We show that graphene can be magnetized by coupling to a ferromagnetic Co film through a
Au monolayer. The presence of dislocation loops under graphene leads to a ferrimagnetic …

Au (001) surfaces exhibit a complex reconstructed structure [Hex− Au (001)] comprising a
hexagonal surface and square bulk lattices, yielding a quasi-one-dimensional corrugated …

Metal intercalation under graphene has attracted extensive experimental and theoretical
research because of its capability to manipulate the electronic structure and properties of …

Compared to monolayer graphene, electrons in Bernal-stacked bilayer graphene (BLG)
have an additional layer degree of freedom, offering a platform for developing layered …

We introduce apz-d coupling model Hamiltonian for the π-graphene/Au bands that predicts
a rather large intrinsic spin-orbit (SO) coupling as is being reported in recent experiments …

The proximity-induced effects of the nearly commensurate lattice structure of a graphene
layer AC stacked on Ni (111) and Co (0001) substrates are addressed. To this end, a …

We investigate collective spin excitations in graphene with proximity-induced spin-orbit
coupling (SOC) of the Rashba and valley-Zeeman types, as it is the case, eg, for graphene …

In 2010, the quantum anomalous Hall effect (QAHE) in graphene was proposed in the
presence of Rashba spin-orbit coupling and a ferromagnetic exchange field. After a decade …

Intercalation of noble metals can produce giant Rashba-type spin–orbit splittings in
graphene. The spin–orbit splitting of more than 100 meV has yet to be achieved in graphene …

Inversion symmetry in bilayer graphene allows for layered opposite Rashba spin-orbit
coupling (LO-RSOC)—the situation when the RSOC has the same magnitude but the …