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{"title":"铁-镍-钴体系因瓦效应的原位高通量研究","authors":"Jianhao Wang, Cai Chen, Yuanxun Zhou, Zheyu Wu, Xingyu Gao, Bingbing Zhao, Lanting Zhang, Hong Wang","doi":"10.1016/j.jallcom.2024.177755","DOIUrl":null,"url":null,"abstract":"The Fe–Ni based classical Invar alloy and the Fe–Ni–Co based super Invar alloy are the basis for designing multicomponent alloys with low thermal expansion. In this work, we applied in-situ high-throughput experimental methods to map chemical composition, crystal structure, coefficient of thermal expansion (CTE) and magnetism in the Fe–Ni–Co system. The distribution of CTE (80~200℃) measured by the in-situ micro-beam X-ray diffraction on the combinatorial materials chips (CMC) showed low CTE regions in agreement with previous reports. Combined with the MOKE measurements, the <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">&#x3BC;</mi></mrow><mo is=\"true\">&#x305;</mo></mover><mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\">&#x2212;</mo><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">&#x305;</mo></mover></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.202ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -647.8 2336.1 947.9\" width=\"5.426ex\" 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\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g><g is=\"true\" transform=\"translate(108,-35)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g><g is=\"true\" transform=\"translate(825,0)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><g is=\"true\" transform=\"translate(1826,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMATHI-65\"></use></g></g><g is=\"true\" transform=\"translate(68,-34)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mo is=\"true\" linebreak=\"badbreak\" linebreakstyle=\"after\">−</mo><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></span></span><script type=\"math/mml\"><math><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mo linebreak=\"badbreak\" linebreakstyle=\"after\" is=\"true\">−</mo><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></script></span> relation of the Fe–Ni–Co ternary FCC phase is found to follow the reported FCC Fe–Ni alloys in the Slater-Pauling curve. A low CTE region is centred at <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">&#x305;</mo></mover></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.74ex\" role=\"img\" style=\"vertical-align: -0.028ex; margin-bottom: -0.208ex;\" viewbox=\"0 -647.8 509.6 749.2\" width=\"1.184ex\" 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\"><g is=\"true\"><use xlink:href=\"#MJMATHI-65\"></use></g></g><g is=\"true\" transform=\"translate(68,-34)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></span></span><script type=\"math/mml\"><math><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">e</mi></mrow><mo is=\"true\">̅</mo></mover></math></script></span> = 26.7 and <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">&#x3BC;</mi></mrow><mo is=\"true\">&#x305;</mo></mover><mspace width=\"1em\" is=\"true\" /></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.202ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -647.8 1603.5 947.9\" width=\"3.724ex\" 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\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g><g is=\"true\" transform=\"translate(108,-35)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g><g is=\"true\"></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mspace is=\"true\" width=\"1em\"></mspace></math></span></span><script type=\"math/mml\"><math><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mi is=\"true\">μ</mi></mrow><mo is=\"true\">̅</mo></mover><mspace width=\"1em\" is=\"true\"></mspace></math></script></span>= 1.26 <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">&#x3BC;</mi></mrow><mrow is=\"true\"><mi is=\"true\">B</mi></mrow></msub></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.971ex\" role=\"img\" style=\"vertical-align: -0.812ex;\" viewbox=\"0 -498.8 1240.5 848.5\" width=\"2.881ex\" 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\"><g is=\"true\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g><g is=\"true\" transform=\"translate(603,-253)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMATHI-42\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"><mi is=\"true\" mathvariant=\"italic\">μ</mi></mrow><mrow is=\"true\"><mi is=\"true\">B</mi></mrow></msub></math></span></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"><mi mathvariant=\"italic\" is=\"true\">μ</mi></mrow><mrow is=\"true\"><mi is=\"true\">B</mi></mrow></msub></math></script></span> in the Slater-Pauling curve. The observed low CTE zone not only matches with the classical Invar and super Invar alloys but also agrees with the reported Fe–Ni–Co based multicomponent alloys with a small amount of doping (< 5<!-- --> <!-- -->at.%) by Cu, Cr, Mn etc. The effect of Cr addition (> 5<!-- --> <!-- -->at.%) to Fe–Ni–Co alloys on the Invar effect is further discussed in terms of the interplay between magnetism and austinite stability.