Sweta Yadav, Swati, Manish K. Niranjan, Jai Prakash
{"title":"具有复杂Te-Te相互作用的Ba16Si8Te44+δ和Ba6Si4Te6(Te3)3结构的合成与表征","authors":"Sweta Yadav, Swati, Manish K. Niranjan, Jai Prakash","doi":"10.1021/acs.inorgchem.4c04189","DOIUrl":null,"url":null,"abstract":"Multinary tellurides with complex structures and narrow bandgaps are potential candidates for thermoelectric applications. Herein, we report the syntheses of two new ternary polytellurides, Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44+δ</sub> and Ba<sub>6</sub>Si<sub>4</sub>Te<sub>6</sub>(Te<sub>3</sub>)<sub>3</sub>. Both title structures adopt unprecedented structure types. Interestingly, the Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44+δ</sub> structure shows three types of polytelluride units: Te<sub>7</sub>, Te<sub>3</sub>, and Te<sub>2</sub>. Each of the two crystallographically unique Si atoms of the structure forms a slightly distorted tetrahedral SiTe<sub>4</sub> unit. The assignment of formal charges on the atoms of the Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44+δ</sub> structure is difficult due to intermediate Te–Te interactions. The Ba<sub>6</sub>Si<sub>4</sub>Te<sub>6</sub>(Te<sub>3</sub>)<sub>3</sub> structure is also complex, including three Ba, two Si, and eight Te sites. The Si<sub>2</sub>Te<sub>6</sub> dimers and Te<sub>3</sub> trimers are the primary motifs of the Ba<sub>6</sub>Si<sub>4</sub>Te<sub>6</sub>(Te<sub>3</sub>)<sub>3</sub> structure, forming the anionic <i></i><span style=\"color: inherit;\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mfrac linethickness=\"0pt\"><mrow><mn>2</mn></mrow><mrow><mi>&#x221E;</mi></mrow></mfrac></math>' role=\"presentation\" style=\"position: relative;\" tabindex=\"0\"><nobr aria-hidden=\"true\"><span style=\"width: 1.13em; display: inline-block;\"><span style=\"display: inline-block; position: relative; width: 0.925em; height: 0px; font-size: 122%;\"><span style=\"position: absolute; clip: rect(1.13em, 1000.87em, 2.718em, -999.997em); top: -2.2em; left: 0em;\"><span><span><span style=\"display: inline-block; position: relative; width: 0.72em; height: 0px; margin-right: 0.105em; margin-left: 0.105em;\"><span style=\"position: absolute; clip: rect(3.384em, 1000.31em, 4.152em, -999.997em); top: -4.454em; left: 50%; margin-left: -0.151em;\"><span><span style=\"font-size: 70.7%; font-family: MathJax_Main;\">2</span></span><span style=\"display: inline-block; width: 0px; height: 3.998em;\"></span></span><span style=\"position: absolute; clip: rect(3.537em, 1000.67em, 4.152em, -999.997em); top: -3.635em; left: 50%; margin-left: -0.356em;\"><span><span style=\"font-size: 70.7%; font-family: MathJax_Main;\">∞</span></span><span style=\"display: inline-block; width: 0px; height: 3.998em;\"></span></span></span></span></span><span style=\"display: inline-block; width: 0px; height: 2.205em;\"></span></span></span><span style=\"display: inline-block; overflow: hidden; vertical-align: -0.497em; border-left: 0px solid; width: 0px; height: 1.691em;\"></span></span></nobr><span role=\"presentation\"><math display=\"inline\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><mfrac linethickness=\"0pt\"><mrow><mn>2</mn></mrow><mrow><mi>∞</mi></mrow></mfrac></math></span></span><script type=\"math/mml\"><math display=\"inline\"><mfrac linethickness=\"0pt\"><mrow><mn>2</mn></mrow><mrow><mi>∞</mi></mrow></mfrac></math></script>[Si<sub>4</sub>Te<sub>15</sub>]<sup>12–</sup> layers. Interestingly, the structure has two types of Te<sub>3</sub> trimers: a linear Te<sub>3</sub> unit with equidistant Te atoms and a bent Te<sub>3</sub> unit with two different Te–Te interactions. A polycrystalline Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44.2</sub> sample