Hauptseite > Publikationsdatenbank > Density functional study of gold atoms and clusters on a graphite (0001) surface with defects > print |
001 | 57125 | ||
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024 | 7 | _ | |a 10.1103/PhysRevB.74.165404 |2 DOI |
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041 | _ | _ | |a eng |
082 | _ | _ | |a 530 |
084 | _ | _ | |2 WoS |a Physics, Condensed Matter |
100 | 1 | _ | |a Akola, J. |b 0 |u FZJ |0 P:(DE-Juel1)VDB6340 |
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 |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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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. |
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542 | _ | _ | |i 2006-10-06 |2 Crossref |u http://link.aps.org/licenses/aps-default-license |
588 | _ | _ | |a Dataset connected to Web of Science |
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700 | 1 | _ | |a Häkkinen, H. |b 1 |0 P:(DE-HGF)0 |
773 | 1 | 8 | |a 10.1103/physrevb.74.165404 |b American Physical Society (APS) |d 2006-10-06 |n 16 |p 165404 |3 journal-article |2 Crossref |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 |n 16 |q 74<165404 |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 |y OpenAccess |z Published final document. |
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