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85038269603
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The total energy of the supercell depends on the actual configuration of atoms even in the absence of the vacancy. This is mainly due to the fact that (Formula presented) and (Formula presented) are lattice mismatched, and a redistribution of atoms induces a change in the excess strain energy, cf. Ref. 16. The charge transfer effects due to different electronegativities of Al and Ga (or Si and Ge) change the total energy by one order of magnitude less (Ref. 16). To minimize this effect, the (Formula presented) variants were obtained by a series of exchanges of adjacent atoms. In this way, the locations of almost all the atoms in the supercell were the same for all cases. In particular, for configurations corresponding to (Formula presented) and (Formula presented) variants, the total energies of the supercells without defects agree to within 0.2 eV
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The total energy of the supercell depends on the actual configuration of atoms even in the absence of the vacancy. This is mainly due to the fact that (Formula presented) and (Formula presented) are lattice mismatched, and a redistribution of atoms induces a change in the excess strain energy, cf. Ref. 16. The charge transfer effects due to different electronegativities of Al and Ga (or Si and Ge) change the total energy by one order of magnitude less (Ref. 16). To minimize this effect, the (Formula presented) variants were obtained by a series of exchanges of adjacent atoms. In this way, the locations of almost all the atoms in the supercell were the same for all cases. In particular, for configurations corresponding to (Formula presented) and (Formula presented) variants, the total energies of the supercells without defects agree to within 0.2 eV.
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18
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85038312057
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A more precise statement would necessitate the calculation of the band-gap correction to the local-density approximation, an assessment of the bowing effect (Ref. 18), and an inclusion of more k points in the supercell calculations
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A more precise statement would necessitate the calculation of the band-gap correction to the local-density approximation, an assessment of the bowing effect (Ref. 18), and an inclusion of more k points in the supercell calculations.
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24
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4243618941
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C. G. Van De Walle, D. B. Laks, G. F. Neumark, and S. T. Pantelides, Phys. Rev. B 47, 9425 (1993).
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Van De Walle, C.G.1
Laks, D.B.2
Neumark, G.F.3
Pantelides, S.T.4
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