Segregation of P and S Impurities to A Σ9 Grain Boundary in Cu

The segregation of P and S to grain boundaries (GBs) in fcc Cu has implications in diverse physical-chemical properties of the material and this can be of particular high relevance when the material is employed in high performance applications. Here, we studied the segregation of P and S to the symm...

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Main Authors: Cláudio M. Lousada, Pavel A. Korzhavyi
Format: Article
Language:English
Published: MDPI AG 2020-10-01
Series:Metals
Subjects:
Σ9
Online Access:https://www.mdpi.com/2075-4701/10/10/1362
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spelling doaj-776cb221e3f94801af7bb4459cffdcc12020-11-25T01:53:22ZengMDPI AGMetals2075-47012020-10-01101362136210.3390/met10101362Segregation of P and S Impurities to A Σ9 Grain Boundary in CuCláudio M. Lousada0Pavel A. Korzhavyi1Department of Materials Science and Engineering, KTH Royal Institute of Technology, SE-100 44 Stockholm, SwedenDepartment of Materials Science and Engineering, KTH Royal Institute of Technology, SE-100 44 Stockholm, SwedenThe segregation of P and S to grain boundaries (GBs) in fcc Cu has implications in diverse physical-chemical properties of the material and this can be of particular high relevance when the material is employed in high performance applications. Here, we studied the segregation of P and S to the symmetric tilt Σ9 (<inline-formula><math display="inline"><semantics><mrow><mn>2</mn><mover accent="true"><mn>2</mn><mo>¯</mo></mover><mover accent="true"><mn>1</mn><mo>¯</mo></mover></mrow></semantics></math></inline-formula>) [110], 38.9° GB of fcc Cu. This GB is characterized by a variety of segregation sites within and near the GB plane, with considerable differences in both atomic site volume and coordination number and geometry. We found that the segregation energies of P and S vary considerably both with distance from the GB plane and sites within the GB plane. The segregation energy is significantly large at the GB plane but drops to almost zero at a distance of only ≈3.5 Å from this. Additionally, for each impurity there are considerable variations in energy (up to 0.6 eV) between segregation sites in the GB plane. These variations have origins both in differences in coordination number and atomic site volume with the effect of coordination number dominating. For sites with the same coordination number, up to a certain atomic site volume, a larger atomic site volume leads to a stronger segregation. After that limit in volume has been reached, a larger volume leads to weaker segregation. The fact that the segregation energy varies with such magnitude within the Σ9 GB plane may have implications in the accumulation of these impurities at these GBs in the material. Because of this, atomic-scale variations of concentration of P and S are expected to occur at the Σ9 GB center and in other GBs with similar features.https://www.mdpi.com/2075-4701/10/10/1362grain boundariessegregationcopperdensity functional theorysigma 9Σ9
collection DOAJ
language English
format Article
sources DOAJ
author Cláudio M. Lousada
Pavel A. Korzhavyi
spellingShingle Cláudio M. Lousada
Pavel A. Korzhavyi
Segregation of P and S Impurities to A Σ9 Grain Boundary in Cu
Metals
grain boundaries
segregation
copper
density functional theory
sigma 9
Σ9
author_facet Cláudio M. Lousada
Pavel A. Korzhavyi
author_sort Cláudio M. Lousada
title Segregation of P and S Impurities to A Σ9 Grain Boundary in Cu
title_short Segregation of P and S Impurities to A Σ9 Grain Boundary in Cu
title_full Segregation of P and S Impurities to A Σ9 Grain Boundary in Cu
title_fullStr Segregation of P and S Impurities to A Σ9 Grain Boundary in Cu
title_full_unstemmed Segregation of P and S Impurities to A Σ9 Grain Boundary in Cu
title_sort segregation of p and s impurities to a σ9 grain boundary in cu
publisher MDPI AG
series Metals
issn 2075-4701
publishDate 2020-10-01
description The segregation of P and S to grain boundaries (GBs) in fcc Cu has implications in diverse physical-chemical properties of the material and this can be of particular high relevance when the material is employed in high performance applications. Here, we studied the segregation of P and S to the symmetric tilt Σ9 (<inline-formula><math display="inline"><semantics><mrow><mn>2</mn><mover accent="true"><mn>2</mn><mo>¯</mo></mover><mover accent="true"><mn>1</mn><mo>¯</mo></mover></mrow></semantics></math></inline-formula>) [110], 38.9° GB of fcc Cu. This GB is characterized by a variety of segregation sites within and near the GB plane, with considerable differences in both atomic site volume and coordination number and geometry. We found that the segregation energies of P and S vary considerably both with distance from the GB plane and sites within the GB plane. The segregation energy is significantly large at the GB plane but drops to almost zero at a distance of only ≈3.5 Å from this. Additionally, for each impurity there are considerable variations in energy (up to 0.6 eV) between segregation sites in the GB plane. These variations have origins both in differences in coordination number and atomic site volume with the effect of coordination number dominating. For sites with the same coordination number, up to a certain atomic site volume, a larger atomic site volume leads to a stronger segregation. After that limit in volume has been reached, a larger volume leads to weaker segregation. The fact that the segregation energy varies with such magnitude within the Σ9 GB plane may have implications in the accumulation of these impurities at these GBs in the material. Because of this, atomic-scale variations of concentration of P and S are expected to occur at the Σ9 GB center and in other GBs with similar features.
topic grain boundaries
segregation
copper
density functional theory
sigma 9
Σ9
url https://www.mdpi.com/2075-4701/10/10/1362
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