1990
DOI: 10.1103/physrevlett.65.3313
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Phase behavior of the Au(111) surface: Discommensurations and kinks

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Cited by 143 publications
(74 citation statements)
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“…The reconstruction can be described as a continuous commensurate-incommensurate transformation in which the surface layer is isotropically compressed relative to the underlying bulk lattice. A similar reconstruction occurring above 0.65 Tmhas also been reported for (111) oriented Au surfaces [62]. At lower temperatures, a 23 x ",/3 reconstruction has been observed in Au(111) that can be described as an insertion of an extra row of atoms every 23 rows on the surface [63].…”
Section: Surface Reconstructions Of Clean Metal Surfacessupporting
confidence: 50%
“…The reconstruction can be described as a continuous commensurate-incommensurate transformation in which the surface layer is isotropically compressed relative to the underlying bulk lattice. A similar reconstruction occurring above 0.65 Tmhas also been reported for (111) oriented Au surfaces [62]. At lower temperatures, a 23 x ",/3 reconstruction has been observed in Au(111) that can be described as an insertion of an extra row of atoms every 23 rows on the surface [63].…”
Section: Surface Reconstructions Of Clean Metal Surfacessupporting
confidence: 50%
“…In fact, it has been clear for many years that some restructuring of this surface occurs as the thiolate SAM forms, because the clean Au(111) surface is, itself, reconstructed, and this reconstruction is lifted as the thiolate coverage increases [72]. In particular, the outermost atomic layer of clean Au(111) adopts a uniaxially-compressed hexagonal close-packing leading to an Au-Au interatomic spacing smaller that that of the underlying bulk [73,74,75]. The atomic density of this layer is 4.4% larger than that of the bulk layers below, and this surface layer rumples over the substrate to give a (23x3)rect.…”
Section: Reconstruction and Au Adatomsmentioning
confidence: 99%
“…9 At room temperature, the (22 × 3) phase is stable, while the first-order phase transition to the (1 × 1) phase requires heating to 880 K under ultrahigh vacuum (UHV). 10 In an electrochemical environment, however, the phase transition can be induced by changing the electrode potential. The existence of this phase transition in electrochemical environments was first suggested by classical voltammetry.…”
Section: Introductionmentioning
confidence: 99%