We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) surfaces by scanning tunneling microscopy. Contrary to what is observed on the singular surface, three-dimensional Ge nanoislands form directly through the elastic relaxation of step-edge protrusions during the unstable step-flow growth. As the substrate misorientation is increased, the islands undergo a shape transformation which is driven by surface energy minimization and controlled by the miscut angle. Using finite element simulations, we show that the dynamics of islanding observed in the experiment results from the anisotropy of the strain relaxation. © 2011 American Institute of Physics
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
A complete description of Ge growth on vicinal Si(001) surfaces in the angular miscut range 0 –8 is...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) surfac...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) 6 sur...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) 6 sur...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) 6 sur...
A complete description of Ge growth on vicinal Si(001) surfaces is provided. The distinctive mechani...
A complete description of Ge growth on vicinal Si(001) surfaces is provided. The distinctive mechani...
A complete description of Ge growth on vicinal Si(001) surfaces in the angular miscut range 0°-8° is...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
A complete description of Ge growth on vicinal Si(001) surfaces in the angular miscut range 0 –8 is...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) surfac...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) 6 sur...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) 6 sur...
We examine the structure and the evolution of Ge islands epitaxially grown on vicinal Si(111) 6 sur...
A complete description of Ge growth on vicinal Si(001) surfaces is provided. The distinctive mechani...
A complete description of Ge growth on vicinal Si(001) surfaces is provided. The distinctive mechani...
A complete description of Ge growth on vicinal Si(001) surfaces in the angular miscut range 0°-8° is...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
We have followed the evolution of strained Ge/Si(111) Stranski-Krastanov islands by atomic force and...
A complete description of Ge growth on vicinal Si(001) surfaces in the angular miscut range 0 –8 is...