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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3.4 Challenges <strong>of</strong> Hetero<strong>epitaxial</strong> Growth <strong>of</strong> <strong>III</strong>-V on Silicon<br />
tempts and research activities at defect-free hetero-integration. Lattice constant<br />
mismatch in most <strong>III</strong>-V/Si combinations causes detrimentally high dislocation<br />
densities in the <strong>III</strong>-V epilayers [37]. The thermal expansion coecient dierences<br />
between Si and <strong>III</strong>-V materials leads to variable strain conditions during temperature<br />
changes, making alternative large area scale solutions, such as wafer<br />
bonding, a signicant challenge [38]. Additionally, the heterovalent (i.e. polar/nonpolar)<br />
nature <strong>of</strong> the <strong>III</strong>-V/Si interface is a source <strong>of</strong> numerous harmful<br />
defects, such as anti-phase domains (APDs), stacking faults (SF), and microtwins<br />
(MT) [1, 39]. The combinations <strong>of</strong> these problems has proved a signicant road<br />
block to high-quality <strong>III</strong>-V on silicon hetero-integration. In this section, the fundamental<br />
challenges and barriers <strong>of</strong> the <strong>epitaxial</strong> integration between <strong>III</strong>-V and<br />
silicon are discussed in details.<br />
The major material dierences between <strong>III</strong>-V's like InAs, GaP, GaAs and<br />
silicon are summarized in Table 3.1.<br />
Semiconductor/Property Si InAs GaAs GaP<br />
Crystal structure Diamond Zinc Blende Zinc Blende Zinc Blende<br />
Lattice constant (A ◦ ) 5.43095 6.0584 5.6533 5.4512<br />
Thermal expansion coecient<br />
2.6 × 10 −6 5.19 × 10 −6 5.7 × 10 −6 4.7 × 10 −6<br />
at 300 K (K −1 )<br />
Band gap energy at 300 K 1.12 0.354 1.424 2.26<br />
(eV )<br />
Band gap type Indirect Direct Direct Indirect<br />
Polarity Non-Polar Polar Polar Polar<br />
Table 3.1: Basic material properties dierence between dierent <strong>III</strong>-V compounds and<br />
Si substrate [40].<br />
It can be seen clearly from Table 3.1 that there are signicant disparities in<br />
the crystal structure, polarity, lattice constant, thermal expansion coecient and<br />
band gap nature between <strong>III</strong>-V compounds and Si.<br />
31