Besides active, functional molecular building blocks such as diodes or switches, passive components as, e.g., molecular wires, are required to realize molecular-scale electronics. Incorporating metal centers in the molecular backbone enables the molecular energy levels to be tuned in respect to the Fermi energy of the electrodes. Furthermore, by using more than one metal center and sp-bridging ligands, a strongly delocalized electron system is formed between these metallic "dopants", facilitating transport along the molecular backbone. Here, we study the influence of molecule-metal coupling on charge transport of dinuclear X(PP) 2 FeC 4 Fe(PP) 2 X molecular wires (PP = Et 2 PCH 2 CH 2 PEt 2 ); X = CN (1), NCS (2), NCSe (3), C 4 SnMe 3 (4) and C 2 SnMe 3 (5)) under ultra-high vacuum and variable temperature conditions. In contrast to 1 which showed unstable junctions at very low conductance (8.1 · 10 −7 G 0 ), 4 formed a Au-C 4 FeC 4 FeC 4 -Au junction 4 after SnMe 3 extrusion which revealed a conductance of 8.9 · 10 −3 G 0 , three orders of magnitude higher than for 2 (7.9 · 10 −6 G 0 ) and two orders of magnitude higher than for 3 (3.8 · 10 −4 G 0 ). Density functional theory (DFT) confirmed the experimental trend in the conductance for the various anchoring motifs. The strong hybridization of molecular and metal states found in the C-Au coupling case enables the delocalized electronic system of the organometallic Fe 2 backbone to be extended over the molecule-metal interfaces to the metal electrodes to establish high-conductive molecular wires.KEYWORDS: Molecular wire, Single-molecule junctions, electronic transport, break-junctions, organometallic compounds, density functional theory Molecular electronics aims at employing single molecules as functional building blocks in electronic circuits. Besides such active components which provide, e.g., current rectifying or switching properties, also passive components such as molecular wires are required for the realization of molecular-scale electronics. Generally, an ideal wire has lowest resistance with almost linear (ohmic) and length-independent (ballistic) transport properties. For molecular wires, the required high conductance can in principle be achieved if low injection barriers for charge-carriers are present at the molecule-metal interfaces, if molecular orbitals (MOs) are available close to the Fermi energy of the electrodes, and if a large degree of electronic conjugation across the backbone is present. Already the first task seems to be difficult to achieve as the most frequently used thiol anchoring 1,2 suffers from an electronically weak molecule-metal coupling. Additionally, multiple bonding sites available on the Au surface for the thiol bond give rise to alter- † IBM Research -Zurich ‡ University of Vienna ¶ University of Zurich nating energy barriers for charge-carrier injection and result in large fluctuations in the transport properties. Therefore other anchoring schemes such as nitriles, 3 isocyanides, 4 amines, 5 and pyridines 6 were ...