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Computer simulation of nanosized silicon clusters with reconstructed surfaces

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The Fifth Conference “ Nuclear Science and Its Application”, 14-17 October 2008

COMPUTER SIMULATION OF NANOSIZED SILICON CLUSTERS WITH

RECONSTRUCTED SURFACES

F.T. UMAROVA. A.P. MUKHTAROV, P.L. TERESHCHUK, N.T. SULAYMANOV, M.T. SWIHART*

Institute o f Nuclear Physics o f Academy of Science o f Uzbekistan *New York University at Buffalo, USA

Nanosized silicon clusters have been attracting much attention, due to their luminescent properties. The core o f luminescent Si nanoparticles is commonly presumed to be diamond-like as in bulk silicon, and has a form o f the perfect tetrahedron. But a large value o f surface curvature and presence of dangling bonds on surface may strongly distort tetrahedral coordination o f inner atoms and change length o f covalent bonds, that, in turns, influence on their electronic properties. Unlike bulk materials, in the case o f clusters the problem is absence o f appropriate models describing energetically favorable surface structures. In this work influence o f surface reconstructions on inner structure o f clusters Sİ29, Sİ38, and Sİ59 are investigated by non-conventional tight-binding molecular dynamics method.

Some possible variants o f surface reconstructions o f bare silicon clusters are simulated. For clusters with a diamond-like core, energetically unfavorable dangling bonds on their surface were partially eliminated by dimerization (trimerization) o f Si atoms with two dangling bonds and/or overcoordination o f surface atoms. Optimized geometries o f clusters w ith a diamond-like core were sensitive to the initial surface reconstruction model. Clusters w ith dimerized and trimerized surface atoms Sİ29D, Sİ38D, Sİ59T preserve its tetrahedral coordination after optimization. One can see significant shrinking o f the surface formed by dimerized atoms in the cluster Sİ29D. The dimerized cluster Sİ38D showed strong surface reconstruction that led to the formation o f capped pentagon motifs on the surface. In other cases (embedding additional atoms in surface positions (Sİ29E6, Sİ38E6, Sİ59E12) correspond to a tetrahedral interstitial positions in bulk silicon, or smoothing surface by removing three-coordinated vertex atoms in possible strain configurations Sİ32S, Sİ38S, Sİ65S) optimized cluster geometries give structures, those do not contain a diamond­ like core. Simulation o f clusters with various surface reconstructions shows, that the surface regions o f large diamond-like clusters are expected to be reconstructed such that they consist o f pentagon- based fragments attached to the diamond-like core.

The highest occupied molecular orbital - lowest unoccupied molecular orbital (HOMO-LUMO) gap of the clusters calculated here considerable changes with growth of its size and is in qualitative agreement with the experiment (B. Marsen, M. Lonfat, P. Scheier, K. Sattler, Phys. Rev. B 62,6892 (2000)), reflecting non­ regularity of gap with cluster size and a similar maximum gap o f0.523 eV for cluster Sİ29 with embedding six additional atoms in surface positions. The surface reconstruction models, based on dimerization, can explain metallic or semi-metallic behavior of the clusters as well. The mixing of the closed HOMO-LUMO states, the number of those increases with cluster size, can cause disordering and even amorphization of clusters.

The HOMO-LUMO gap o f clusters with H-terminated surface increases with increasing the number o f hydrogen atoms on surface. For example, the gap width for cluster Sİ29D achieves value o f 2.7-3.0 eV at fiili saturation o f dangling bonds by 24 atoms o f hydrogen.

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