Ta-Re二元体系中B2相的多模态表征

IF 8.3 1区 材料科学 Q1 MATERIALS SCIENCE, MULTIDISCIPLINARY
Bryan J. Crossman, Junxin Wang, Loic Perrière, Si Athena Chen, Jean-Philippe Couzinié, Maryam Ghazisaeidi, Michael J. Mills
{"title":"Ta-Re二元体系中B2相的多模态表征","authors":"Bryan J. Crossman, Junxin Wang, Loic Perrière, Si Athena Chen, Jean-Philippe Couzinié, Maryam Ghazisaeidi, Michael J. Mills","doi":"10.1016/j.actamat.2025.121097","DOIUrl":null,"url":null,"abstract":"The energy and transportation industries demand materials that retain their mechanical property at high temperatures. Refractory complex concentrated alloys (RCCAs) with a BCC + B2 microstructure offer a potential solution, where maintaining the high temperature mechanical properties can be achieved by precipitation strengthening. This depends on the B2 phase in RCCAs being thermodynamically stable with a high solvus temperature. Recently, we predicted the high temperature stability of the B2 structure in the Ta-Re binary system, using density functional theory. Here, we provide experimental evidence for the existence of this phase for the first time, using a <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi is=\"true\"&gt;T&lt;/mi&gt;&lt;msub is=\"true\"&gt;&lt;mi is=\"true\"&gt;a&lt;/mi&gt;&lt;mn is=\"true\"&gt;65&lt;/mn&gt;&lt;/msub&gt;&lt;mi is=\"true\"&gt;R&lt;/mi&gt;&lt;msub is=\"true\"&gt;&lt;mi is=\"true\"&gt;e&lt;/mi&gt;&lt;mn is=\"true\"&gt;35&lt;/mn&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.317ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -747.2 4075.6 997.6\" width=\"9.466ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-54\"></use></g><g is=\"true\" transform=\"translate(704,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-61\"></use></g><g is=\"true\" transform=\"translate(529,-150)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-36\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-35\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(2041,0)\"><use xlink:href=\"#MJMATHI-52\"></use></g><g is=\"true\" transform=\"translate(2801,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-65\"></use></g><g is=\"true\" transform=\"translate(466,-150)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-35\" y=\"0\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mi is=\"true\">T</mi><msub is=\"true\"><mi is=\"true\">a</mi><mn is=\"true\">65</mn></msub><mi is=\"true\">R</mi><msub is=\"true\"><mi is=\"true\">e</mi><mn is=\"true\">35</mn></msub></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">T</mi><msub is=\"true\"><mi is=\"true\">a</mi><mn is=\"true\">65</mn></msub><mi is=\"true\">R</mi><msub is=\"true\"><mi is=\"true\">e</mi><mn is=\"true\">35</mn></msub></mrow></math></script></span> alloy. Despite Ta-Re binary phase diagrams predicting a single-phase BCC microstructure for <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mi is=\"true\"&gt;T&lt;/mi&gt;&lt;msub is=\"true\"&gt;&lt;mi is=\"true\"&gt;a&lt;/mi&gt;&lt;mn is=\"true\"&gt;65&lt;/mn&gt;&lt;/msub&gt;&lt;mi is=\"true\"&gt;R&lt;/mi&gt;&lt;msub is=\"true\"&gt;&lt;mi is=\"true\"&gt;e&lt;/mi&gt;&lt;mn is=\"true\"&gt;35&lt;/mn&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.317ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -747.2 4075.6 997.6\" width=\"9.466ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-54\"></use></g><g is=\"true\" transform=\"translate(704,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-61\"></use></g><g is=\"true\" transform=\"translate(529,-150)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-36\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-35\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(2041,0)\"><use xlink:href=\"#MJMATHI-52\"></use></g><g is=\"true\" transform=\"translate(2801,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-65\"></use></g><g is=\"true\" transform=\"translate(466,-150)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-35\" y=\"0\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mi is=\"true\">T</mi><msub is=\"true\"><mi is=\"true\">a</mi><mn is=\"true\">65</mn></msub><mi is=\"true\">R</mi><msub is=\"true\"><mi is=\"true\">e</mi><mn