2010
DOI: 10.1039/c004229c
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On the atomic structure of thiol-protected gold nanoparticles: a combined experimental and theoretical study

Abstract: In the present work new findings on the structure of the S-Au interface are presented. Theoretical calculations using a new semiempirical potential, based on density functional theory and a bond-order Morse potential, are employed to simulate the adsorption process in a more realistic way. The simulation results reveal the formation of gold adatoms on the nanoparticle surface and high surface disorder due to the strong S-Au bond. Experimental data were acquired by aberration (Cs) corrected scanning transmissio… Show more

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Cited by 43 publications
(46 citation statements)
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“…16 Results from molecular simulations suggest that the influence of the capping molecule can also reach deeper atomic layers in gold nanoparticles smaller than 2 nm. 17,18 In the case of planar palladium, DFT calculations show that when only thiolates are adsorbed on the surface, there is no reordering of the metal atoms in the first layers; 7,13 however, when sulfide is incorporated as an adsorbate, a considerable surface reconstruction takes place. This behavior is attributed to…”
Section: −14mentioning
confidence: 99%
“…16 Results from molecular simulations suggest that the influence of the capping molecule can also reach deeper atomic layers in gold nanoparticles smaller than 2 nm. 17,18 In the case of planar palladium, DFT calculations show that when only thiolates are adsorbed on the surface, there is no reordering of the metal atoms in the first layers; 7,13 however, when sulfide is incorporated as an adsorbate, a considerable surface reconstruction takes place. This behavior is attributed to…”
Section: −14mentioning
confidence: 99%
“…Au-Au distances and isolated Au atoms are observed close to the edges of the particles, irrespective of their size (see Movies S1-S4), while isolated Au atoms are also distributed across the film. Although it is tempting to associate the rough surfaces of some of the particles with the thiol molecules (Mariscal et al, 2010;Luedtke and Landman, 1996;Kaushik and Clancy, 2012), the low atomic numbers of the atoms in the molecules and the high contrast of the C support suggest that they are not readily visible. Fig.…”
Section: Image Simulationmentioning
confidence: 99%
“…In recent years, aberration-corrected HRTEM has been successfully combined with ab initio calculations to study the binding sites and energies of single atoms on graphene (Meyer et al, 2008;Boukhvalov and Katsnelson, 2009;Cretu et al, 2010;Vanin et al, 2010;Zan et al, 2012;Ramasse et al, 2012;Wang et al, 2012aWang et al, , 2012bWang et al, , 2013Hardcastle et al, 2013), Ostwald ripening between mono-and bi-metallic nanoparticles on a-C (Yoshida et al, 2012Alloyeau et al, 2012), the diffusion of metal atoms and clusters on a-C, graphene and C nanotubes (Werner et al, 2005;Wanner et al, 2006;Batson, 2008;Gan et al, 2008;Cretu et al, 2010Cretu et al, , 2012 and the diffusion and etching of clusters on graphene (Booth et al, 2011;Wang et al,2012bWang et al, , 2013. Aberration-corrected HRTEM and density functional theory have also been used to investigate the structures of thiol-protected clusters (Mariscal et al, 2010).…”
Section: Introductionmentioning
confidence: 99%
“…Finally, temperature was reduced exponentially until it reached 0.5 K, using the Andersen thermostat with a velocity-Verlet algorithm to produce the trajectories. We have used a new interatomic potential, recently developed by Mariscal et al, 28,29 to represent the interaction between various atoms. The force-field is based on a bond-order Morse potential to represent the interaction between CO molecules and the Pd/ Au atoms.…”
Section: Computer Simulation Detailsmentioning
confidence: 99%