Calculation of deep states in SiGe alloys: Interstitial carbon-oxygen complexes
Calculation of deep states in SiGe alloys: Interstitial carbon-oxygen complexes
Balsas, A; Coutinho, J; Torres, V. J. B; Briddon, P. R; Barroso, M. R
2004-08-15 00:00:00
We show that using a density-functional supercell method we are able to follow the location of defect gap levels in SiGe alloys for different alloying compositions. The method is tested for several properties of the alloys, with special emphasis in the local bond-length relaxations. Our results indicate a predominant Pauling character for the alloys, with a topological rigidity parameter a * * lying between 0.7 and 0.8. A comparative study between the electrical properties of the interstitial carbon ( C i ) and carbon-oxygen ( C i O i ) centers in the alloys, shows that these complexes interact weakly with Ge atoms. The C i O i defect is predicted to produce a hole trap that varies as Δ E ( 0 ∕ + ) = 0.41 − 0.76 x eV , implying its disappearance for Ge fractions x greater than ∼ 0.5 .
http://www.deepdyve.com/assets/images/DeepDyve-Logo-lg.pngPhysical Review BAmerican Physical Society (APS)http://www.deepdyve.com/lp/american-physical-society-aps/calculation-of-deep-states-in-sige-alloys-interstitial-carbon-oxygen-GLZ7BoiyYb
Calculation of deep states in SiGe alloys: Interstitial carbon-oxygen complexes
We show that using a density-functional supercell method we are able to follow the location of defect gap levels in SiGe alloys for different alloying compositions. The method is tested for several properties of the alloys, with special emphasis in the local bond-length relaxations. Our results indicate a predominant Pauling character for the alloys, with a topological rigidity parameter a * * lying between 0.7 and 0.8. A comparative study between the electrical properties of the interstitial carbon ( C i ) and carbon-oxygen ( C i O i ) centers in the alloys, shows that these complexes interact weakly with Ge atoms. The C i O i defect is predicted to produce a hole trap that varies as Δ E ( 0 ∕ + ) = 0.41 − 0.76 x eV , implying its disappearance for Ge fractions x greater than ∼ 0.5 .
Journal
Physical Review B
– American Physical Society (APS)
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