is=\"true\">35</mn></msub></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mi is=\"true\">T</mi><msub is=\"true\"><mi is=\"true\">a</mi><mn is=\"true\">65</mn></msub><mi is=\"true\">R</mi><msub is=\"true\"><mi is=\"true\">e</mi><mn is=\"true\">35</mn></msub></mrow></math></script></span>, we show that a high Z nanoscale secondary phase appears after heat treatment at 1550 °C<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mspace width=\"0.33em\" is=\"true\" /&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"0.24ex\" role=\"img\" style=\"vertical-align: -0.12ex;\" viewbox=\"0 -51.7 330 103.4\" width=\"0.766ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mspace is=\"true\" width=\"0.33em\"></mspace></math></span></span><script type=\"math/mml\"><math><mspace width=\"0.33em\" is=\"true\"></mspace></math></script></span>and 1100 °C<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mspace width=\"0.33em\" is=\"true\" /&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"0.24ex\" role=\"img\" style=\"vertical-align: -0.12ex;\" viewbox=\"0 -51.7 330 103.4\" width=\"0.766ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mspace is=\"true\" width=\"0.33em\"></mspace></math></span></span><script type=\"math/mml\"><math><mspace width=\"0.33em\" is=\"true\"></mspace></math></script></span>. Scanning transmission electron microscopy (STEM) revealed that this phase has a cubic structure and is equiatomic TaRe though B2 superlattice reflections were absent in fast Fourier transforms (FFT) and diffraction patterns (DPs). DP simulations indicate that the B2 TaRe superlattice reflections are up to two orders of magnitude weaker than their fundamental reflections, making their detection challenging via electron microscopy. Neutron diffraction confirmed the second phase had a B2 structure. This study identified a previously unobserved high temperature stable B2 phase in the Ta-Re system, enabling the development of new high temperature BCC + B2 RCCAs.","PeriodicalId":238,"journal":{"name":"Acta Materialia","volume":"26 1","pages":""},"PeriodicalIF":8.3000,"publicationDate":"2025-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Multi-Modal Characterization of the B2 Phase in the Ta-Re Binary System\",\"authors\":\"Bryan J. Crossman, Junxin Wang, Loic Perrière, Si Athena Chen, Jean-Philippe Couzinié, Maryam Ghazisaeidi, Michael J. Mills\",\"doi\":\"10.1016/j.actamat.2025.121097\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The energy and transportation industries demand materials that retain their mechanical property at high temperatures. Refractory complex concentrated alloys (RCCAs) with a BCC + B2 microstructure offer a potential solution, where maintaining the high temperature mechanical properties can be achieved by precipitation strengthening. This depends on the B2 phase in RCCAs being thermodynamically stable with a high solvus temperature. Recently, we predicted the high temperature stability of the B2 structure in the Ta-Re binary system, using density functional theory. Here, we provide experimental evidence for the existence of this phase for the first time, using a <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;T&lt;/mi&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;a&lt;/mi&gt;&lt;mn is=\\\"true\\\"&gt;65&lt;/mn&gt;&lt;/msub&gt;&lt;mi is=\\\"true\\\"&gt;R&lt;/mi&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;e&lt;/mi&gt;&lt;mn is=\\\"true\\\"&gt;35&lt;/mn&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.317ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -747.2 4075.6 997.6\\\" width=\\\"9.466ex\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g fill=\\\"currentColor\\\" stroke=\\\"currentColor\\\" stroke-width=\\\"0\\\" transform=\\\"matrix(1 0 0 -1 0 0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-54\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(704,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-61\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(529,-150)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-36\\\"></use><use