AVS 56th International Symposium & Exhibition | |
Surface Science | Friday Sessions |
Session SS1-FrM |
Session: | Nanoclusters, Organics and Beam Induced Chemistry |
Presenter: | M. Trelka, Universidad Autonoma de Madrid, Spain |
Authors: | M. Trelka, Universidad Autonoma de Madrid, Spain A. Medina, Universidad Autonoma de Madrid, Spain C. Urban, Universidad Autonoma de Madrid, Spain C. Claessens, Universidad Autonoma de Madrid, Spain R. Otero, UAM & IMDEA-Nano, Spain J.M. Gallego, ICMM-CSIC, Spain T. Torres, Universidad Autonoma de Madrid, Spain R. Miranda, UAM & IMDEA-Nano, Spain |
Correspondent: | Click to Email |
Organic nanoparticles display size-dependent absorption and fluorescence bands and single photon emission. The detailed understanding of these effects is hindered by the difficulty in the synthesis of organic nanocrystals, i.e. organic nanoparticles with an ordered molecular arrangement. A possibility that remains mostly unexplored is the synthesis of such nanocrystals on solid surfaces. In the same way in which crystalline inorganic nanodots can be epitaxially grown on suitable substrates under conditions in which 3D Volmer-Weber growth takes place, an organic system could in principle be devised such that the growth of crystalline 3D islands sets in before the completion of the first monolayer. In practice, however, for organic adsorbates deposited on inorganic substrates intermolecular interactions are much weaker than molecule-substrate interactions, thus promoting a layer-by-layer growth mode, and preventing the fabrication of isolated 3D nanocrystal.
Here we show that, upon deposition of cone-shaped subphthalocyanine (SubPc) molecules on Cu(111), isolated triangular nanocrystallites up to 3 ML high appear on the surface before the completion of the first monolayer. The different molecular layers show an alternating or antiferroelectric (AF) stacking of the molecular dipole moments. The structure of such nanocrystals can be explained by the joint effect of electrostatic (dipole-dipole) and dispersive (π-π) interactions. Although 1 ML-thick islands can also be found on the surface, the molecular arrangement in these areas is different from the geometry of the 1st-layer molecules in the crystallites. We suggest that the formation mechanism of the organic nanocrystals is related to the existence of two different adsorption geometries, cone-up and cone-down, each of which sits on different molecular layers placed at different distances from the surface upon crystallite formation.