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Kinetic and Strain-Induced Self-Organization of SiGe ...

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18 CHAPTER 2. MOLECULAR BEAM EPITAXY (MBE)<br />

Figure 2.2: Schematic illustration <strong>of</strong> surface processes occurring during MBEgrowth<br />

[12].<br />

� Source: MBE surface-kinetics.jpg<br />

temperature <strong>of</strong> the region <strong>of</strong> their origin (source temperature). This initial temperature Ti is<br />

usually higher than the substrate temperature TS; hence they have to loose energy via energy<br />

exchange with the substrate until thermodynamic equilibrium at TS is reached. When the<br />

impinging species stays adsorbed due to a lack <strong>of</strong> energy for desorption (re-evaporation into<br />

vacuum) the particles diffuse along the surface in order to find an energetically favored lattice-<br />

site, such as a kink-position, where one half <strong>of</strong> the bonds is occupied. Other possibilities for<br />

reactions on the surface are inter-diffusion (two atoms exchange sites) or nucleation processes<br />

that appear, when migrating atoms aggregate <strong>and</strong> form a new isl<strong>and</strong> on a flat part <strong>of</strong> the<br />

substrate surface. [55]<br />

2.1.3 Growth-Modes<br />

As mentioned at the end <strong>of</strong> the last section, atoms preferentially become incorporated at kink-<br />

sites. Incorporation itself has been experimentally documented [59] <strong>and</strong> can be understood<br />

as a two-step condensation process in which the chemisorbed state is reached via a precursor<br />

physisorbed phase [60]. According to the model in Ref. [61, 62, 63] the atom as physisorbed<br />

species is allowed to diffuse over the surface with a rate constant kdiff to find an energetically<br />

favored site. The interaction potentials as seen by an atom approaching the surface are<br />

schematically depicted in Fig. 2.3 [55, 64]. It is evident from Fig. 2.3 that the physisorbed

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