001     57125
005     20230426083239.0
024 7 _ |a 10.1103/PhysRevB.74.165404
|2 DOI
024 7 _ |a WOS:000241723700090
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024 7 _ |a 2128/7692
|2 Handle
037 _ _ |a PreJuSER-57125
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |a Akola, J.
|b 0
|u FZJ
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245 _ _ |a Density functional study of gold atoms and clusters on a graphite (0001) surface with defects
260 _ _ |a College Park, Md.
|b APS
|c 2006
300 _ _ |a 165404
336 7 _ |a Journal Article
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336 7 _ |a article
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440 _ 0 |a Physical Review B
|x 1098-0121
|0 4919
|v 74
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a Adsorption of gold atoms and clusters (N=6) on a graphite (0001) surface with defects has been studied using density functional theory. In addition to perfect graphite (0001), three types of surface defects have been considered: a surface vacancy (hole), a pyridinelike defect comprising three grouped nitrogen atoms, and a substitutional doping by N or B. Results for Au and Au-6 indicate that the surface vacancy can form chemical bonds with Au as the three nearby carbons align their dangling bonds towards the gold particle (binding energy 2.4-2.6 eV). A similar chemically saturated holelike construction with three pyridinic N atoms results in a significant polarization interaction (1.1-1.2 eV), whereas the binding with the perfect graphite surface is weak (similar to 0.3 eV). The corresponding energies for the B/N substituted surface are 0.8-1.2 eV (B) and 0.2-0.6 eV (N), and the N impurity donates charge to Au/Au-6. Several Au-6 isomers have been tested in different orientations on substrate, and the triangular gas-phase geometry (D-3h) standing on its apex is a low-energy configuration (N substitution is an exception). In general, coordination through corner atoms is energetically favorable. For the surface vacancy, the presence of gold particles leads to a significant surface reconstruction, whereas the pyridinelike defect appears rigid. There is no significant charge transfer, and the net charge on Au-6 ranges between -0.2e and 0.1e.
536 _ _ |a Kondensierte Materie
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542 _ _ |i 2006-10-06
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588 _ _ |a Dataset connected to Web of Science
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700 1 _ |a Häkkinen, H.
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773 1 8 |a 10.1103/physrevb.74.165404
|b American Physical Society (APS)
|d 2006-10-06
|n 16
|p 165404
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|t Physical Review B
|v 74
|y 2006
|x 1098-0121
773 _ _ |a 10.1103/PhysRevB.74.165404
|g Vol. 74, p. 165404
|p 165404
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|0 PERI:(DE-600)2844160-6
|t Physical review / B
|v 74
|y 2006
|x 1098-0121
856 7 _ |u http://dx.doi.org/10.1103/PhysRevB.74.165404
856 4 _ |u https://juser.fz-juelich.de/record/57125/files/FZJ-57125.pdf
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999 C 5 |y 1992
|2 Crossref
|t Physics and Chemistry of Finite Systems: From Clusters to Crystals I+II
|o Physics and Chemistry of Finite Systems: From Clusters to Crystals I+II 1992
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