shows a remarkably low total thermal conductivity (<i>κ<sub>tot</sub></i>) value of 0.41 Wm<sup>–1</sup> K<sup>–1</sup> at 623 K. Interestingly, an upturn below 60 K was revealed by a resistivity study of the sample. Moreover, DFT calculations were carried out to understand the theoretical electronic structures of the phases.","PeriodicalId":40,"journal":{"name":"Inorganic Chemistry","volume":"36 1","pages":""},"PeriodicalIF":4.7000,"publicationDate":"2025-01-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Syntheses and Characterization of Ba16Si8Te44+δ and Ba6Si4Te6(Te3)3 Structures with Complex Te–Te Interactions\",\"authors\":\"Sweta Yadav, Swati, Manish K. Niranjan, Jai Prakash\",\"doi\":\"10.1021/acs.inorgchem.4c04189\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Multinary tellurides with complex structures and narrow bandgaps are potential candidates for thermoelectric applications. Herein, we report the syntheses of two new ternary polytellurides, Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44+δ</sub> and Ba<sub>6</sub>Si<sub>4</sub>Te<sub>6</sub>(Te<sub>3</sub>)<sub>3</sub>. Both title structures adopt unprecedented structure types. Interestingly, the Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44+δ</sub> structure shows three types of polytelluride units: Te<sub>7</sub>, Te<sub>3</sub>, and Te<sub>2</sub>. Each of the two crystallographically unique Si atoms of the structure forms a slightly distorted tetrahedral SiTe<sub>4</sub> unit. The assignment of formal charges on the atoms of the Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44+δ</sub> structure is difficult due to intermediate Te–Te interactions. The Ba<sub>6</sub>Si<sub>4</sub>Te<sub>6</sub>(Te<sub>3</sub>)<sub>3</sub> structure is also complex, including three Ba, two Si, and eight Te sites. The Si<sub>2</sub>Te<sub>6</sub> dimers and Te<sub>3</sub> trimers are the primary motifs of the Ba<sub>6</sub>Si<sub>4</sub>Te<sub>6</sub>(Te<sub>3</sub>)<sub>3</sub> structure, forming the anionic <i></i><span style=\\\"color: inherit;\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mfrac linethickness=\\\"0pt\\\"><mrow><mn>2</mn></mrow><mrow><mi>&#x221E;</mi></mrow></mfrac></math>' role=\\\"presentation\\\" style=\\\"position: relative;\\\" tabindex=\\\"0\\\"><nobr aria-hidden=\\\"true\\\"><span style=\\\"width: 1.13em; display: inline-block;\\\"><span style=\\\"display: inline-block; position: relative; width: 0.925em; height: 0px; font-size: 122%;\\\"><span style=\\\"position: absolute; clip: rect(1.13em, 1000.87em, 2.718em, -999.997em); top: -2.2em; left: 0em;\\\"><span><span><span style=\\\"display: inline-block; position: relative; width: 0.72em; height: 0px; margin-right: 0.105em; margin-left: 0.105em;\\\"><span style=\\\"position: absolute; clip: rect(3.384em, 1000.31em, 4.152em, -999.997em); top: -4.454em; left: 50%; margin-left: -0.151em;\\\"><span><span style=\\\"font-size: 70.7%; font-family: MathJax_Main;\\\">2</span></span><span style=\\\"display: inline-block; width: 0px; height: 3.998em;\\\"></span></span><span style=\\\"position: absolute; clip: rect(3.537em, 1000.67em, 4.152em, -999.997em); top: -3.635em; left: 50%; margin-left: -0.356em;\\\"><span><span style=\\\"font-size: 70.7%; font-family: MathJax_Main;\\\">∞</span></span><span style=\\\"display: inline-block; width: 0px; height: 3.998em;\\\"></span></span></span></span></span><span style=\\\"display: inline-block; width: 0px; height: 2.205em;\\\"></span></span></span><span style=\\\"display: inline-block; overflow: hidden; vertical-align: -0.497em; border-left: 0px solid; width: 0px; height: 1.691em;\\\"></span></span></nobr><span