Atomic structure of an Al-Co-Ni decagonal quasicrystalline surface

J. Yuhara1, J. Klikovits2, M. Schmid2, P.Varga2, Y. Yokoyama3, T. Shishido4, K. Soda5

1 Department of Physical Science and Engineering, School of Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, 464-8603, Japan
2 Institut für Allgemeine Physik, Technische Universität Wien, 1040 Wien, Austria
3 Faculty of Engineering, Himeji Institute of Technology, Shosha, Himeji, 671-2201, Japan
4 Institute for Materials Research, Tohoku University, Sendai, 980-8577, Japan
5 Department of Crystalline Materials Science, School of Engineering, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, 464-8603, Japan

Phys. Rev. B 70 (2004) 024203

We have analyzed the structure and composition of the first layer of an Al72Co16Ni12 tenfold surface by means of scanning tunneling microscopy (STM), ion scattering spectroscopy (ISS), and Auger electron spectroscopy (AES). High-resolution STM images reveal local structures that have decagonal symmetry in addition to the usual pentagonal symmetry of the surface. This quasicrystal surface resembles a random tiling instead of an ideal quasiperiodic tiling. After annealing at 1100 K, the total surface atomic density found by ISS is (9±1)x1014 cm-2. The surface densities of Al and TM (transition metal, i.e., Co and Ni) are determined as (8±1)x1014 cm-2 and (1.0±0.2)x1014 cm-2, respectively, from ISS, indicating a similar density of Al and much lower density of the TM atoms in the surface layer than in a trucated bulk. The Al surface atomic density agrees well with the number of corrugation maxima in the STM images. A model of the arrangement of the Al atoms in the top layer is presented. Scanning tunneling spectroscopy (STS) is performed to study the local electronic structure. The STS spectrum at the corrugation maxima is similar to that at the corrugation minima. A few approx. 0.12 nm high protrusions in the STM images are attributed to local oxide clusters due to their different STS spectra different from the corrugation maxima and through in-situ STM observations during exposure to O2 gas at 2x10-6 Pa at RT.

Corresponding author: J. Yuhara. Reprints also available from M. Schmid (schmid< encoded email address >).

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