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We have substantiated our claim by carrying out a relaxation under the same condition used in Refs. 4,9. We found the distance between the adatom and the layer-2 atom directly underneath it to be 2.6 Å, in agreement with the TB result of Ref. 4. Furthermore, calculation in Ref. 8 indicated that the inclusion of an ad hoc Hubbard-like term, although moderates the charge transfer in the buckled dimers of the reconstructed Si(001) surface, changes the surface energy by only less than 0.01 eV/atom, inducing no significant change in the structure. Considering that no unusual configuration such as the buckled dimers on the surface of the Si(111)-7 × 7 surface, it is even more unlikely that there will be any appreciable effect on the dynamics of the Si(111)-7 × 7 surface associated with the charge transfer
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We have substantiated our claim by carrying out a relaxation under the same condition used in Refs. 4,9. We found the distance between the adatom and the layer-2 atom directly underneath it to be 2.6 Å, in agreement with the TB result of Ref. 4. Furthermore, calculation in Ref. 8 indicated that the inclusion of an ad hoc Hubbard-like term, although moderates the charge transfer in the buckled dimers of the reconstructed Si(001) surface, changes the surface energy by only less than 0.01 eV/atom, inducing no significant change in the structure. Considering that no unusual configuration such as the buckled dimers on the surface of the Si(111)-7 × 7 surface, it is even more unlikely that there will be any appreciable effect on the dynamics of the Si(111)-7 × 7 surface associated with the charge transfer.
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11
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0011435553
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See, for example, references therein
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See, for example, S.Y. Wu and C.S. Jayanthi, Int. J. Mod. Phys. B 9, 1869 (1995), and references therein.
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Wu, S.Y.1
Jayanthi, C.S.2
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