The adsorption of molecules on surfaces plays an important role in bottom-up nanofabrication. 1,2 Azobenzene and derivatives thereof are particularly interesting since these molecules are considered as model systems for molecular switches, 3-6 based on light-induced reversible trans-cis isomerizations. Consequently, they play an important role for optically active materials and devices. Switching of azobenzene derivatives at the liquid-solid interface has been demonstrated, [7][8][9][10] while investigations into the adsorption and switching behavior of azobenzene at surfaces under well-defined ultrahigh vacuum (UHV) conditions are only just emerging. 11,12 In this Communication, we investigate the adsorption geometries of azobenzene on the Cu(110) surface at low coverage and saturation limits. We show that only the trans-isomer is observed, and we investigate its diffusion behavior in both preferred and energetically metastable adsorption states.Scanning tunneling microscopy (STM) measurements were acquired with the variable-temperature Aarhus STM under UHV conditions. 13,14 Azobenzene (Sigma-Aldrich, 99.5% purity) was held in a transparent glass vial at room temperature and admitted into the UHV system via a leak valve. The Cu(110) surface was cleaned by repeated cycles of 1.5 keV Ar + ion bombardment followed by annealing to 820 K. All STM measurements were obtained in a temperature range of 120-170 K.Upon deposition at room temperature, individual molecules appear as two bright protrusions, attributed to flat lying phenyl rings, separated by a darker line associated with the NdN bond ( Figure 1a). This molecular signature is qualitatively as expected for the trans-isomer. The molecules adsorb with their axis at a slight angle to the close-packed [1 -1 0] direction and with their NdN bond at a bridge site as determined from images showing the Cu lattice at atomic resolution ( Figure 1c). Loss of symmetry upon adsorption results in two different surface enantiomers, distinguishable by the direction of the central dark line, as indicated by arrows in Figure 1a. A possible model of the molecular adsorption geometry is depicted in Figure 1b (the enantiomer with the NdN bond along the dark line is tentatively chosen to correspond to the shown direction of rotation).As the coverage is increased, the molecules do not show a strong tendency to cluster together, even if annealed to 500 K. Near half of saturation coverage (Figure 1d), the molecules begin to order by stacking sideways into columns running along the substrate [001] direction. The molecular head-to-head interaction appears to be weak or even repulsive as no ordering is observed along this direction. At saturation coverage (Figure 1e), the molecules form columns along the [001] direction with a periodicity of 7.9 ( 0.8 Å (dimension a in Figure 1e), consistent with two lattice spacings of the Cu substrate. At this separation, intermolecular H-N hydrogen bonding can occur with a reasonable bond length of less than 4 Å. The column-column distance along the ...