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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5.6 Realization <strong>of</strong> P-N Junction Structure<br />
5.6 Realization <strong>of</strong> P-N Junction Structure<br />
Another task is to realize a P-N structure by MBE. The capability <strong>of</strong> realizing<br />
well-controlled abrupt doping proles and alloy heterojunctions oer many opportunities<br />
to implement device structures, however, have not been practical or<br />
realizable by MBE in silicon in the past. The development <strong>of</strong> Si MBE technology<br />
is particularly important since there is an enormous Si technology base already<br />
existing in industry, and any new advance in Si technology is extremely important<br />
to the <strong>semiconductor</strong> industry as a whole. However, in order to realize P-N junction<br />
structure as well as controlled doping prole for light emitting diode (LED)<br />
applications, a Si layer with dierent As 4 uxes and dierent Si thicknesses was<br />
grown on exactly oriented undoped Si (100) substrate in MBE system. Group V<br />
<strong>semiconductor</strong>s like arsenic (As) or phosphor (P) act as n-type dopant <strong>of</strong> Si. The<br />
silicon homo<strong>epitaxial</strong> <strong>growth</strong> was performed by electron <strong>beam</strong> evaporation system<br />
(EBE), since the vapor pressure <strong>of</strong> silicon is extremely low, and conventional<br />
eusion cells cannot generate a sucient silicon vapor. However, due to the fact<br />
that in our <strong>III</strong>-V MBE system used for silicon homoepitaxy only an arsenic cell<br />
is installed and no phosphorous cell, the n-type doping in Si was performed by<br />
As 4 .<br />
After our standard ex-situ (BHF wet etching for 2 min.) and in-situ (thermal<br />
oxide desorption at 870 ◦ C for 15 min.) surface treatment, the substrate temperature<br />
was reduced to 650 ◦ C for doped Si layer <strong>growth</strong>. The <strong>growth</strong> rate <strong>of</strong><br />
Si was set to ∼ 5 nm/min, which corresponds to an emission current <strong>of</strong> 68 mA<br />
and voltage <strong>of</strong> 6 kV. However, in order to study the inuence <strong>of</strong> As 4 ux on the<br />
doping level <strong>of</strong> the grown Si layer, three dierent samples with dierent As 4 uxes<br />
were grown with the same <strong>growth</strong> conditions and same Si layer thickness. A Si<br />
buer layer with 100 nm thickness was grown at 650 ◦ C and As 4 equivalent <strong>beam</strong><br />
pressure (EBP) <strong>of</strong> 1.2 × 10 −8 Torr. While, the next two samples were grown as<br />
the rst sample but with double and triple As 4 ux. After that, a contact layer <strong>of</strong><br />
metallic contact stripes with 20 nm Pt, 80 nm Ti and 300 nm Au were deposited<br />
on the top <strong>of</strong> the doped Si layer for further electrical resistivity characterizations<br />
as shown in Fig. 5.31. The red arrow shows the direction <strong>of</strong> the current ow<br />
between two <strong>of</strong> the stripes highlighted in dark-orange color. The measurement<br />
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