Probing structure, electronic property, and hydrogen adsorption for the alkali auride series

. The structural evolution, relative stability, electronic property, and hydrogen adsorption of the alkali auride series, Au n M ( n = 1 - 8 ), M = Li , Na, K, Rb, Cs), have been investigated using the density functional theory calculations at PW91 level. For the lowest-energy clusters, the dopant a...

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Veröffentlicht in:European physical journal plus 2017-04, Vol.132 (4), p.159, Article 159
Hauptverfasser: Li, Yang, Li, Yan-Fang, Tan, Jia-Jin, Jiang, Bi-Fen, OuYang, Yong-Zhong
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description . The structural evolution, relative stability, electronic property, and hydrogen adsorption of the alkali auride series, Au n M ( n = 1 - 8 ), M = Li , Na, K, Rb, Cs), have been investigated using the density functional theory calculations at PW91 level. For the lowest-energy clusters, the dopant atom M prefers to occupy a peripheral or capped site in the host, and M-induced geometries become three-dimensional more easily. The average binding energy per atom, fragmentation energy, second-order difference of energy, and HOMO-LUMO energy gap show a pronounced odd-even oscillation with the number of Au atoms, and the enhanced relative stabilities are found in Au 5 M ( M = Li , Na, K) and Au 3 M ( M = Rb , Cs) clusters. In these clusters, the H 2 molecule would like to bond with Au atom rather than impurity atom. After adsorption, the Au n M structures and H 2 molecule in all Au n M-H 2 clusters are hardly perturbed and still maintain their structural integrity. The geometrical and energetic information indicates a weak adsorption of H 2 molecule.
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The structural evolution, relative stability, electronic property, and hydrogen adsorption of the alkali auride series, Au n M ( n = 1 - 8 ), M = Li , Na, K, Rb, Cs), have been investigated using the density functional theory calculations at PW91 level. For the lowest-energy clusters, the dopant atom M prefers to occupy a peripheral or capped site in the host, and M-induced geometries become three-dimensional more easily. The average binding energy per atom, fragmentation energy, second-order difference of energy, and HOMO-LUMO energy gap show a pronounced odd-even oscillation with the number of Au atoms, and the enhanced relative stabilities are found in Au 5 M ( M = Li , Na, K) and Au 3 M ( M = Rb , Cs) clusters. In these clusters, the H 2 molecule would like to bond with Au atom rather than impurity atom. After adsorption, the Au n M structures and H 2 molecule in all Au n M-H 2 clusters are hardly perturbed and still maintain their structural integrity. 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Phys. J. Plus</addtitle><description>. The structural evolution, relative stability, electronic property, and hydrogen adsorption of the alkali auride series, Au n M ( n = 1 - 8 ), M = Li , Na, K, Rb, Cs), have been investigated using the density functional theory calculations at PW91 level. For the lowest-energy clusters, the dopant atom M prefers to occupy a peripheral or capped site in the host, and M-induced geometries become three-dimensional more easily. The average binding energy per atom, fragmentation energy, second-order difference of energy, and HOMO-LUMO energy gap show a pronounced odd-even oscillation with the number of Au atoms, and the enhanced relative stabilities are found in Au 5 M ( M = Li , Na, K) and Au 3 M ( M = Rb , Cs) clusters. In these clusters, the H 2 molecule would like to bond with Au atom rather than impurity atom. After adsorption, the Au n M structures and H 2 molecule in all Au n M-H 2 clusters are hardly perturbed and still maintain their structural integrity. 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Phys. J. Plus</stitle><date>2017-04-01</date><risdate>2017</risdate><volume>132</volume><issue>4</issue><spage>159</spage><pages>159-</pages><artnum>159</artnum><issn>2190-5444</issn><eissn>2190-5444</eissn><abstract>. The structural evolution, relative stability, electronic property, and hydrogen adsorption of the alkali auride series, Au n M ( n = 1 - 8 ), M = Li , Na, K, Rb, Cs), have been investigated using the density functional theory calculations at PW91 level. For the lowest-energy clusters, the dopant atom M prefers to occupy a peripheral or capped site in the host, and M-induced geometries become three-dimensional more easily. The average binding energy per atom, fragmentation energy, second-order difference of energy, and HOMO-LUMO energy gap show a pronounced odd-even oscillation with the number of Au atoms, and the enhanced relative stabilities are found in Au 5 M ( M = Li , Na, K) and Au 3 M ( M = Rb , Cs) clusters. 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subjects Adsorption
Applied and Technical Physics
Atomic
Atomic properties
Cesium
Clusters
Complex Systems
Condensed Matter Physics
Density functional theory
Energy gap
Hydrogen
Lithium
Mathematical and Computational Physics
Molecular
Molecular orbitals
Optical and Plasma Physics
Physics
Physics and Astronomy
Regular Article
Rubidium
Structural integrity
Structural stability
Theoretical
title Probing structure, electronic property, and hydrogen adsorption for the alkali auride series
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