{"title":"Influence of pressure-induced structural change in Al2O3–SiO2 glasses on the sound velocity and Poisson's ratio under pressure","authors":"Itaru Ohira, Yoshio Kono, Steeve Gréaux, Sayako Inoué, Nozomi M. Kondo, Sho Kakizawa, Yuji Higo, Noriyoshi Tsujino, Rostislav Hrubiak, Guoyin Shen and Atsunobu Masuno","doi":"10.1039/D6MA00275G","DOIUrl":null,"url":null,"abstract":"<p >In this study, we investigated pressure-induced changes in the structure and elastic properties of <em>x</em>Al<small><sub>2</sub></small>O<small><sub>3</sub></small>–(100 − <em>x</em>)SiO<small><sub>2</sub></small> glasses (<em>x</em> = 29, 36, 43, 50, 60 mol%; referred to as <em>x</em>AS) by <em>in situ</em> high-pressure pair distribution function measurement and sound velocity measurement. The 29AS and 60AS glasses are regarded as Si-rich/Al-rich end-member compositions, and the 36AS, 43AS, and 50AS glasses consist of the two end-member phases at the nanoscale. The 29AS glass shows gradual changes in the intermediate-range order up to 9.3 GPa, similar to SiO<small><sub>2</sub></small> glass, while the 60AS glass exhibits a rapid structural change at 7.4–8.4 GPa, similar to CaAl<small><sub>2</sub></small>O<small><sub>4</sub></small> glass. This rapid structural change causes a kink in the sound velocity–pressure trend near 8 GPa, as also observed in CaAl<small><sub>2</sub></small>O<small><sub>4</sub></small> glass. In contrast, the Si-rich end-member 29AS glass does not exhibit the velocity kink. The Poisson's ratios of the five AS glasses and the SiO<small><sub>2</sub></small> glass start to converge above ∼11 GPa, finally reaching a constant value of ∼0.32 at a pressure of ∼20 GPa. This result indicates that both the Si-rich and Al-rich end-members have a similar structure above ∼20 GPa.</p>","PeriodicalId":18242,"journal":{"name":"Materials Advances","volume":" 11","pages":" 5561-5568"},"PeriodicalIF":5.8000,"publicationDate":"2026-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2026/ma/d6ma00275g?page=search","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Materials Advances","FirstCategoryId":"1085","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2026/ma/d6ma00275g","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
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Abstract
In this study, we investigated pressure-induced changes in the structure and elastic properties of xAl2O3–(100 − x)SiO2 glasses (x = 29, 36, 43, 50, 60 mol%; referred to as xAS) by in situ high-pressure pair distribution function measurement and sound velocity measurement. The 29AS and 60AS glasses are regarded as Si-rich/Al-rich end-member compositions, and the 36AS, 43AS, and 50AS glasses consist of the two end-member phases at the nanoscale. The 29AS glass shows gradual changes in the intermediate-range order up to 9.3 GPa, similar to SiO2 glass, while the 60AS glass exhibits a rapid structural change at 7.4–8.4 GPa, similar to CaAl2O4 glass. This rapid structural change causes a kink in the sound velocity–pressure trend near 8 GPa, as also observed in CaAl2O4 glass. In contrast, the Si-rich end-member 29AS glass does not exhibit the velocity kink. The Poisson's ratios of the five AS glasses and the SiO2 glass start to converge above ∼11 GPa, finally reaching a constant value of ∼0.32 at a pressure of ∼20 GPa. This result indicates that both the Si-rich and Al-rich end-members have a similar structure above ∼20 GPa.