transform=\\\"scale(0.707)\\\" x=\\\"500\\\" xlink:href=\\\"#MJMAIN-35\\\" y=\\\"0\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(2041,0)\\\"><use xlink:href=\\\"#MJMATHI-52\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(2801,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-65\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(466,-150)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use><use transform=\\\"scale(0.707)\\\" x=\\\"500\\\" xlink:href=\\\"#MJMAIN-35\\\" y=\\\"0\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">T</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">a</mi><mn is=\\\"true\\\">65</mn></msub><mi is=\\\"true\\\">R</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">e</mi><mn is=\\\"true\\\">35</mn></msub></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mi is=\\\"true\\\">T</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">a</mi><mn is=\\\"true\\\">65</mn></msub><mi is=\\\"true\\\">R</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">e</mi><mn is=\\\"true\\\">35</mn></msub></mrow></math></script></span> alloy. Despite Ta-Re binary phase diagrams predicting a single-phase BCC microstructure for <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;T&lt;/mi&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;a&lt;/mi&gt;&lt;mn is=\\\"true\\\"&gt;65&lt;/mn&gt;&lt;/msub&gt;&lt;mi is=\\\"true\\\"&gt;R&lt;/mi&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mi is=\\\"true\\\"&gt;e&lt;/mi&gt;&lt;mn is=\\\"true\\\"&gt;35&lt;/mn&gt;&lt;/msub&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.317ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -747.2 4075.6 997.6\\\" width=\\\"9.466ex\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g fill=\\\"currentColor\\\" stroke=\\\"currentColor\\\" stroke-width=\\\"0\\\" transform=\\\"matrix(1 0 0 -1 0 0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-54\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(704,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-61\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(529,-150)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-36\\\"></use><use transform=\\\"scale(0.707)\\\" x=\\\"500\\\" xlink:href=\\\"#MJMAIN-35\\\" y=\\\"0\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(2041,0)\\\"><use xlink:href=\\\"#MJMATHI-52\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(2801,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-65\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(466,-150)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use><use transform=\\\"scale(0.707)\\\" x=\\\"500\\\" xlink:href=\\\"#MJMAIN-35\\\" y=\\\"0\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">T</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">a</mi><mn is=\\\"true\\\">65</mn></msub><mi is=\\\"true\\\">R</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">e</mi><mn is=\\\"true\\\">35</mn></msub></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mi is=\\\"true\\\">T</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">a</mi><mn is=\\\"true\\\">65</mn></msub><mi is=\\\"true\\\">R</mi><msub is=\\\"true\\\"><mi is=\\\"true\\\">e</mi><mn is=\\\"true\\\">35</mn></msub></mrow></math></script></span>, we show that a high Z nanoscale secondary phase appears after heat treatment at 1550 °C<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mspace width=\\\"0.33em\\\" is=\\\"true\\\" /&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"0.24ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.12ex;\\\" viewbox=\\\"0 -51.7 330 103.4\\\" width=\\\"0.766ex\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g fill=\\\"currentColor\\\" stroke=\\\"currentColor\\\" stroke-width=\\\"0\\\" transform=\\\"matrix(1 0 0 -1 0 0)\\\"><g is=\\\"true\\\"></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mspace is=\\\"true\\\" width=\\\"0.33em\\\"></mspace></math></span></span><script type=\\\"math/mml\\\"><math><mspace width=\\\"0.33em\\\" is=\\\"true\\\"></mspace></math></script></span>and 1100 °C<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mspace width=\\\"0.33em\\\" is=\\\"true\\\" /&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"0.24ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.12ex;\\\" viewbox=\\\"0 -51.7 330 103.4\\\" width=\\\"0.766ex\\\" xmlns:xlink=\\\"http://www.w3.org/1999/xlink\\\"><g fill=\\\"currentColor\\\" stroke=\\\"currentColor\\\" stroke-width=\\\"0\\\" transform=\\\"matrix(1 0 0 -1 0 0)\\\"><g is=\\\"true\\\"></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mspace is=\\\"true\\\" width=\\\"0.33em\\\"></mspace></math></span></span><script type=\\\"math/mml\\\"><math><mspace width=\\\"0.33em\\\" is=\\\"true\\\"></mspace></math></script></span>. Scanning transmission electron microscopy (STEM) revealed that this phase has a cubic structure and is equiatomic TaRe though B2 superlattice reflections were absent in fast Fourier transforms (FFT) and diffraction patterns (DPs). DP simulations indicate that the B2 TaRe superlattice reflections are up to two orders of magnitude weaker than their fundamental reflections, making their detection challenging via electron microscopy. Neutron diffraction confirmed the second phase had a B2 structure. This study identified a previously unobserved high temperature stable B2 phase in the Ta-Re system, enabling the development of new high temperature BCC + B2 RCCAs.\",\"PeriodicalId\":238,\"journal\":{\"name\":\"Acta Materialia\",\"volume\":\"26 1\",\"pages\":\"\"},\"PeriodicalIF\":8.3000,\"publicationDate\":\"2025-05-01\",\"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.2025.121097\",\"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}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Acta Materialia","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.actamat.2025.121097","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

摘要

能源和运输行业需要在高温下保持其机械性能的材料。具有BCC + B2组织的难熔复合浓缩合金(RCCAs)提供了一种潜在的解决方案,通过沉淀强化可以保持高温机械性能。这取决于RCCAs中的B2相在高溶剂温度下的热力学稳定性。最近,我们利用密度泛函理论预测了Ta-Re二元体系中B2结构的高温稳定性。本文采用Ta65Re35Ta65Re35合金,首次为该相的存在提供了实验证据。尽管Ta-Re二元相图预测了Ta65Re35Ta65Re35的单相BCC微观结构,但我们发现在1550°C和1100°C热处理后出现了高Z纳米级二次相。扫描透射电子显微镜(STEM)显示该相具有立方结构和等原子TaRe,尽管在快速傅里叶变换(FFT)和衍射图(DPs)中没有B2超晶格反射。DP模拟表明,B2 TaRe超晶格反射比其基本反射弱两个数量级,这使得通过电子显微镜检测它们具有挑战性。中子衍射证实第二相具有B2结构。本研究在Ta-Re体系中发现了以前未观察到的高温稳定B2相,从而开发了新的高温BCC + B2 RCCAs。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Multi-Modal Characterization of the B2 Phase in the Ta-Re Binary System

Multi-Modal Characterization of the B2 Phase in the Ta-Re Binary System
The energy and transportation industries demand materials that retain their mechanical property at high temperatures. Refractory complex concentrated alloys (RCCAs) with a BCC + B2 microstructure offer a potential solution, where maintaining the high temperature mechanical properties can be achieved by precipitation strengthening. This depends on the B2 phase in RCCAs being thermodynamically stable with a high solvus temperature. Recently, we predicted the high temperature stability of the B2 structure in the Ta-Re binary system, using density functional theory. Here, we provide experimental evidence for the existence of this phase for the first time, using a Ta65Re35 alloy. Despite Ta-Re binary phase diagrams predicting a single-phase BCC microstructure for Ta65Re35, we show that a high Z nanoscale secondary phase appears after heat treatment at 1550 °Cand 1100 °C. Scanning transmission electron microscopy (STEM) revealed that this phase has a cubic structure and is equiatomic TaRe though B2 superlattice reflections were absent in fast Fourier transforms (FFT) and diffraction patterns (DPs). DP simulations indicate that the B2 TaRe superlattice reflections are up to two orders of magnitude weaker than their fundamental reflections, making their detection challenging via electron microscopy. Neutron diffraction confirmed the second phase had a B2 structure. This study identified a previously unobserved high temperature stable B2 phase in the Ta-Re system, enabling the development of new high temperature BCC + B2 RCCAs.
求助全文
通过发布文献求助,成功后即可免费获取论文全文。 去求助
来源期刊
Acta Materialia
Acta Materialia 工程技术-材料科学:综合
CiteScore
16.10
自引率
8.50%
发文量
801
审稿时长
53 days
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.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信