Abstract
The geometry of PTCDA adsorbed on a (110)-oriented silver crystal is optimized on a finite metal cluster used as a rigid substrate. In a comparison between second-order Moller−Plesset perturbation theory (MP2) and density functional theory (DFT), we find pronounced differences; MP2 gives a nearly flat adsorbate, in agreement with the geometries deduced from X-ray standing wave studies on similar substrates, whereas the lack of dispersion interactions in DFT results in a strongly bent geometry. In MP2, the van-der-Waals attraction counterbalances the overlap repulsion, resulting in an average height of the PTCDA adsorbate above the topmost substrate layer of 2.68 A for C atoms, comparing favorably with recent measurements based on X-ray standing wave techniques. The carboxylic oxygens interact more strongly with the substrate than the anhydride groups, so that we predict a height difference of 0.13 A between both types of oxygen atoms.
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