First Principle Investigation Of Doped SiC and ZnO For Optoelectronic Applications
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newlineThis dissertation provides a comprehensive examination of pristine and doped silicon carbide
newline(SiC), and zinc oxide (ZnO) systems, utilizing a first-principles density functional theory
newline(DFT) methodology to explore their structural, electronic, magnetic optical properties for
newlineoptoelectronic devices. Zigzag SiC Nanotubes ((8,0), (9,0), (10,0)) were systematically studied
newlinetogether with ZnO primitive and supercell models utilizing BIOVIA Materials Studio with the
newlineCASTEP module in the intrinsic, transition metal doped and group-III doped configuration
newlineincluding oxygen vacancies for ZnO.
newlineIntrinsic SiC nanotubes possessed well-defined semiconducting behavior, with their band gap
newlinenarrowing as the diameter increased owing to quantum size effects. Their optical behavior
newlineexhibited high absorption in the UV and low absorption in the visible, indicating their
newlinetransparency. Doping with transition metals vanadium and manganese exhibited large
newlineelectronic and magnetic changes. V-doped SiC nanotubes exhibited half-metallicity with high
newlinespin polarization and would therefore be suitable for spintronic devices and UV photodetectors.
newlineMn-doped SiC nanotubes exhibited half-metallic magnetic semiconductor behavior under UV
newlinelight, with extended absorption into the IR range, and could be promising materials in IR/NIR
newlinesensors applications.
newlineIn the case of ZnO systems, confirmed that intrinsic ZnO is a wide band gap semiconductor
newlinewith lattice parameter values comparable to what was determined experimentally. Doping with
newlineGroup-III elements (B, Al, Ga, In) led to a significant increase in n-type conductivity; the
newlineatomic radius of B, Al, and Ga, which is smaller than the radius of Zn, led to decreases in the
newlinelattice constants while the doping of In cause expansion in the lattice constants of ZnO.
newlineOxygen vacancies were crucial because they introduce shallow donor states near the energy of
newlinethe conduction band edge, which increased carrier concentrations in the samples and altered
newlinethe optical responses of samples