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Hubbard J 1963 Proc. R. Soc. A 276 238 Hubbard J 1964 Proc. R. Soc. A 277 237 Hubbard J 1964 Proc. R. Soc. A 281 401
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Ruban, A.1
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31
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11644255204
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note
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(iii) (ζ) = 11.802 and 3.628 electrons for Zn/Cu and Nb/Cu respectively. These results support the success of our method as applied within the level of approximation (ii) as they indicate that the transferred charge is not appreciably affected by the charge relaxation within the surrounding impurity cells.
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32
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11644266100
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note
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The present method can be used to verify the approximation according to which a bulk excited atom with atomic number Z having a hole in an inner-electron shell can be approximated as a Z + 1 impurity atom in a Z-atom host [9].
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35
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0001492781
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Shirley D A, Martin R L, Kowalczyk S P, McFeely F R and Ley L 1977 Phys. Rev. B 15 544
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(1977)
Phys. Rev. B
, vol.15
, pp. 544
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Shirley, D.A.1
Martin, R.L.2
Kowalczyk, S.P.3
McFeely, F.R.4
Ley, L.5
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41
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11644275007
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note
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Our results for the free-atom excitation energies were found to be practically unaffected if the Hedin-Lundqvist [38] expression for the exchange and correlation energy per atom is replaced by that of Vosko, Wilk and Nusair [40].
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43
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0001131756
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Vosko S H, Wilk L and Nusair M 1980 Can. J. Phys. 58 1200 Painter G S 1981 Phys. Rev. B 24 4264
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(1981)
Phys. Rev. B
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, pp. 4264
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Painter, G.S.1
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44
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11644319833
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note
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1 type.
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45
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11644270417
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note
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A similar case is observed in other LDA-based electronic structure calculations. For example, state-of-the-art computations [43] of the bulk modulus of various metals predict results in very good agreement with experiment if the bulk modulus is calculated at the experimentally observed lattice constant of the metal instead of using the one found theoretically.
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