Tube-like Gold Clusters M<sub>2</sub>@Au<sub>17</sub><sup><i>q</i></sup> (M = W, Mo; <i>q</i> = 0, ±1): Structure, Electronic\nProperty, and Optical Nonlinearity

Density functional\ntheory (DFT) calculations are carried out to\ndetermine the geometries and electronic and nonlinear optical (NLO)\nproperties of the doubly doped gold clusters in three charge states\nM<sub>2</sub> @ Au<sub>17</sub><sup><i>q</i></sup> with M = W, Mo and <i>q</i> =\n0, ±1. At their lowest-lying equilibrium structures, the impurities\nthat are vertically encapsulated inside a cylindrical gold framework,\nsignificantly enhance the stability and modify properties of the host.\nThe presence of M<sub>2</sub> units results in the formation of a\ntube-like ground state, which is identified for the first time for\ngold clusters. Having 30 itinerant electrons, the electron shell of\nM<sub>2</sub>@Au<sub>17</sub><sup>–</sup> can be described as 1S<sup>2</sup>1P<sup>6</sup>1D<sup>10</sup>2S<sup>2</sup>{1F<sub><i>xz</i><sup>2</sup></sub><sup>2</sup>1F<sub><i>yz</i><sup>2</sup></sub><sup>2</sup>}1F<sub><i>z</i><sup>3</sup></sub><sup>2</sup>{1F<sub><i>xyz</i></sub><sup>2</sup>1F<sub><i>z</i>(<i>x</i><sup>2</sup>–<i>y</i><sup>2</sup>)</sub><sup>2</sup>}{1F<sub><i>y</i>(3<i>x</i><sup>2</sup><i>–y</i><sup>2</sup>)</sub>,1F<sub><i>x</i>(<i>x</i><sup>2</sup><i>–</i>3<i>y</i><sup>2</sup>)</sub>}. The species\nis thus stabilized upon doping, but it is not a magic cluster. The\noptical transitions are shifted to the lower-energy region upon doping\nMo and W atoms into Au<sub>17</sub><sup><i>q</i></sup>. The static and dynamic NLO properties of\nM<sub>2</sub>@Au<sub>17</sub><sup><i>q</i></sup> are also computed and compared to those\nof the pure Au<sub>19</sub><sup><i>q</i></sup> (having the same number of atoms) and an external\nreference molecule, i.e., para-nitroaniline (<i>p</i>-NA).\nFor hyperpolarizabilities, the doped clusters possess smaller values\nthan those of their pure counterparts but much larger values than\nthe <i>p</i>-NA. Of the doubly doped systems, the neutral\nM<sub>2</sub>@Au<sub>17</sub> exhibits particularly high first and\nsecond hyperpolarizability tensors. The doped cluster units can also\nbe used as building blocks for the design of gold-based nanowires\nwith outstanding electronic and optical characteristics.

Publication Details

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Figshare
Published
2024-09-08
DOI
https://doi.org/10.1021/acsomega.4c02724.s001
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Biomedical and Chemical Research
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article

Tube-like Gold Clusters M2@Au17q (M = W, Mo; q = 0, ±1): Structure, Electronic\nProperty, and Optical Nonlinearity

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Biomedical and Chemical Research
article

Tube-like Gold Clusters M2@Au17q (M = W, Mo; q = 0, ±1): Structure, Electronic\nProperty, and Optical Nonlinearity

article en

Abstract

Density functional\ntheory (DFT) calculations are carried out to\ndetermine the geometries and electronic and nonlinear optical (NLO)\nproperties of the doubly doped gold clusters in three charge states\nM<sub>2</sub> @ Au<sub>17</sub><sup><i>q</i></sup> with M = W, Mo and <i>q</i> =\n0, ±1. At their lowest-lying equilibrium structures, the impurities\nthat are vertically encapsulated inside a cylindrical gold framework,\nsignificantly enhance the stability and modify properties of the host.\nThe presence of M<sub>2</sub> units results in the formation of a\ntube-like ground state, which is identified for the first time for\ngold clusters. Having 30 itinerant electrons, the electron shell of\nM<sub>2</sub>@Au<sub>17</sub><sup>–</sup> can be described as 1S<sup>2</sup>1P<sup>6</sup>1D<sup>10</sup>2S<sup>2</sup>{1F<sub><i>xz</i><sup>2</sup></sub><sup>2</sup>1F<sub><i>yz</i><sup>2</sup></sub><sup>2</sup>}1F<sub><i>z</i><sup>3</sup></sub><sup>2</sup>{1F<sub><i>xyz</i></sub><sup>2</sup>1F<sub><i>z</i>(<i>x</i><sup>2</sup>–<i>y</i><sup>2</sup>)</sub><sup>2</sup>}{1F<sub><i>y</i>(3<i>x</i><sup>2</sup><i>–y</i><sup>2</sup>)</sub>,1F<sub><i>x</i>(<i>x</i><sup>2</sup><i>–</i>3<i>y</i><sup>2</sup>)</sub>}. The species\nis thus stabilized upon doping, but it is not a magic cluster. The\noptical transitions are shifted to the lower-energy region upon doping\nMo and W atoms into Au<sub>17</sub><sup><i>q</i></sup>. The static and dynamic NLO properties of\nM<sub>2</sub>@Au<sub>17</sub><sup><i>q</i></sup> are also computed and compared to those\nof the pure Au<sub>19</sub><sup><i>q</i></sup> (having the same number of atoms) and an external\nreference molecule, i.e., para-nitroaniline (<i>p</i>-NA).\nFor hyperpolarizabilities, the doped clusters possess smaller values\nthan those of their pure counterparts but much larger values than\nthe <i>p</i>-NA. Of the doubly doped systems, the neutral\nM<sub>2</sub>@Au<sub>17</sub> exhibits particularly high first and\nsecond hyperpolarizability tensors. The doped cluster units can also\nbe used as building blocks for the design of gold-based nanowires\nwith outstanding electronic and optical characteristics.

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