The Sm2S3-X-SmS-Sm2O2S refractory system: thermal analysis, phase diagram, and properties of the phases

Samarium monosulfide, a strain gauge and barometric material, exists in equilibrium with Sm 3 S 4 and Sm 2 O 2 S in the S-Sm–O system. Therefore, studying phase equilibria in the refractory Sm 2 S 3-X -SmS-Sm 2 O 2 S system is a scientifically interesting task. In this system, 49 samples were synthe...

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Veröffentlicht in:Journal of thermal analysis and calorimetry 2024-03, Vol.149 (5), p.2057-2073
Hauptverfasser: Yurev, Ilya Olegovich, Aleksandrovsky, Aleksandr Sergeevich, Kamaev, Dmitriy Nikolaevich, Polkovnikov, Aleksei Aleksandrovich, Grigorchenko, Viktoriya Maksimovna, Yarovenko, Aleksandr Aleksandrovich, Zelenaya, Anna Eduardovna, Parfenova, Mariya Dmitriyevna, Andreev, Oleg Valeryevich
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container_issue 5
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container_title Journal of thermal analysis and calorimetry
container_volume 149
creator Yurev, Ilya Olegovich
Aleksandrovsky, Aleksandr Sergeevich
Kamaev, Dmitriy Nikolaevich
Polkovnikov, Aleksei Aleksandrovich
Grigorchenko, Viktoriya Maksimovna
Yarovenko, Aleksandr Aleksandrovich
Zelenaya, Anna Eduardovna
Parfenova, Mariya Dmitriyevna
Andreev, Oleg Valeryevich
description Samarium monosulfide, a strain gauge and barometric material, exists in equilibrium with Sm 3 S 4 and Sm 2 O 2 S in the S-Sm–O system. Therefore, studying phase equilibria in the refractory Sm 2 S 3-X -SmS-Sm 2 O 2 S system is a scientifically interesting task. In this system, 49 samples were synthesized and studied by powder XRD, differential scanning calorimetry, visual thermal analysis, and microstructural analysis. Melting points of Sm 3 S 4 , SmS, and Sm 2 O 2 S compounds were determined. Eutectic diagrams of Sm 3 S 4 -Sm 2 O 2 S, SmS-Sm 2 O 2 S, SmS-Sm 3 S 4 systems were constructed. Temperatures and compositions of the binary eutectic points were determined. Fusion enthalpies for Sm 3 S 4 , SmS, and Sm 2 O 2 S phases were estimated using the Schröder–Le Chatelier equation. The liquidus lines were calculated using second-degree polynomials and Redlich–Kister model. Coordinates of the ternary eutectic point in the Sm 3 S 4 -SmS-Sm 2 O 2 S system were calculated using the cutting-plane method and the Scheffé method. The calculated compositions of ternary eutectic points were averaged at one most probable point, in accordance with the data on the samples microstructure. The experimental temperature of the ternary eutectic point coincides with the calculated values within the margin of error. Positions of eutectic valleys and approximate positions of isotherms in the system were established. Thermodynamic parameters of the α-Sm 2 S 3  → γ-Sm 2 S 3 polymorphic transition and the dependence of the Sm 2 S 3-X composition on heat treatment conditions were determined. According to the scanning electron microscopy data, the approximate composition of the crystallized from the melt Sm 2 S 3 sample is Sm 2 S 2.95 . The Sm 10 S 14 O phase decomposes at 1470 ± 15 °C in the course of a solid-phase reaction. The phase diagram of the Sm 2 S 3-X -Sm 2 O 2 S system was revisited. Optical band gaps of Sm 10 S 14 O and Sm 2 O 2 S phases were determined. The Sm 10 S 14 O compound was optically characterized for the first time; its direct and indirect optical bandgaps were found equal to 2.48 and 2.37 eV, respectively. The determined direct and indirect optical bandgaps of Sm 2 O 2 S (4.4 eV and 3.95 eV, respectively) agree with the earlier measurements, thus confirming the accuracy of the chosen synthesis procedures.
