{"title":"Structural fragility and Curie-Weiss behavior distinguishing glass forming ability in Ti-based metallic alloys","authors":"N.A. Mauro, K.F. Kelton","doi":"10.1016/j.actamat.2024.120650","DOIUrl":null,"url":null,"abstract":"The results of synchrotron x-ray scattering studies of glass forming Ti<sub>40</sub>Zr<sub>10</sub>Cu<sub>36</sub>Pd<sub>14</sub> and Ti<sub>34</sub>Zr<sub>11</sub>Cu<sub>47</sub>Ni<sub>8</sub> (Vit101) liquids and glasses are presented. Containerless experiments on the liquids were made using electrostatic levitation, while the corresponding glasses were thermally cycled to measure and account for structural relaxation. The total structure factor and total pair-distribution functions were measured as a function of temperature for the two equilibrium and supercooled Ti-based liquids, and for the corresponding glasses from room temperature to their respective glass transition temperatures. The rate of structural ordering was determined from the rate of increase in the magnitude of the first peak in the X-ray structure factors with decreasing temperature. Structural fragility is observed in these systems, with the magnitude of the fragility factor inversely correlated with the glass forming-ability. The amplitude of the first peak in the x-ray static structure factor in both alloys displays evidence for a Curie-Weiss type behavior. A proposed order parameter distinguishing glass-forming ability, <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msup is=\"true\"><mrow is=\"true\"><mo is=\"true\">(</mo><mrow is=\"true\"><mi is=\"true\">S</mi><mo is=\"true\">(</mo><mi is=\"true\">T</mi><mo is=\"true\">,</mo><msub is=\"true\"><mi is=\"true\">q</mi><mn is=\"true\">1</mn></msub><mo is=\"true\">)</mo><mo is=\"true\">&#x2212;</mo><mn is=\"true\">1</mn></mrow><mo is=\"true\">)</mo></mrow><mrow is=\"true\"><mo is=\"true\">&#x2212;</mo><mn is=\"true\">1</mn></mrow></msup></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"3.24ex\" role=\"img\" style=\"vertical-align: -0.812ex;\" viewbox=\"0 -1045.3 6981.4 1395\" width=\"16.215ex\" 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=\"#MJMAIN-28\"></use></g><g is=\"true\" transform=\"translate(389,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-53\"></use></g><g is=\"true\" transform=\"translate(645,0)\"><use xlink:href=\"#MJMAIN-28\"></use></g><g is=\"true\" transform=\"translate(1035,0)\"><use xlink:href=\"#MJMATHI-54\"></use></g><g is=\"true\" transform=\"translate(1739,0)\"><use xlink:href=\"#MJMAIN-2C\"></use></g><g is=\"true\" transform=\"translate(2184,0)\"><g is=\"true\"><use xlink:href=\"#MJMATHI-71\"></use></g><g is=\"true\" transform=\"translate(446,-150)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-31\"></use></g></g><g is=\"true\" transform=\"translate(3085,0)\"><use xlink:href=\"#MJMAIN-29\"></use></g><g is=\"true\" transform=\"translate(3696,0)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><g is=\"true\" transform=\"translate(4697,0)\"><use xlink:href=\"#MJMAIN-31\"></use></g></g><g is=\"true\" transform=\"translate(5587,0)\"><use xlink:href=\"#MJMAIN-29\"></use></g></g><g is=\"true\" transform=\"translate(5977,477)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-2212\"></use></g><g is=\"true\" transform=\"translate(550,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-31\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msup is=\"true\"><mrow is=\"true\"><mo is=\"true\">(</mo><mrow is=\"true\"><mi is=\"true\">S</mi><mo is=\"true\">(</mo><mi is=\"true\">T</mi><mo is=\"true\">,</mo><msub is=\"true\"><mi is=\"true\">q</mi><mn is=\"true\">1</mn></msub><mo is=\"true\">)</mo><mo is=\"true\">−</mo><mn is=\"true\">1</mn></mrow><mo is=\"true\">)</mo></mrow><mrow is=\"true\"><mo is=\"true\">−</mo><mn is=\"true\">1</mn></mrow></msup></math></span></span><script type=\"math/mml\"><math><msup is=\"true\"><mrow is=\"true\"><mo is=\"true\">(</mo><mrow is=\"true\"><mi is=\"true\">S</mi><mo is=\"true\">(</mo><mi is=\"true\">T</mi><mo is=\"true\">,</mo><msub is=\"true\"><mi is=\"true\">q</mi><mn is=\"true\">1</mn></msub><mo is=\"true\">)</mo><mo is=\"true\">−</mo><mn is=\"true\">1</mn></mrow><mo is=\"true\">)</mo></mrow><mrow is=\"true\"><mo is=\"true\">−</mo><mn is=\"true\">1</mn></mrow></msup></math></script></span>, shows a peak in the effective Curie temperature. This peak is at a higher temperature for the better glass former, consistent with a liquid that is closer to the ideal glass structure at a higher temperature.","PeriodicalId":238,"journal":{"name":"Acta Materialia","volume":"29 1","pages":""},"PeriodicalIF":8.3000,"publicationDate":"2024-12-14","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.2024.120650","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 results of synchrotron x-ray scattering studies of glass forming Ti40Zr10Cu36Pd14 and Ti34Zr11Cu47Ni8 (Vit101) liquids and glasses are presented. Containerless experiments on the liquids were made using electrostatic levitation, while the corresponding glasses were thermally cycled to measure and account for structural relaxation. The total structure factor and total pair-distribution functions were measured as a function of temperature for the two equilibrium and supercooled Ti-based liquids, and for the corresponding glasses from room temperature to their respective glass transition temperatures. The rate of structural ordering was determined from the rate of increase in the magnitude of the first peak in the X-ray structure factors with decreasing temperature. Structural fragility is observed in these systems, with the magnitude of the fragility factor inversely correlated with the glass forming-ability. The amplitude of the first peak in the x-ray static structure factor in both alloys displays evidence for a Curie-Weiss type behavior. A proposed order parameter distinguishing glass-forming ability, , shows a peak in the effective Curie temperature. This peak is at a higher temperature for the better glass former, consistent with a liquid that is closer to the ideal glass structure at a higher temperature.
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.