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Molecular beam epitaxial growth of III-V semiconductor ... - KOBRA

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MBE Growth <strong>of</strong> Self-Assembled InAs and InGaAs Quantum Dots Embedded in<br />

Silicon Matrix<br />

carried out at constant voltage <strong>of</strong> 1 V , while the current was measured at different<br />

stripe distances. The I-V curve was recorded and the doping level was<br />

calculated for dierent As 4 uxes. Fig. 5.32 shows the doping level dependence<br />

with the BEP As 4 ux. A linear carrier concentration dependence on As 4 ux<br />

was observed up to a doping level <strong>of</strong> 7.28 × 10 17 cm −3 for a As 4 <strong>of</strong> BEP value<br />

3.6 × 10 −8 Torr. A new series <strong>of</strong> samples were studied by keeping the As ux<br />

constant at 1.2 × 10 −8 Torr but with increasing the layer thickness from 100 nm<br />

to 200 nm.<br />

Figure 5.31: Schematic digram <strong>of</strong> the metallic stripes with dierent widths deposited<br />

on the top <strong>of</strong> the doped Si layer, for the electrical resistivity measurements.<br />

Resistivity measurement showed that the doping density increased by a factor<br />

<strong>of</strong> three with increased layer thicknesses from 100 nm to 200 nm, this can be explained<br />

by the band bending eect, which will get less with thicker layers. Hence,<br />

the transfered electrons that occupy the region where the conduction energy E c<br />

is below the Fermi level, and constitute an accumulation layer whose thickness<br />

is much less than the width <strong>of</strong> the band-bending in metal n-type <strong>semiconductor</strong><br />

junction [15].<br />

100

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