Relaxation Mechanisms, Structure and Properties of Semi-Coherent Interfaces

In this work, using the Cu–Ni (111) semi-coherent interface as a model system, we combine atomistic simulations and defect theory to reveal the relaxation mechanisms, structure, and properties of semi-coherent interfaces. By calculating the generalized stacking fault energy (GSFE) profile of the int...

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Main Authors: Shuai Shao, Jian Wang
Format: Article
Language:English
Published: MDPI AG 2015-10-01
Series:Metals
Subjects:
Online Access:http://www.mdpi.com/2075-4701/5/4/1887
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spelling doaj-8e49b2f2a31943adb439a907adb3205b2020-11-24T23:48:38ZengMDPI AGMetals2075-47012015-10-01541887190110.3390/met5041887met5041887Relaxation Mechanisms, Structure and Properties of Semi-Coherent InterfacesShuai Shao0Jian Wang1Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, NM 87545, USAMaterials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, NM 87545, USAIn this work, using the Cu–Ni (111) semi-coherent interface as a model system, we combine atomistic simulations and defect theory to reveal the relaxation mechanisms, structure, and properties of semi-coherent interfaces. By calculating the generalized stacking fault energy (GSFE) profile of the interface, two stable structures and a high-energy structure are located. During the relaxation, the regions that possess the stable structures expand and develop into coherent regions; the regions with high-energy structure shrink into the intersection of misfit dislocations (nodes). This process reduces the interface excess potential energy but increases the core energy of the misfit dislocations and nodes. The core width is dependent on the GSFE of the interface. The high-energy structure relaxes by relative rotation and dilatation between the crystals. The relative rotation is responsible for the spiral pattern at nodes. The relative dilatation is responsible for the creation of free volume at nodes, which facilitates the nodes’ structural transformation. Several node structures have been observed and analyzed. The various structures have significant impact on the plastic deformation in terms of lattice dislocation nucleation, as well as the point defect formation energies.http://www.mdpi.com/2075-4701/5/4/1887atomistic simulationsdislocationinterface structurenucleationnodesface-centered-cubic crystals
collection DOAJ
language English
format Article
sources DOAJ
author Shuai Shao
Jian Wang
spellingShingle Shuai Shao
Jian Wang
Relaxation Mechanisms, Structure and Properties of Semi-Coherent Interfaces
Metals
atomistic simulations
dislocation
interface structure
nucleation
nodes
face-centered-cubic crystals
author_facet Shuai Shao
Jian Wang
author_sort Shuai Shao
title Relaxation Mechanisms, Structure and Properties of Semi-Coherent Interfaces
title_short Relaxation Mechanisms, Structure and Properties of Semi-Coherent Interfaces
title_full Relaxation Mechanisms, Structure and Properties of Semi-Coherent Interfaces
title_fullStr Relaxation Mechanisms, Structure and Properties of Semi-Coherent Interfaces
title_full_unstemmed Relaxation Mechanisms, Structure and Properties of Semi-Coherent Interfaces
title_sort relaxation mechanisms, structure and properties of semi-coherent interfaces
publisher MDPI AG
series Metals
issn 2075-4701
publishDate 2015-10-01
description In this work, using the Cu–Ni (111) semi-coherent interface as a model system, we combine atomistic simulations and defect theory to reveal the relaxation mechanisms, structure, and properties of semi-coherent interfaces. By calculating the generalized stacking fault energy (GSFE) profile of the interface, two stable structures and a high-energy structure are located. During the relaxation, the regions that possess the stable structures expand and develop into coherent regions; the regions with high-energy structure shrink into the intersection of misfit dislocations (nodes). This process reduces the interface excess potential energy but increases the core energy of the misfit dislocations and nodes. The core width is dependent on the GSFE of the interface. The high-energy structure relaxes by relative rotation and dilatation between the crystals. The relative rotation is responsible for the spiral pattern at nodes. The relative dilatation is responsible for the creation of free volume at nodes, which facilitates the nodes’ structural transformation. Several node structures have been observed and analyzed. The various structures have significant impact on the plastic deformation in terms of lattice dislocation nucleation, as well as the point defect formation energies.
topic atomistic simulations
dislocation
interface structure
nucleation
nodes
face-centered-cubic crystals
url http://www.mdpi.com/2075-4701/5/4/1887
work_keys_str_mv AT shuaishao relaxationmechanismsstructureandpropertiesofsemicoherentinterfaces
AT jianwang relaxationmechanismsstructureandpropertiesofsemicoherentinterfaces
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