Diplomarbeit Diplom-Ingenieur - Institut für Halbleiter
Diplomarbeit Diplom-Ingenieur - Institut für Halbleiter
Diplomarbeit Diplom-Ingenieur - Institut für Halbleiter
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8<br />
conditions are essential for the crystal growth. A common method for in situ<br />
characterisation is Reflection High Energy Electron Diffraction (RHEED).<br />
The basic processes of crystal growth take place in three zones between the<br />
effusion cell and the sample surface. Firstly, there is the molecular beam generation<br />
zone. The vapour elements mix in the mixing zone and crystal growth takes place in<br />
the crystallisation zone on the substrate surface. The growth itself is controlled by the<br />
substrate temperature, the beam flux and the process time. A schematic drawing of a<br />
MBE system with the tree process zones can be seen in Fig. 2.3.<br />
Figure 2.3: Sketch of a MBE System [27]. The essential parts of the system are shown,<br />
and the tree main process zones are indicated.<br />
In general, three epitaxial growth modes driven by energy minimisation can be<br />
distinguished. The energy terms are the surface, interface and strain energy. The<br />
Frank-van der Merwe growth is a monolayer-by-monolayer growth. The substrate and<br />
the epi-material have a fitting lattice constant, thus no strain is established during the<br />
crystal growth. The interface energy is smaller than the surface energy, consequently<br />
the epi-layer minimises its surface and grows in closed monolayer steps. The Volmer-<br />
Weber mode refers to a pure island growth on the surface. The strain energy term<br />
plays again no role. The surface energy is now the smaller term and the crystal grows<br />
with the minimum interface in the shape of islands. The Stranski-Krastanov growth is