4.6 Article

The size-dependent influence of palladium doping on the structures of cationic gold clusters

期刊

NANOSCALE ADVANCES
卷 3, 期 21, 页码 6197-6205

出版社

ROYAL SOC CHEMISTRY
DOI: 10.1039/d1na00587a

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资金

  1. KU Leuven Research Council [C14/18/073]
  2. Research Foundation-Flanders (FWO) [G0A0519N]
  3. EU Framework Programme for Research and Innovation HORIZON 2020 [730872]
  4. FELIX Laboratory by the Nederlandse Organisatie voor Wetenschappelijk Onderzoek (NWO)
  5. Project HPC-EUROPA3 [INFRAIA-2016-1-730897]
  6. EC Research Innovation Action under the H2020 Programme
  7. King's College London through the NMES Faculty Studentship Scheme
  8. EPSRC [EP/R029431, EP/P020194, EP/T022213]
  9. Royal Society [RG 120207]

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The physicochemical properties of small metal clusters are strongly influenced by their precise geometry. This study investigated the lowest-energy structures of Pd-doped gold clusters using experimental spectroscopy and computational modeling, revealing the significant Pd-Au interaction and the 2D to 3D transition induced by Pd doping at smaller cluster sizes than for pure gold clusters. Despite the strong interaction, recognizable cluster geometries were maintained in Pd-doped clusters up to n = 7.
The physicochemical properties of small metal clusters strongly depend on their precise geometry. Determining such geometries, however, is challenging, particularly for clusters formed by multiple elements. In this work, we combine infrared multiple photon dissociation spectroscopy and density functional theory calculations to investigate the lowest-energy structures of Pd doped gold clusters, PdAun-1+ (n <= 10). The high-quality experimental spectra allow for an unambiguous determination of the structures adopted by the clusters. Our results show that the Pd-Au interaction is so large that the structures of PdAun-1+ and Au-n(+) are very different. Pd doping induces a 2D to 3D transition at much smaller cluster sizes than for pure Au-n(+) clusters. PdAun-1+ clusters are three-dimensional from n = 4, whereas for Au-n(+) this transition only takes place at n = 7. Despite the strong Au-Pd interaction, the Au-n-1(+) cluster geometries remain recognizable in PdAun-1+ up to n = 7. This is particularly clear for PdAu6+. In PdAu8+ and PdAu9+, Pd triggers major rearrangements of the Au clusters, which adopt pyramidal shapes. For PdAu4+ we find a geometry that was not considered in previous studies, and the geometry found for PdAu8+ does not correspond to the lowest-energy structure predicted by DFT, suggesting kinetic trapping during formation. This work demonstrates that even with the continuous improvement of computational methods, unambiguous assignment of cluster geometries still requires a synergistic approach, combining experiment and computational modelling.

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