role=\\\"presentation\\\"><math display=\\\"inline\\\" xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mfrac linethickness=\\\"0pt\\\"><mrow><mn>2</mn></mrow><mrow><mi>∞</mi></mrow></mfrac></math></span></span><script type=\\\"math/mml\\\"><math display=\\\"inline\\\"><mfrac linethickness=\\\"0pt\\\"><mrow><mn>2</mn></mrow><mrow><mi>∞</mi></mrow></mfrac></math></script>[Si<sub>4</sub>Te<sub>15</sub>]<sup>12–</sup> layers. Interestingly, the structure has two types of Te<sub>3</sub> trimers: a linear Te<sub>3</sub> unit with equidistant Te atoms and a bent Te<sub>3</sub> unit with two different Te–Te interactions. A polycrystalline Ba<sub>16</sub>Si<sub>8</sub>Te<sub>44.2</sub> sample shows a remarkably low total thermal conductivity (<i>κ<sub>tot</sub></i>) value of 0.41 Wm<sup>–1</sup> K<sup>–1</sup> at 623 K. Interestingly, an upturn below 60 K was revealed by a resistivity study of the sample. Moreover, DFT calculations were carried out to understand the theoretical electronic structures of the phases.\",\"PeriodicalId\":40,\"journal\":{\"name\":\"Inorganic Chemistry\",\"volume\":\"36 1\",\"pages\":\"\"},\"PeriodicalIF\":4.7000,\"publicationDate\":\"2025-01-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Inorganic Chemistry\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://doi.org/10.1021/acs.inorgchem.4c04189\",\"RegionNum\":2,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"CHEMISTRY, INORGANIC & NUCLEAR\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Inorganic Chemistry","FirstCategoryId":"92","ListUrlMain":"https://doi.org/10.1021/acs.inorgchem.4c04189","RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, INORGANIC & NUCLEAR","Score":null,"Total":0}
Syntheses and Characterization of Ba16Si8Te44+δ and Ba6Si4Te6(Te3)3 Structures with Complex Te–Te Interactions
Multinary tellurides with complex structures and narrow bandgaps are potential candidates for thermoelectric applications. Herein, we report the syntheses of two new ternary polytellurides, Ba16Si8Te44+δ and Ba6Si4Te6(Te3)3. Both title structures adopt unprecedented structure types. Interestingly, the Ba16Si8Te44+δ structure shows three types of polytelluride units: Te7, Te3, and Te2. Each of the two crystallographically unique Si atoms of the structure forms a slightly distorted tetrahedral SiTe4 unit. The assignment of formal charges on the atoms of the Ba16Si8Te44+δ structure is difficult due to intermediate Te–Te interactions. The Ba6Si4Te6(Te3)3 structure is also complex, including three Ba, two Si, and eight Te sites. The Si2Te6 dimers and Te3 trimers are the primary motifs of the Ba6Si4Te6(Te3)3 structure, forming the anionic 2∞[Si4Te15]12– layers. Interestingly, the structure has two types of Te3 trimers: a linear Te3 unit with equidistant Te atoms and a bent Te3 unit with two different Te–Te interactions. A polycrystalline Ba16Si8Te44.2 sample shows a remarkably low total thermal conductivity (κtot) value of 0.41 Wm–1 K–1 at 623 K. Interestingly, an upturn below 60 K was revealed by a resistivity study of the sample. Moreover, DFT calculations were carried out to understand the theoretical electronic structures of the phases.
期刊介绍:
Inorganic Chemistry publishes fundamental studies in all phases of inorganic chemistry. Coverage includes experimental and theoretical reports on quantitative studies of structure and thermodynamics, kinetics, mechanisms of inorganic reactions, bioinorganic chemistry, and relevant aspects of organometallic chemistry, solid-state phenomena, and chemical bonding theory. Emphasis is placed on the synthesis, structure, thermodynamics, reactivity, spectroscopy, and bonding properties of significant new and known compounds.