{"title":"Effects of Y solutes on the activation of the {112̄1}〈1̄1̄26〉 deformation twinning in MgY solid solution alloys","authors":"Jianwei Xiao, Junjie Gao, Songwei Li, Rui Wang, Chuang Deng, Yuntian Zhu, Zhaoxuan Wu","doi":"10.1016/j.actamat.2024.120648","DOIUrl":null,"url":null,"abstract":"The <span><math><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">〈</mo><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">2</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">6</mn><mo is=\"true\">〉</mo></mrow></mrow></math></span> deformation twin is common in nominally pure HCP Ti, Zr, Re, Co, but not in Mg. Rare-earth (RE) solutes such as Y and Gd at low atomic concentrations, however, can activate this twin mode and make it competitive to the regular <span><math><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">2</mn><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">〈</mo><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mo is=\"true\">〉</mo></mrow></mrow></math></span> extension twin in Mg. Previously models have not explicitly revealed the role of RE solutes on twinning and the RE-effects remain poorly understood. Using a reduced-constraint (RC) slip path, DFT calculations and two newly-developed interatomic potentials for MgY and MgAl, we reveal the physical origin of the RE solute effects in activating the <span><math><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">〈</mo><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">2</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">6</mn><mo is=\"true\">〉</mo></mrow></mrow></math></span> twin in MgY alloys with random and short range order solute states. The RC-path shows that localized slip in the <span><math><mrow is=\"true\"><mo is=\"true\">〈</mo><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">2</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">6</mn><mo is=\"true\">〉</mo></mrow></math></span> twinning direction simultaneously drives shear and <span><math><mrow is=\"true\"><mo is=\"true\">〈</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mo is=\"true\">〉</mo></mrow></math></span>-direction shuffle displacements on the corrugated <span><math><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mo is=\"true\">}</mo></mrow></math></span> twinning plane. The shuffle displacements are essential to reverse the asymmetry of <span><math><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mo is=\"true\">}</mo></mrow></math></span> atom-planes to satisfy the twin symmetry. However, such shuffle displacements are insufficient in pure Mg or MgAl, leaving twin nucleation to the multi-layer slip path with high energy barriers. Y-solutes are able to enhance the slip-driven shuffling to levels sufficient to reverse the <span><math><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mo is=\"true\">}</mo></mrow></math></span> atom-planes asymmetry, leading to spontaneous nucleation of multi-layer twin embryo with reduced energy barriers lower than that for the competing <span><math><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">2</mn><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">〈</mo><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">0</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mo is=\"true\">〉</mo></mrow></mrow></math></span> extension twin in Mg. The RC-slip path and <span><math><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">1</mn><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">〈</mo><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mover accent=\"false\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">1</mn></mrow><mo accent=\"true\" is=\"true\">¯</mo></mover><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">2</mn><mspace is=\"true\" width=\"0.16667em\"></mspace><mn is=\"true\">6</mn><mo is=\"true\">〉</mo></mrow></mrow></math></span> twin nucleation is directly demonstrated in atomistic simulations of a blunted cracks under mode-II loading. This slip driven, solute-modulated twin nucleation mechanism is expected to be general across all HCP metals and alloys.","PeriodicalId":238,"journal":{"name":"Acta Materialia","volume":"27 1","pages":""},"PeriodicalIF":8.3000,"publicationDate":"2024-12-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta Materialia","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.actamat.2024.120648","RegionNum":1,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
The deformation twin is common in nominally pure HCP Ti, Zr, Re, Co, but not in Mg. Rare-earth (RE) solutes such as Y and Gd at low atomic concentrations, however, can activate this twin mode and make it competitive to the regular extension twin in Mg. Previously models have not explicitly revealed the role of RE solutes on twinning and the RE-effects remain poorly understood. Using a reduced-constraint (RC) slip path, DFT calculations and two newly-developed interatomic potentials for MgY and MgAl, we reveal the physical origin of the RE solute effects in activating the twin in MgY alloys with random and short range order solute states. The RC-path shows that localized slip in the twinning direction simultaneously drives shear and -direction shuffle displacements on the corrugated twinning plane. The shuffle displacements are essential to reverse the asymmetry of atom-planes to satisfy the twin symmetry. However, such shuffle displacements are insufficient in pure Mg or MgAl, leaving twin nucleation to the multi-layer slip path with high energy barriers. Y-solutes are able to enhance the slip-driven shuffling to levels sufficient to reverse the atom-planes asymmetry, leading to spontaneous nucleation of multi-layer twin embryo with reduced energy barriers lower than that for the competing extension twin in Mg. The RC-slip path and twin nucleation is directly demonstrated in atomistic simulations of a blunted cracks under mode-II loading. This slip driven, solute-modulated twin nucleation mechanism is expected to be general across all HCP metals and alloys.
期刊介绍:
Acta Materialia serves as a platform for publishing full-length, original papers and commissioned overviews that contribute to a profound understanding of the correlation between the processing, structure, and properties of inorganic materials. The journal seeks papers with high impact potential or those that significantly propel the field forward. The scope includes the atomic and molecular arrangements, chemical and electronic structures, and microstructure of materials, focusing on their mechanical or functional behavior across all length scales, including nanostructures.