Ge quantum dots on a large band gap semiconductor: the first growth stages on 4H–SiC(0 0 0 1) |
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Authors: | K Aït-Mansour D Dentel J L Bischoff L Kubler M Diani A Barski M Derivaz P No |
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Institution: | a LPSE, UMR 7014 CNRS-UHA, 4 rue des Frères Lumière, 68093, Mulhouse Cedex, France;b LSGM, Département de Physique, Faculté des Sciences et Techniques, BP 416, Tanger, Morocco;c CEA-DRFMC, 17 rue des Martyrs, 38054, Grenoble Cedex 9, France |
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Abstract: | The Ge growth on SiC(0 0 0 1) follows a Stranski–Krastanov mode for Si-rich (3×3) and
reconstructed surfaces. For Ge deposit in particular temperature conditions, a new (4×4) superstructure takes place and the reflection high energy electron diffraction (RHEED) specular spot intensity presents one oscillation proving a wetting layer formation. An island nucleation is then ascertained by the oscillation vanishing and by the appearance of a k-modulated RHEED pattern. On the other hand, on a
C-rich surface, a direct Ge island nucleation is observed from the first growth stage. Indeed, for 1 ML Ge, the RHEED diagram consists in spots and rings, and the atomic force microscopy analysis indicates a high density (8×1010 cm−2) of small islands (30 nm, h3 nm). The RHEED spot analysis shows a preferential epitaxial relationship with the substrate Ge(1 1 1)//SiC(0 0 0 1). The Ge–C bonding being energetically unfavourable, Ge tends to form islands immediately rather than wetting the graphite-terminated surface. The Ge growth mode on C-rich surface is thus of Volmer–Weber type. |
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Keywords: | SiC Ge nanocrystals Molecular beam epitaxy Electron diffraction Surface reconstructions |
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