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Dopant-Dependent Electronic Structures Observed for M<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub> Clusters (M = Pt, Pd)

71

Citations

54

References

2018

Year

Abstract

Heteroatom doping is a powerful means to tune the optical and electronic properties of gold clusters at the atomic level. We herein report that doping a Au<sub>38</sub> cluster with Pt and Pd atoms leads to core-doped [Pt<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub>]<sup>2-</sup> and [Pd<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub>]<sup>0</sup>, respectively. Voltammetric investigations show that these clusters exhibit drastically different electronic structures; whereas the HOMO-LUMO gap of [Pt<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub>]<sup>2-</sup> is found to be 0.95 V, that of [Pd<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub>]<sup>0</sup> is drastically decreased to 0.26 V, suggesting Jahn-Teller distortion of the 12-electron cluster. Density functional investigations confirm that the HOMO-LUMO gap of the Pd-doped cluster is indeed reduced. Analysis of the optimized geometry for the 12-electron [Pd<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub>]<sup>0</sup> reveals that the rod-like M<sub>2</sub>Au<sub>21</sub> core becomes more flattened upon Pd-doping. Reversible geometrical interconversion between [Pt<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub>]<sup>0</sup> and [Pt<sub>2</sub>Au<sub>36</sub>(SC<sub>6</sub>H<sub>13</sub>)<sub>24</sub>]<sup>2-</sup> is clearly demonstrated by manipulating the oxidation state of the cluster.

References

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