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Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces

In semi-coherent interface, a superposed network of interface dislocations accommodates the attendant coherency strains in the adjacent crystals and their intersections (referred to as nodes) can act as sinks and sources for point defects because of the low formation energy. Nodes in {111} semi-cohe...

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Autores principales: Shao, Shuai, Wang, Jian, Misra, Amit, Hoagland, Richard G.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2013
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3744083/
https://www.ncbi.nlm.nih.gov/pubmed/23945821
http://dx.doi.org/10.1038/srep02448
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author Shao, Shuai
Wang, Jian
Misra, Amit
Hoagland, Richard G.
author_facet Shao, Shuai
Wang, Jian
Misra, Amit
Hoagland, Richard G.
author_sort Shao, Shuai
collection PubMed
description In semi-coherent interface, a superposed network of interface dislocations accommodates the attendant coherency strains in the adjacent crystals and their intersections (referred to as nodes) can act as sinks and sources for point defects because of the low formation energy. Nodes in {111} semi-coherent interfaces are characterized with a spiral pattern (SP), wherein the line direction of each dislocation entering a node curves. The structure of SP nodes is able to switch between condensed and expanded by either reaction with point defects or mechanical deformation. Due to the switching of the node structures, point defect formation energies at nodes can be significantly reduced. Combining atomistic simulation and dislocation theory, these features are proven universal corresponding to the node density and the character of interface dislocations.
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spelling pubmed-37440832013-08-15 Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces Shao, Shuai Wang, Jian Misra, Amit Hoagland, Richard G. Sci Rep Article In semi-coherent interface, a superposed network of interface dislocations accommodates the attendant coherency strains in the adjacent crystals and their intersections (referred to as nodes) can act as sinks and sources for point defects because of the low formation energy. Nodes in {111} semi-coherent interfaces are characterized with a spiral pattern (SP), wherein the line direction of each dislocation entering a node curves. The structure of SP nodes is able to switch between condensed and expanded by either reaction with point defects or mechanical deformation. Due to the switching of the node structures, point defect formation energies at nodes can be significantly reduced. Combining atomistic simulation and dislocation theory, these features are proven universal corresponding to the node density and the character of interface dislocations. Nature Publishing Group 2013-08-15 /pmc/articles/PMC3744083/ /pubmed/23945821 http://dx.doi.org/10.1038/srep02448 Text en Copyright © 2013, Macmillan Publishers Limited. All rights reserved http://creativecommons.org/licenses/by-nc-sa/3.0/ This work is licensed under a Creative Commons Attribution-NonCommercial-ShareALike 3.0 Unported License. To view a copy of this license, visit http://creativecommons.org/licenses/by-nc-sa/3.0/
spellingShingle Article
Shao, Shuai
Wang, Jian
Misra, Amit
Hoagland, Richard G.
Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces
title Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces
title_full Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces
title_fullStr Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces
title_full_unstemmed Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces
title_short Spiral Patterns of Dislocations at Nodes in (111) Semi-coherent FCC Interfaces
title_sort spiral patterns of dislocations at nodes in (111) semi-coherent fcc interfaces
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3744083/
https://www.ncbi.nlm.nih.gov/pubmed/23945821
http://dx.doi.org/10.1038/srep02448
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