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M. Castro et al. (to be published)
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M. Castro et al. (to be published).
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18144422390
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note
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Due to their irrelevance at the θ = 0 condition considered here, we have ignored the anisotropies of the sputtering yield with substrate directions, studied in [20].
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28
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18144401979
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note
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In [5] θ ≠= 0 is used, with simultaneous substrate rotation. Results below apply after azimuthal average [20].
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29
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18144391888
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note
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3H. The former is cubic, rather than quadratic, in derivatives of H. The latter is multiplied by a small coefficient in the limit taken. Although, they influence properties like the dot shape [20], being small, they do not change the qualitative properties of in-plane dot ordering of interest here.
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32
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18144381910
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note
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2- See experiments in, e.g., G. Costantini et al., Surf. Sci. 416, 245 (1998).
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33
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0032181054
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2- See experiments in, e.g., G. Costantini et al., Surf. Sci. 416, 245 (1998).
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Costantini, G.1
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0034890412
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As in the KS theory of IBS [see, e.g., S. Facsko et al., Phys. Rev. B 63, 165329 (2001)], qualitative predictions are accurate, but quantitative predictions may deviate due to neglected mechanisms actually contributing to the interface equation with the same terms as considered.
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Facsko, S.1
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35
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18144421862
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F. Frost et al. (to be published)
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F. Frost et al. (to be published).
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