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Therefore, studying phase equilibria in the refractory Sm 2 S 3-X -SmS-Sm 2 O 2 S system is a scientifically interesting task. In this system, 49 samples were synthesized and studied by powder XRD, differential scanning calorimetry, visual thermal analysis, and microstructural analysis. Melting points of Sm 3 S 4 , SmS, and Sm 2 O 2 S compounds were determined. Eutectic diagrams of Sm 3 S 4 -Sm 2 O 2 S, SmS-Sm 2 O 2 S, SmS-Sm 3 S 4 systems were constructed. Temperatures and compositions of the binary eutectic points were determined. Fusion enthalpies for Sm 3 S 4 , SmS, and Sm 2 O 2 S phases were estimated using the Schröder–Le Chatelier equation. The liquidus lines were calculated using second-degree polynomials and Redlich–Kister model. Coordinates of the ternary eutectic point in the Sm 3 S 4 -SmS-Sm 2 O 2 S system were calculated using the cutting-plane method and the Scheffé method. The calculated compositions of ternary eutectic points were averaged at one most probable point, in accordance with the data on the samples microstructure. The experimental temperature of the ternary eutectic point coincides with the calculated values within the margin of error. Positions of eutectic valleys and approximate positions of isotherms in the system were established. Thermodynamic parameters of the α-Sm 2 S 3  → γ-Sm 2 S 3 polymorphic transition and the dependence of the Sm 2 S 3-X composition on heat treatment conditions were determined. According to the scanning electron microscopy data, the approximate composition of the crystallized from the melt Sm 2 S 3 sample is Sm 2 S 2.95 . The Sm 10 S 14 O phase decomposes at 1470 ± 15 °C in the course of a solid-phase reaction. The phase diagram of the Sm 2 S 3-X -Sm 2 O 2 S system was revisited. Optical band gaps of Sm 10 S 14 O and Sm 2 O 2 S phases were determined. The Sm 10 S 14 O compound was optically characterized for the first time; its direct and indirect optical bandgaps were found equal to 2.48 and 2.37 eV, respectively. The determined direct and indirect optical bandgaps of Sm 2 O 2 S (4.4 eV and 3.95 eV, respectively) agree with the earlier measurements, thus confirming the accuracy of the chosen synthesis procedures.</description><identifier>ISSN: 1388-6150</identifier><identifier>EISSN: 1588-2926</identifier><identifier>DOI: 10.1007/s10973-023-12792-z</identifier><language>eng</language><publisher>Cham: Springer International Publishing</publisher><subject>Analytical Chemistry ; Chemistry ; Chemistry and Materials Science ; Crystallization ; Energy gap ; Enthalpy ; Eutectic composition ; Eutectic temperature ; Heat treatment ; Inorganic Chemistry ; Liquidus ; Measurement Science and Instrumentation ; Melting points ; Microstructural analysis ; Microstructure ; Phase diagrams ; Phase equilibria ; Physical Chemistry ; Polymer Sciences ; Polynomials ; Samarium ; Solid phases ; Strain gauges ; Thermal analysis</subject><ispartof>Journal of thermal analysis and calorimetry, 2024-03, Vol.149 (5), p.2057-2073</ispartof><rights>Akadémiai Kiadó, Budapest, Hungary 2024. 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Therefore, studying phase equilibria in the refractory Sm 2 S 3-X -SmS-Sm 2 O 2 S system is a scientifically interesting task. In this system, 49 samples were synthesized and studied by powder XRD, differential scanning calorimetry, visual thermal analysis, and microstructural analysis. Melting points of Sm 3 S 4 , SmS, and Sm 2 O 2 S compounds were determined. Eutectic diagrams of Sm 3 S 4 -Sm 2 O 2 S, SmS-Sm 2 O 2 S, SmS-Sm 3 S 4 systems were constructed. Temperatures and compositions of the binary eutectic points were determined. Fusion enthalpies for Sm 3 S 4 , SmS, and Sm 2 O 2 S phases were estimated using the Schröder–Le Chatelier equation. The liquidus lines were calculated using second-degree polynomials and Redlich–Kister model. Coordinates of the ternary eutectic point in the Sm 3 S 4 -SmS-Sm 2 O 2 S system were calculated using the cutting-plane method and the Scheffé method. The calculated compositions of ternary eutectic points were averaged at one most probable point, in accordance with the data on the samples microstructure. The experimental temperature of the ternary eutectic point coincides with the calculated values within the margin of error. Positions of eutectic valleys and approximate positions of isotherms in the system were established. Thermodynamic parameters of the α-Sm 2 S 3  → γ-Sm 2 S 3 polymorphic transition and the dependence of the Sm 2 S 3-X composition on heat treatment conditions were determined. According to the scanning electron microscopy data, the approximate composition of the crystallized from the melt Sm 2 S 3 sample is Sm 2 S 2.95 . The Sm 10 S 14 O phase decomposes at 1470 ± 15 °C in the course of a solid-phase reaction. The phase diagram of the Sm 2 S 3-X -Sm 2 O 2 S system was revisited. Optical band gaps of Sm 10 S 14 O and Sm 2 O 2 S phases were determined. The Sm 10 S 14 O compound was optically characterized for the first time; its direct and indirect optical bandgaps were found equal to 2.48 and 2.37 eV, respectively. The determined direct and indirect optical bandgaps of Sm 2 O 2 S (4.4 eV and 3.95 eV, respectively) agree with the earlier measurements, thus confirming the accuracy of the chosen synthesis procedures.