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"15 1","pages":""},"PeriodicalIF":5.8000,"publicationDate":"2024-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"An in-situ high-throughput study of the Invar effect in the Fe–Ni–Co system\",\"authors\":\"Jianhao Wang, Cai Chen, Yuanxun Zhou, Zheyu Wu, Xingyu Gao, Bingbing Zhao, Lanting Zhang, Hong Wang\",\"doi\":\"10.1016/j.jallcom.2024.177755\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The Fe–Ni based classical Invar alloy and the Fe–Ni–Co based super Invar alloy are the basis for designing multicomponent alloys with low thermal expansion. In this work, we applied in-situ high-throughput experimental methods to map chemical composition, crystal structure, coefficient of thermal expansion (CTE) and magnetism in the Fe–Ni–Co system. The distribution of CTE (80~200℃) measured by the in-situ micro-beam X-ray diffraction on the combinatorial materials chips (CMC) showed low CTE regions in agreement with previous reports. Combined with the MOKE measurements, the <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">&#x3BC;</mi></mrow><mo is=\\\"true\\\">&#x305;</mo></mover><mo linebreak=\\\"badbreak\\\" linebreakstyle=\\\"after\\\" is=\\\"true\\\">&#x2212;</mo><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">e</mi></mrow><mo is=\\\"true\\\">&#x305;</mo></mover></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.202ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.697ex;\\\" viewbox=\\\"0 -647.8 2336.1 947.9\\\" width=\\\"5.426ex\\\" 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\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-3BC\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(108,-35)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g><g is=\\\"true\\\" transform=\\\"translate(825,0)\\\"><use xlink:href=\\\"#MJMAIN-2212\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1826,0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-65\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(68,-34)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">μ</mi></mrow><mo is=\\\"true\\\">̅</mo></mover><mo is=\\\"true\\\" linebreak=\\\"badbreak\\\" linebreakstyle=\\\"after\\\">−</mo><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">e</mi></mrow><mo is=\\\"true\\\">̅</mo></mover></math></span></span><script type=\\\"math/mml\\\"><math><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">μ</mi></mrow><mo is=\\\"true\\\">̅</mo></mover><mo linebreak=\\\"badbreak\\\" linebreakstyle=\\\"after\\\" is=\\\"true\\\">−</mo><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">e</mi></mrow><mo is=\\\"true\\\">̅</mo></mover></math></script></span> relation of the Fe–Ni–Co ternary FCC phase is found to follow the reported FCC Fe–Ni alloys in the Slater-Pauling curve. A low CTE region is centred at <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">e</mi></mrow><mo is=\\\"true\\\">&#x305;</mo></mover></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.74ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.028ex; margin-bottom: -0.208ex;\\\" viewbox=\\\"0 -647.8 509.6 749.2\\\" width=\\\"1.184ex\\\" 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\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-65\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(68,-34)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">e</mi></mrow><mo is=\\\"true\\\">̅</mo></mover></math></span></span><script type=\\\"math/mml\\\"><math><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">e</mi></mrow><mo is=\\\"true\\\">̅</mo></mover></math></script></span> = 26.7 and <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">&#x3BC;</mi></mrow><mo is=\\\"true\\\">&#x305;</mo></mover><mspace width=\\\"1em\\\" is=\\\"true\\\" /></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.202ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.697ex;\\\" viewbox=\\\"0 -647.8 1603.5 947.9\\\" width=\\\"3.724ex\\\" 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\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-3BC\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(108,-35)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g><g is=\\\"true\\\"></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">μ</mi></mrow><mo is=\\\"true\\\">̅</mo></mover><mspace is=\\\"true\\\" width=\\\"1em\\\"></mspace></math></span></span><script type=\\\"math/mml\\\"><math><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">μ</mi></mrow><mo is=\\\"true\\\">̅</mo></mover><mspace width=\\\"1em\\\" is=\\\"true\\\"></mspace></math></script></span>= 1.26 <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msub is=\\\"true\\\"><mrow is=\\\"true\\\"><mi mathvariant=\\\"italic\\\" is=\\\"true\\\">&#x3BC;</mi></mrow><mrow is=\\\"true\\\"><mi is=\\\"true\\\">B</mi></mrow></msub></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.971ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.812ex;\\\" viewbox=\\\"0 -498.8 1240.5 848.5\\\" width=\\\"2.881ex\\\" 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\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMATHI-3BC\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(603,-253)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMATHI-42\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msub is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\" mathvariant=\\\"italic\\\">μ</mi></mrow><mrow is=\\\"true\\\"><mi is=\\\"true\\\">B</mi></mrow></msub></math></span></span><script type=\\\"math/mml\\\"><math><msub is=\\\"true\\\"><mrow is=\\\"true\\\"><mi mathvariant=\\\"italic\\\" is=\\\"true\\\">μ</mi></mrow><mrow is=\\\"true\\\"><mi is=\\\"true\\\">B</mi></mrow></msub></math></script></span> in the Slater-Pauling curve. The observed low CTE zone not only matches with the classical Invar and super Invar alloys but also agrees with the reported Fe–Ni–Co based multicomponent alloys with a small amount of doping (< 5<!-- --> <!-- -->at.%) by Cu, Cr, Mn etc. The effect of Cr addition (> 5<!-- --> <!-- -->at.%) to Fe–Ni–Co alloys on the Invar effect is further discussed in terms of the interplay between magnetism and austinite stability.\",\"PeriodicalId\":344,\"journal\":{\"name\":\"Journal of Alloys and Compounds\",\"volume\":\"15 1\",\"pages\":\"\"},\"PeriodicalIF\":5.8000,\"publicationDate\":\"2024-11-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Alloys and Compounds\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.1016/j.jallcom.2024.177755\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Compounds","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jallcom.2024.177755","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
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