O. B. Tsiok, V. V. Brazhkin, E. Bychkov, A. S. Tverjanovich
{"title":"P, t相图上As2S3的玻璃化过渡线直至熔体的金属化压力","authors":"O. B. Tsiok, V. V. Brazhkin, E. Bychkov, A. S. Tverjanovich","doi":"10.1134/S0021364025606633","DOIUrl":null,"url":null,"abstract":"<p>An inelastic behavior is observed in the form of diffuse structural transformations with complex logarithmic kinetics in most chalcogenide glasses compressed above pressures of 1–1.5 GPa. The corresponding melts also exhibit a change in the structure of the intermediate- and short-range orders usually in the pressure range from 1 to 10 GPa. At the same time, the glass transition temperature <i>T</i><sub>g</sub> for chalcogenide systems at pressures above 1 GPa has not yet been studied. In this work, the glass transition in the “classical” glass-forming compound As<sub>2</sub>S<sub>3</sub> has been studied for the first time at a high hydrostatic pressure up to 5 GPa, i.e., in the range where diffuse transformations and growth of chemical disorder in glass and in melt are observed. At higher pressures, smooth metallization and chemical disproportion of the melt begins, and glasses are not formed during cooling. The initial slope <i>dT</i><sub>g</sub>/<i>dP</i> of the glass transition line agrees well with the estimate from the Prigogine–Defay thermodynamic relations. The glass transition line has a large curvature, sharply flattens under compression up to a pressure of 3 GPa, and then becomes almost straight. The ratio of the glass transition temperature to the melting point <i>T</i><sub>g</sub>/<i>T</i><sub>m</sub> for As<sub>2</sub>S<sub>3</sub> decreases from 0.8 to 0.6 with increasing pressure to 5 GPa, which indicates a drastic decrease in the tendency to glass formation under compression. A possible relationship between the features of the glass transition line and transformations in melt and glass at the corresponding pressures has been discussed.</p>","PeriodicalId":604,"journal":{"name":"JETP Letters","volume":"121 11","pages":"859 - 863"},"PeriodicalIF":1.3000,"publicationDate":"2025-07-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1134/S0021364025606633.pdf","citationCount":"0","resultStr":"{\"title\":\"Glass Transition Line of As2S3 on the P, T-Phase Diagram up to the Metallization Pressures of the Melt\",\"authors\":\"O. B. Tsiok, V. V. Brazhkin, E. Bychkov, A. S. Tverjanovich\",\"doi\":\"10.1134/S0021364025606633\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>An inelastic behavior is observed in the form of diffuse structural transformations with complex logarithmic kinetics in most chalcogenide glasses compressed above pressures of 1–1.5 GPa. The corresponding melts also exhibit a change in the structure of the intermediate- and short-range orders usually in the pressure range from 1 to 10 GPa. At the same time, the glass transition temperature <i>T</i><sub>g</sub> for chalcogenide systems at pressures above 1 GPa has not yet been studied. In this work, the glass transition in the “classical” glass-forming compound As<sub>2</sub>S<sub>3</sub> has been studied for the first time at a high hydrostatic pressure up to 5 GPa, i.e., in the range where diffuse transformations and growth of chemical disorder in glass and in melt are observed. At higher pressures, smooth metallization and chemical disproportion of the melt begins, and glasses are not formed during cooling. The initial slope <i>dT</i><sub>g</sub>/<i>dP</i> of the glass transition line agrees well with the estimate from the Prigogine–Defay thermodynamic relations. The glass transition line has a large curvature, sharply flattens under compression up to a pressure of 3 GPa, and then becomes almost straight. The ratio of the glass transition temperature to the melting point <i>T</i><sub>g</sub>/<i>T</i><sub>m</sub> for As<sub>2</sub>S<sub>3</sub> decreases from 0.8 to 0.6 with increasing pressure to 5 GPa, which indicates a drastic decrease in the tendency to glass formation under compression. A possible relationship between the features of the glass transition line and transformations in melt and glass at the corresponding pressures has been discussed.</p>\",\"PeriodicalId\":604,\"journal\":{\"name\":\"JETP Letters\",\"volume\":\"121 11\",\"pages\":\"859 - 863\"},\"PeriodicalIF\":1.3000,\"publicationDate\":\"2025-07-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1134/S0021364025606633.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"JETP Letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1134/S0021364025606633\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"JETP Letters","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S0021364025606633","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Glass Transition Line of As2S3 on the P, T-Phase Diagram up to the Metallization Pressures of the Melt
An inelastic behavior is observed in the form of diffuse structural transformations with complex logarithmic kinetics in most chalcogenide glasses compressed above pressures of 1–1.5 GPa. The corresponding melts also exhibit a change in the structure of the intermediate- and short-range orders usually in the pressure range from 1 to 10 GPa. At the same time, the glass transition temperature Tg for chalcogenide systems at pressures above 1 GPa has not yet been studied. In this work, the glass transition in the “classical” glass-forming compound As2S3 has been studied for the first time at a high hydrostatic pressure up to 5 GPa, i.e., in the range where diffuse transformations and growth of chemical disorder in glass and in melt are observed. At higher pressures, smooth metallization and chemical disproportion of the melt begins, and glasses are not formed during cooling. The initial slope dTg/dP of the glass transition line agrees well with the estimate from the Prigogine–Defay thermodynamic relations. The glass transition line has a large curvature, sharply flattens under compression up to a pressure of 3 GPa, and then becomes almost straight. The ratio of the glass transition temperature to the melting point Tg/Tm for As2S3 decreases from 0.8 to 0.6 with increasing pressure to 5 GPa, which indicates a drastic decrease in the tendency to glass formation under compression. A possible relationship between the features of the glass transition line and transformations in melt and glass at the corresponding pressures has been discussed.
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