Molecular beam epitaxial growth of III-V semiconductor ... - KOBRA
Molecular beam epitaxial growth of III-V semiconductor ... - KOBRA
Molecular beam epitaxial growth of III-V semiconductor ... - KOBRA
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4.2 <strong>Molecular</strong> Beam Epitaxy Technique<br />
Figure 4.1: Schematic digram <strong>of</strong> general MBE <strong>growth</strong> chamber with its majors parts<br />
like, eusion cells or even other types <strong>of</strong> cells like sumo and cracker cells and their<br />
shutters, RHEED system, <strong>beam</strong> ux monitoring gauge, sample transfer manipulator,<br />
liquid nitrogen cooled panels and substrate heater supply with speed motor for rotation.<br />
Figure modied according to reference [33].<br />
in the UHV range, typically in the range <strong>of</strong> 10 −9 to 10 −11 T orr, by a combination<br />
<strong>of</strong> pumps, including ion pump, cryogenic pump, turbo molecular pump, trapping<br />
pump and liquid-nitrogen-lled cryo shroud. The UHV environment allows deposition<br />
with extremely low impurity concentrations and enables the use <strong>of</strong> in-situ<br />
surface analysis tools, such as reective high energy electron diraction as illustrated<br />
in Fig. 4.1. More importantly, it maintains source uxes in the molecular<br />
ow regime, so that individual molecules do not collide or react with each other<br />
before reaching the substrate referred as physical deposition, and species that<br />
miss or desorb from the substrate are pumped away immediately.<br />
Material sources in MBE systems are typically Knudsen eusion cells or Sumo<br />
cells, which are loaded with ultra pure materials and dopants like group II, <strong>III</strong> and<br />
IV materials (eg., In, Ga, Al, Be, Si) from which molecular <strong>beam</strong>s are generated by<br />
thermal evaporation or sublimation (temperature controlled cells). The elemental<br />
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