{"title":"M (M = Sn和Ti)取代b位对双钙钛矿结构Sr2(SmNb)1-0.5xMxO6陶瓷晶体结构和微波介电性能的影响","authors":"Akinori Kan , Soma Naruse , Susumu Takahashi","doi":"10.1016/j.solidstatesciences.2025.108062","DOIUrl":null,"url":null,"abstract":"<div><div>The Sn substitution for Sm and Nb in Sr<sub>2</sub>(SmNb)<sub>1-0.5<em>x</em></sub>Sn<sub><em>x</em></sub>O<sub>6</sub> (SSNS) ceramics formed solid solutions over the whole composition range. The solubility limit of Ti substitution for Sm and Nb was <em>x</em> = 0.5 for Sr<sub>2</sub>(SmNb)<sub>1-0.5<em>x</em></sub>Ti<sub><em>x</em></sub>O<sub>6</sub> (SSNT) ceramics. Crystal structure refinement of SSNS and SSNT by the Rietveld method revealed that the crystal structure of SSNS changed from monoclinic (<em>P</em>2<sub>1</sub>/<em>n</em>) to orthorhombic (<em>Pnma</em>) at <em>x</em> ≥ 0.5, while the crystal structure of SSNT changed from monoclinic to trigonal (<em>R</em>-3) at <em>x</em> = 0.5. At <em>x</em> ≥ 0.75, SrTiO<sub>3</sub> was detected as a secondary phase in SSNT ceramics. Such changes in the symmetry of crystal structure for SSNS and SSNT by <em>M</em> substitution for Sm and Nb were also suggested by broadening of Raman peaks, which corresponds to the symmetric <em>B</em>O<sub>6</sub> stretching vibration mode. The <em>M</em> substitution for Sm and Nb leads the decrease in the quality factor (<em>Q</em>・<em>f</em>) of SSNS and SSNT ceramics; the decrease in the degree of <em>B</em>-site ordering and morphological changes in these ceramics affects the <em>Q</em>・<em>f</em> values of the ceramics in single phase region. For SSNS ceramics, the <em>Q</em>・<em>f</em> values decreased from 35,732 GHz to 14,795 GHz, with a dielectric constant (ε<sub>r</sub>) of 31.1–14.7 and the temperature coefficient of resonant frequency (<em>TCf</em>) of −55.9 to - 65.7 ppm/°C.</div></div>","PeriodicalId":432,"journal":{"name":"Solid State Sciences","volume":"169 ","pages":"Article 108062"},"PeriodicalIF":3.3000,"publicationDate":"2025-09-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Influence of M (M = Sn and Ti) substitution for B-site on crystal structure and microwave dielectric properties of double perovskite-structured Sr2(SmNb)1-0.5xMxO6 ceramics\",\"authors\":\"Akinori Kan , Soma Naruse , Susumu Takahashi\",\"doi\":\"10.1016/j.solidstatesciences.2025.108062\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>The Sn substitution for Sm and Nb in Sr<sub>2</sub>(SmNb)<sub>1-0.5<em>x</em></sub>Sn<sub><em>x</em></sub>O<sub>6</sub> (SSNS) ceramics formed solid solutions over the whole composition range. The solubility limit of Ti substitution for Sm and Nb was <em>x</em> = 0.5 for Sr<sub>2</sub>(SmNb)<sub>1-0.5<em>x</em></sub>Ti<sub><em>x</em></sub>O<sub>6</sub> (SSNT) ceramics. Crystal structure refinement of SSNS and SSNT by the Rietveld method revealed that the crystal structure of SSNS changed from monoclinic (<em>P</em>2<sub>1</sub>/<em>n</em>) to orthorhombic (<em>Pnma</em>) at <em>x</em> ≥ 0.5, while the crystal structure of SSNT changed from monoclinic to trigonal (<em>R</em>-3) at <em>x</em> = 0.5. At <em>x</em> ≥ 0.75, SrTiO<sub>3</sub> was detected as a secondary phase in SSNT ceramics. Such changes in the symmetry of crystal structure for SSNS and SSNT by <em>M</em> substitution for Sm and Nb were also suggested by broadening of Raman peaks, which corresponds to the symmetric <em>B</em>O<sub>6</sub> stretching vibration mode. The <em>M</em> substitution for Sm and Nb leads the decrease in the quality factor (<em>Q</em>・<em>f</em>) of SSNS and SSNT ceramics; the decrease in the degree of <em>B</em>-site ordering and morphological changes in these ceramics affects the <em>Q</em>・<em>f</em> values of the ceramics in single phase region. For SSNS ceramics, the <em>Q</em>・<em>f</em> values decreased from 35,732 GHz to 14,795 GHz, with a dielectric constant (ε<sub>r</sub>) of 31.1–14.7 and the temperature coefficient of resonant frequency (<em>TCf</em>) of −55.9 to - 65.7 ppm/°C.</div></div>\",\"PeriodicalId\":432,\"journal\":{\"name\":\"Solid State Sciences\",\"volume\":\"169 \",\"pages\":\"Article 108062\"},\"PeriodicalIF\":3.3000,\"publicationDate\":\"2025-09-04\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Solid State Sciences\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S1293255825002407\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, INORGANIC & NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Solid State Sciences","FirstCategoryId":"92","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1293255825002407","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, INORGANIC & NUCLEAR","Score":null,"Total":0}
Influence of M (M = Sn and Ti) substitution for B-site on crystal structure and microwave dielectric properties of double perovskite-structured Sr2(SmNb)1-0.5xMxO6 ceramics
The Sn substitution for Sm and Nb in Sr2(SmNb)1-0.5xSnxO6 (SSNS) ceramics formed solid solutions over the whole composition range. The solubility limit of Ti substitution for Sm and Nb was x = 0.5 for Sr2(SmNb)1-0.5xTixO6 (SSNT) ceramics. Crystal structure refinement of SSNS and SSNT by the Rietveld method revealed that the crystal structure of SSNS changed from monoclinic (P21/n) to orthorhombic (Pnma) at x ≥ 0.5, while the crystal structure of SSNT changed from monoclinic to trigonal (R-3) at x = 0.5. At x ≥ 0.75, SrTiO3 was detected as a secondary phase in SSNT ceramics. Such changes in the symmetry of crystal structure for SSNS and SSNT by M substitution for Sm and Nb were also suggested by broadening of Raman peaks, which corresponds to the symmetric BO6 stretching vibration mode. The M substitution for Sm and Nb leads the decrease in the quality factor (Q・f) of SSNS and SSNT ceramics; the decrease in the degree of B-site ordering and morphological changes in these ceramics affects the Q・f values of the ceramics in single phase region. For SSNS ceramics, the Q・f values decreased from 35,732 GHz to 14,795 GHz, with a dielectric constant (εr) of 31.1–14.7 and the temperature coefficient of resonant frequency (TCf) of −55.9 to - 65.7 ppm/°C.
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