-
2
-
-
77949489215
-
-
note
-
Not a pure VCA one though, strictly speaking, since there is not a single bond length per alloy whose value varies smoothly between the parent ones when the alloy composition changes
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4
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Note that consistently with the L-version of Figure [SEE TEXT], ab initio calculations by Bellaiche et al., Phys. Rev. B 54, 17568 (1996) have revealed a 'universal' singularity in the average bond length (L) of each species at the related bond percolation threshold (x~0.19, 0.81) of a random alloy. Also, careful examination of the basic 1-bond→1-mode (L) distribution of (first-neighbour) bond lengths calculated by ab initio methods with InGaP by Silverman et al., Phys. Rev. B 51, 10795 (1995) reveals a fine structure under the form of a systematic asymmetry (the same for the two bond species), whose sign changes on each side of the stoichiometry. Such asymmetry finds a natural explanation within the interplay between the two populations of like oscillators in each double branch of the percolation scheme shown in Figure [SEE TEXT]
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9
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33749052002
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This was discussed in detail in our reference 4, and independently validated by ab initio calculations by
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on InGaP
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This was discussed in detail in our reference 4, and independently validated by ab initio calculations by Silvermann et al., Phys. Rev. B 51, 10795 (1995), on InGaP
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This should not be mistaken for some clustering though, as even in the limit of total ordering (η=1) each atom of a given species (say A) has one first-neighbour (out of four) of the other species (B, then)
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77949485123
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The barycentre is found over contributions of the same probed Se atom in the eigenvectors of many (strictly speaking, all) discrete vibration modes (96 in total in our supercell)
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