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85033125737
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We assume the surface alloy is random because no change in the (1x1) pattern is observed. This result is in agreement with recent investigations of the low-coverage regime by the group of Wuttig, who report no ordered superstructures for coverages below 0.3 ML
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We assume the surface alloy is random because no change in the (1x1) pattern is observed. This result is in agreement with recent investigations of the low-coverage regime by the group of Wuttig, who report no ordered superstructures for coverages below 0.3 ML.
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13
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0030243970
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Our calculations were performed using EMT codes devised by Stoltze
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The computational method is described in
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Our calculations were performed using EMT codes devised by Stoltze. The computational method is described in: P. Stoltze, J. Phys. Condens. Matter 6 (1994) 9495.
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Stoltze, P.1
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15
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85033121773
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All of the simulations were performed using a (10x10) slab supercell consisting of five layers, two of which were held fixed at the EMT-derived bulk spacing. A [110] step was created at this surface by placing 0.5 ML of Cu adatoms in the appropriate geometry above the slab
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All of the simulations were performed using a (10x10) slab supercell consisting of five layers, two of which were held fixed at the EMT-derived bulk spacing. A [110] step was created at this surface by placing 0.5 ML of Cu adatoms in the appropriate geometry above the slab.
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