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 Property, and Optical Nonlinearity

Density functional theory (DFT) calculations are carried out to determine the geometries and electronic and nonlinear optical (NLO) properties of the doubly doped gold clusters in three charge states M<sub>2</sub> @ Au<sub>17</sub> <sup><i>q</i></sup> with M = W, Mo and <i>q</i> = 0, ±1. At their lowest-lying equilibrium structures, the impurities that are vertically encapsulated inside a cylindrical gold framework, significantly enhance the stability and modify properties of the host. The presence of M<sub>2</sub> units results in the formation of a tube-like ground state, which is identified for the first time for gold clusters. Having 30 itinerant electrons, the electron shell of M<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 is thus stabilized upon doping, but it is not a magic cluster. The optical transitions are shifted to the lower-energy region upon doping Mo and W atoms into Au<sub>17</sub> <sup><i>q</i></sup> . The static and dynamic NLO properties of M<sub>2</sub>@Au<sub>17</sub> <sup><i>q</i></sup> are also computed and compared to those of the pure Au<sub>19</sub> <sup><i>q</i></sup> (having the same number of atoms) and an external reference molecule, i.e., para-nitroaniline (<i>p</i>-NA). For hyperpolarizabilities, the doped clusters possess smaller values than those of their pure counterparts but much larger values than the <i>p</i>-NA. Of the doubly doped systems, the neutral M<sub>2</sub>@Au<sub>17</sub> exhibits particularly high first and second hyperpolarizability tensors. The doped cluster units can also be used as building blocks for the design of gold-based nanowires with outstanding electronic and optical characteristics.

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Journal
ACS Omega
Published
2024-09-08
DOI
https://doi.org/10.1021/acsomega.4c02724
Citations
1
Primary Topic
Nanocluster Synthesis and Applications
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article
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0.12

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article

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

Minh Tho Nguyen, Minh Triết Đặng, Phạm Thị Bích Thảo, Phạm Vũ Nhật et al.
1 citations
ACS Omega
Nanocluster Synthesis and Applications
0.12
article

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

Minh Tho Nguyen, Minh Triết Đặng, Phạm Thị Bích Thảo, Phạm Vũ Nhật, Nguyen Thi Bao Trang, Trần Thị Ngọc Thảo, Nguyen Thanh
article en
1 citations

Abstract

Density functional theory (DFT) calculations are carried out to determine the geometries and electronic and nonlinear optical (NLO) properties of the doubly doped gold clusters in three charge states M<sub>2</sub> @ Au<sub>17</sub> <sup><i>q</i></sup> with M = W, Mo and <i>q</i> = 0, ±1. At their lowest-lying equilibrium structures, the impurities that are vertically encapsulated inside a cylindrical gold framework, significantly enhance the stability and modify properties of the host. The presence of M<sub>2</sub> units results in the formation of a tube-like ground state, which is identified for the first time for gold clusters. Having 30 itinerant electrons, the electron shell of M<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 is thus stabilized upon doping, but it is not a magic cluster. The optical transitions are shifted to the lower-energy region upon doping Mo and W atoms into Au<sub>17</sub> <sup><i>q</i></sup> . The static and dynamic NLO properties of M<sub>2</sub>@Au<sub>17</sub> <sup><i>q</i></sup> are also computed and compared to those of the pure Au<sub>19</sub> <sup><i>q</i></sup> (having the same number of atoms) and an external reference molecule, i.e., para-nitroaniline (<i>p</i>-NA). For hyperpolarizabilities, the doped clusters possess smaller values than those of their pure counterparts but much larger values than the <i>p</i>-NA. Of the doubly doped systems, the neutral M<sub>2</sub>@Au<sub>17</sub> exhibits particularly high first and second hyperpolarizability tensors. The doped cluster units can also be used as building blocks for the design of gold-based nanowires with outstanding electronic and optical characteristics.

ACS OmegaVol. 9(37)
Can Tho University (VN), Van Lang University (VN), Tra Vinh University (VN)
Bộ Giáo dục và Ðào tạo
Openalex Percentile: Top 60%
Nanocluster Synthesis and Applications
0.12
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