</description><subject>Analytical Chemistry</subject><subject>Chemistry</subject><subject>Chemistry and Materials Science</subject><subject>Crystallization</subject><subject>Energy gap</subject><subject>Enthalpy</subject><subject>Eutectic composition</subject><subject>Eutectic temperature</subject><subject>Heat treatment</subject><subject>Inorganic Chemistry</subject><subject>Liquidus</subject><subject>Measurement Science and Instrumentation</subject><subject>Melting points</subject><subject>Microstructural analysis</subject><subject>Microstructure</subject><subject>Phase diagrams</subject><subject>Phase equilibria</subject><subject>Physical Chemistry</subject><subject>Polymer Sciences</subject><subject>Polynomials</subject><subject>Samarium</subject><subject>Solid phases</subject><subject>Strain gauges</subject><subject>Thermal analysis</subject><issn>1388-6150</issn><issn>1588-2926</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp9UMtOwzAQtBBIlMIPcLLEtQavnTgxN1Txkir1kCJxs5zEaVM1TfCmh_TrcQkSNw77kHZmNDuE3AK_B86TBwSuE8m4kAxEogU7npEJxGnKhBbqPOwy7ApifkmuELecc605TMh6tXE0a0Qm2SfLmiyUWIqMeld5W_StHygO2LvmkfYb5xu7o3ZvdwPWOKPdxqKjZW3X3jazcChp59vO-b52SNvqRBlBeE0uKrtDd_M7p-Tj5Xk1f2OL5ev7_GnBCgm6D13riKdaWisqa5WKFKQKcu1iHYGLUq4SJUWVxxKgVDIFXegqz3XBnZIlyCm5G3WDka-Dw95s24MPjtEILRMZK0hkQIkRVfgWMfxqOl831g8GuDkFasZATQjU_ARqjoEkRxIG8H7t_J_0P6xvG-l3rg</recordid><startdate>20240301</startdate><enddate>20240301</enddate><creator>Yurev, Ilya Olegovich</creator><creator>Aleksandrovsky, Aleksandr Sergeevich</creator><creator>Kamaev, Dmitriy Nikolaevich</creator><creator>Polkovnikov, Aleksei Aleksandrovich</creator><creator>Grigorchenko, Viktoriya Maksimovna</creator><creator>Yarovenko, Aleksandr Aleksandrovich</creator><creator>Zelenaya, Anna Eduardovna</creator><creator>Parfenova, Mariya Dmitriyevna</creator><creator>Andreev, Oleg Valeryevich</creator><general>Springer International Publishing</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-3030-2259</orcidid></search><sort><creationdate>20240301</creationdate><title>The Sm2S3-X-SmS-Sm2O2S refractory system: thermal analysis, phase diagram, and properties of the phases</title><author>Yurev, Ilya Olegovich ; 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Therefore, studying phase equilibria in the refractory Sm 2 S 3-X -SmS-Sm 2 O 2 S system is a scientifically interesting task. In this system, 49 samples were synthesized and studied by powder XRD, differential scanning calorimetry, visual thermal analysis, and microstructural analysis. Melting points of Sm 3 S 4 , SmS, and Sm 2 O 2 S compounds were determined. Eutectic diagrams of Sm 3 S 4 -Sm 2 O 2 S, SmS-Sm 2 O 2 S, SmS-Sm 3 S 4 systems were constructed. Temperatures and compositions of the binary eutectic points were determined. Fusion enthalpies for Sm 3 S 4 , SmS, and Sm 2 O 2 S phases were estimated using the Schröder–Le Chatelier equation. The liquidus lines were calculated using second-degree polynomials and Redlich–Kister model. Coordinates of the ternary eutectic point in the Sm 3 S 4 -SmS-Sm 2 O 2 S system were calculated using the cutting-plane method and the Scheffé method. The calculated compositions of ternary eutectic points were averaged at one most probable point, in accordance with the data on the samples microstructure. The experimental temperature of the ternary eutectic point coincides with the calculated values within the margin of error. Positions of eutectic valleys and approximate positions of isotherms in the system were established. Thermodynamic parameters of the α-Sm 2 S 3  → γ-Sm 2 S 3 polymorphic transition and the dependence of the Sm 2 S 3-X composition on heat treatment conditions were determined. According to the scanning electron microscopy data, the approximate composition of the crystallized from the melt Sm 2 S 3 sample is Sm 2 S 2.95 . The Sm 10 S 14 O phase decomposes at 1470 ± 15 °C in the course of a solid-phase reaction. The phase diagram of the Sm 2 S 3-X -Sm 2 O 2 S system was revisited. Optical band gaps of Sm 10 S 14 O and Sm 2 O 2 S phases were determined. The Sm 10 S 14 O compound was optically characterized for the first time; its direct and indirect optical bandgaps were found equal to 2.48 and 2.37 eV, respectively. The determined direct and indirect optical bandgaps of Sm 2 O 2 S (4.4 eV and 3.95 eV, respectively) agree with the earlier measurements, thus confirming the accuracy of the chosen synthesis procedures.</abstract><cop>Cham</cop><pub>Springer International Publishing</pub><doi>10.1007/s10973-023-12792-z</doi><tpages>17</tpages><orcidid>https://orcid.org/0000-0002-3030-2259</orcidid></addata></record>
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subjects Analytical Chemistry
Chemistry
Chemistry and Materials Science
Crystallization
Energy gap
Enthalpy
Eutectic composition
Eutectic temperature
Heat treatment
Inorganic Chemistry
Liquidus
Measurement Science and Instrumentation
Melting points
Microstructural analysis
Microstructure
Phase diagrams
Phase equilibria
Physical Chemistry
Polymer Sciences
Polynomials
Samarium
Solid phases
Strain gauges
Thermal analysis
title The Sm2S3-X-SmS-Sm2O2S refractory system: thermal analysis, phase diagram, and properties of the phases
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