1996
DOI: 10.1016/0039-6028(95)01011-4
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Minimum energy 2D patterns of atoms adsorbed on a hexagonal lattice

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Cited by 7 publications
(4 citation statements)
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“…Superconducting vortices either in Josephson junction arrays [69,70] or superconducting layers in the presence of periodic pinning [71][72][73][74][75] have been studied extensively by Monte Carlo simulations and analytical approaches [76][77][78][79][80][81][82][83][84][85][86] as well as molecular dynamics simulations [87,88]. Adsorbed atoms on a crystalline surface [89][90][91][92][93][94], colloidal systems on templates [95], organic conductors [96,97], as well as magnetic bubble arrays [98] also exhibit CLG characteristics. Recently, the configuration of a system of polarons in 1T-TaS 2 at very low temperatures has been investigated using the CLG model.…”
Section: Introductionmentioning
confidence: 99%
“…Superconducting vortices either in Josephson junction arrays [69,70] or superconducting layers in the presence of periodic pinning [71][72][73][74][75] have been studied extensively by Monte Carlo simulations and analytical approaches [76][77][78][79][80][81][82][83][84][85][86] as well as molecular dynamics simulations [87,88]. Adsorbed atoms on a crystalline surface [89][90][91][92][93][94], colloidal systems on templates [95], organic conductors [96,97], as well as magnetic bubble arrays [98] also exhibit CLG characteristics. Recently, the configuration of a system of polarons in 1T-TaS 2 at very low temperatures has been investigated using the CLG model.…”
Section: Introductionmentioning
confidence: 99%
“…There is clear evidence for the importance of such lateral interactions in previous work. 4,5 In the case of potassium adsorption on Pt͑111͒ potassium adlayers have been found to be structured in such a way as to minimise dipole-dipole interactions; 4 likewise sodium introduction to a Pt͑111͒ surface un-z E-mail: I.Metcalfe@newcastle.ac.uk der conditions of electrochemical promotion ͑imaged via STM͒ has been seen to result in the formation of ordered surface structures. 5 Now we must make some assumptions about the structure of the double layer to proceed ͑the fact that Fleig and Jamnik do not need to consider the structure of the double layer when introducing a new surface charge is in fact a further clear demonstration that their analysis is incorrect͒.…”
Section: Issuementioning
confidence: 99%
“…The structures corresponding to submonolayer coverages of K were suggested as a possible model of the transition from the p(2 × 2) phase, which is locally formed by potassium adsorbates at a coverage of 0.25 ML, to the ( [22,23,28,29]. Such a model can be interpreted as resulting from minimization of the electrostatic K-K repulsion [27,30] which is caused by a charge transfer to the Pt surface and, hence, by interaction between the partially charged K adatoms. In agreement with this model, K occupies the threefold symmetrical hollow adsorption site.…”
Section: Introductionmentioning
confidence: 99%