorder which drastically influence the spin-filtering properties of conventional magnetic tunnel junctions or interfaces between transition metals and semiconductors. When a single graphene sheet is adsorbed on these open $d$-shell transition metal surfaces, its characteristic electronic structure, with topological singularities at the K points in the two dimensional Brillouin zone, is destroyed by the chemical bonding. Because graphene bonds only weakly to Cu which has no states at the Fermi energy at the K point for either spin, the electronic structure of graphene can be restored by dusting Ni or Co with one or a few monolayers of Cu while still preserving the ideal spin injection property.