Clustering on Magnesium Surfaces – Formation and Diffusion Energies

Abstract The formation and diffusion energies of atomic clusters on Mg surfaces determine the surface roughness and formation of faulted structure, which in turn affect the mechanical deformation of Mg. This paper reports first principles density function theory (DFT) based quantum mechanics calcula...

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Main Authors: Haijian Chu, Hanchen Huang, Jian Wang
Format: Article
Language:English
Published: Nature Publishing Group 2017-07-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-017-05366-1
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spelling doaj-1ca9170762c040d7818fc415d99d4bdb2020-12-08T01:54:18ZengNature Publishing GroupScientific Reports2045-23222017-07-01711810.1038/s41598-017-05366-1Clustering on Magnesium Surfaces – Formation and Diffusion EnergiesHaijian Chu0Hanchen Huang1Jian Wang2Department of Mechanics, Shanghai UniversityDepartment of Mechanical and Industrial Engineering, Northeastern UniversityDepartment of Mechanical and Materials Engineering, University of Nebraska-LincolnAbstract The formation and diffusion energies of atomic clusters on Mg surfaces determine the surface roughness and formation of faulted structure, which in turn affect the mechanical deformation of Mg. This paper reports first principles density function theory (DFT) based quantum mechanics calculation results of atomic clustering on the low energy surfaces {0001} and $$\{\bar{1}011\}$$ { 1 ¯ 011 } . In parallel, molecular statics calculations serve to test the validity of two interatomic potentials and to extend the scope of the DFT studies. On a {0001} surface, a compact cluster consisting of few than three atoms energetically prefers a face-centered-cubic stacking, to serve as a nucleus of stacking fault. On a $$\{\bar{1}011\}$$ { 1 ¯ 011 } , clusters of any size always prefer hexagonal-close-packed stacking. Adatom diffusion on surface $$\{\bar{1}011\}$$ { 1 ¯ 011 } is high anisotropic while isotropic on surface (0001). Three-dimensional Ehrlich–Schwoebel barriers converge as the step height is three atomic layers or thicker. Adatom diffusion along steps is via hopping mechanism, and that down steps is via exchange mechanism.https://doi.org/10.1038/s41598-017-05366-1
collection DOAJ
language English
format Article
sources DOAJ
author Haijian Chu
Hanchen Huang
Jian Wang
spellingShingle Haijian Chu
Hanchen Huang
Jian Wang
Clustering on Magnesium Surfaces – Formation and Diffusion Energies
Scientific Reports
author_facet Haijian Chu
Hanchen Huang
Jian Wang
author_sort Haijian Chu
title Clustering on Magnesium Surfaces – Formation and Diffusion Energies
title_short Clustering on Magnesium Surfaces – Formation and Diffusion Energies
title_full Clustering on Magnesium Surfaces – Formation and Diffusion Energies
title_fullStr Clustering on Magnesium Surfaces – Formation and Diffusion Energies
title_full_unstemmed Clustering on Magnesium Surfaces – Formation and Diffusion Energies
title_sort clustering on magnesium surfaces – formation and diffusion energies
publisher Nature Publishing Group
series Scientific Reports
issn 2045-2322
publishDate 2017-07-01
description Abstract The formation and diffusion energies of atomic clusters on Mg surfaces determine the surface roughness and formation of faulted structure, which in turn affect the mechanical deformation of Mg. This paper reports first principles density function theory (DFT) based quantum mechanics calculation results of atomic clustering on the low energy surfaces {0001} and $$\{\bar{1}011\}$$ { 1 ¯ 011 } . In parallel, molecular statics calculations serve to test the validity of two interatomic potentials and to extend the scope of the DFT studies. On a {0001} surface, a compact cluster consisting of few than three atoms energetically prefers a face-centered-cubic stacking, to serve as a nucleus of stacking fault. On a $$\{\bar{1}011\}$$ { 1 ¯ 011 } , clusters of any size always prefer hexagonal-close-packed stacking. Adatom diffusion on surface $$\{\bar{1}011\}$$ { 1 ¯ 011 } is high anisotropic while isotropic on surface (0001). Three-dimensional Ehrlich–Schwoebel barriers converge as the step height is three atomic layers or thicker. Adatom diffusion along steps is via hopping mechanism, and that down steps is via exchange mechanism.
url https://doi.org/10.1038/s41598-017-05366-1
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AT jianwang clusteringonmagnesiumsurfacesformationanddiffusionenergies
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