The Journal of Physical Chemistry C · 2010 · 93 citations · 47 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsPhysical ChemistrySurface ScienceChemical BondingElectronic StructureMetal-ligand BondingPhotoelectron SpectroscopySurface PhysicsSurface SpectroscopyCharge LocalizationElectronic Density Of StatesFermi LevelFermi SurfaceInterfacial Electronic StructureNear-edge X-ray Absorption Fine Structure SpectroscopyValence BandX-ray Absorption Near Edge Structure
Iron and cobalt phthalocyanines assemble on the Au(110) surface lying parallel to the surface, as deduced by near-edge X-ray absorption fine structure (NEXAFS) taken with linearly polarized radiation at the C and N K edges. The molecular chains, firmly anchored to the underlying metal surface, arrange into long-range ordered rows with a (5 × 3) symmetry along the [001] azimuthal direction at completion of the first single layer. The interaction process is mainly determined by the d orbitals associated with the central Fe and Co atoms, as observed by valence band photoemission and NEXAFS at the Fe and Co L 2,3 edges. The spin and orbital configuration of the FePc and CoPc molecules is strongly influenced by the interface with a charge transfer from the underlying metal to the out-of-plane empty states located at the Fe and Co centers of the molecules. This interaction process induces electronic states located at the interface, localized on the central metal atoms and close to the Fermi level (0.2 eV binding energy for FePc and 0.7 eV for CoPc) without energy dispersion, as deduced by angular-resolved photoemission. On the contrary, a delocalized state has been observed with dispersion along the molecular chains, mainly due to the overlapping of the π charge of the macrocycles ligands mediated by the Au substrate.
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Phthalocyanines. properties and applications
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