AVS 55th International Symposium & Exhibition
    Nanometer-scale Science and Technology Friday Sessions
       Session NS+NC-FrM

Paper NS+NC-FrM3
Fullerene Growth on N-adsorbed Cu(001) Nanopatterned Surfaces

Friday, October 24, 2008, 9:00 am, Room 311

Session: Nanoscale Processes
Presenter: T. Iimori, University of Tokyo, Japan
Authors: T. Iimori, University of Tokyo, Japan
B. Lu, University of Tokyo, Japan
K. Sakamoto, Chiba University, Japan
K. Nakatsuji, University of Tokyo, Japan
F. Rosei, University of Quebec, Canada
F. Komori, University of Tokyo, Japan
Correspondent: Click to Email

Nitrogen (N)-adsorbed Cu(001)-c(2x2) nanopatterned surfaces are used as templates to guide the growth of low-dimensional C60 molecular nanostructures. The detailed nucleation and growth behaviors are studied by in situ scanning tunneling microscopy(STM). At room temperature, on the 0.3 ML-N-covered surface, where 5x5 nm2 patches of the c(2x2)-N surface are squarely arranged and bare Cu(001) surface. In other word, the bare Cu surface forms a nanogrid. Here ML is defined as the Cu atom density of the clean Cu(001) surface. During the initial stages of growth, C60 molecules preferentially adsorb on the bare Cu regions on a partially N-covered grid surface. Subsequently a two-dimensional molecular nanomesh is formed after C60 covers all the bare Cu regions. Further deposition leads to C60 growth on the c(2x2)-N areas until the first molecular layer is completed. For N-saturated surface with trench structures, the <010> steps of these structures serve as initial anchoring sites for C60 growth. From there, the growth proceeds two-dimensionally until a single C60 layer is achieved due to island coalescence. In contrast, no nucleation site was observed when the <110> steps were predominant on the surface. At least up to 6 mono-molecule layer, the growth proceeds layer-by-layer i.e., the overlayer morphologies are directed by the underlying substrate pattern in both (partially and fully N-covered) surfaces. Four rotational domains are observed for the quasi-hexagonally close-packed C60 overlayer with a nearest-neighbor C60-C60 distance of 1.02 nm. It is found that the interaction between C60 and the c(2x2)-N surface is fairly weak, likely to be dominated by van der Waals forces, whereas the C60-Cu interface is chemisorbed. Site-specific electronic effects between these two regions can be resolved by STM even for thick films.