Photoemission, from core levels and valence band, and low-energy electron diffraction (LEED) have been employed to investigate the electronic and structural properties of novel graphene-ferromagnetic (G-FM) systems,\ud
obtained by intercalation of one mono-layer (1ML) and several layers (4ML) of Co on G grown on Ir(111).\ud
Upon intercalation of 1ML of Co, the Co lattice is resized to match the Ir-Ir lattice parameter, resulting in a\ud
mismatched G/Co/Ir(111) system. The intercalation of further Co layers leads to a relaxation of the Co lattice\ud
and a progressive formation of a commensurate G layer lying on top. We show the C 1s line shape and the band\ud
structure of G in the two artificial phases, mismatched and commensurate G/Co, through a comparison with the\ud
electronic structure of G grown directly on a Co thick film. Our results show that while the G valence band\ud
mainly reflects the hybridization with the d states of Co, regardless of the structural phase, the C 1s line shape\ud
is very sensitive to the rumpling of the G layer and the coordination of carbon atoms with the underlying Co.\ud
Even in the commensurate (1x1) G/Co phase, where graphene is in register with the Co film, from the angular\ud
dependence of the C 1s core level we infer the presence of a double component, due to in-equivalent adsorption\ud
sites of carbon sub-lattices
Topological insulators are a promising class of materials for applications in the field of spintronics. New perspectives in this field can arise from interfacing metal-organic molecules with the topological insulator spin-momentum locked surface states, which can be perturbed enhancing or suppressing spintronics-relevant properties such as spin coherence. Here we show results from an angle-resolved photemission spectroscopy (ARPES) and scanning tunnelling microscopy (STM) study of the prototypical cobalt phthalocyanine (CoPc)/Bi2Se3 interface. We demonstrate that that the hybrid interface can act on the topological protection of the surface and bury the Dirac cone below the first quintuple layer.
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