{"title":"金属间体系的簇自组织:用于自组装 RbNa8Ga3As6-oP72、Sr2Ca4In3Ge6-oP56 和 Sr8Li4In4Ge8-oP24 晶体结构的簇-前体 K3、K4 和 K6","authors":"V. Ya. Shevchenko, G. D. Ilyushin","doi":"10.1134/S1087659624600273","DOIUrl":null,"url":null,"abstract":"<p>Using computer methods (the ToposPro software package), combinatorial-topological analysis and modeling of self-assembly of the following crystal structures are carried out: <b>RbNa</b><sub><b>8</b></sub><b>Ga</b><sub><b>3</b></sub><b>As</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>72</b> (<i>a</i> = 22.843Å, <i>b</i> = 4.789 <i>c</i> = 16.861 Å, <i>V</i> = 1844.6 Å<sup>3</sup>, <i>Pnma</i>), <b>Sr</b><sub><b>2</b></sub><b>Ca</b><sub><b>4</b></sub><b>In</b><sub><b>3</b></sub><b>Ge</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>56</b> (<i>a</i> = 13.243 Å, <i>b</i> = 4.460 Å, <i>c</i> = 23.505 Å, <i>V</i> = 1388.47 Å<sup>3</sup>, <i>Pnma</i>), and <b>Sr</b><sub><b>8</b></sub><b>Li</b><sub><b>4</b></sub><b>In4Ge</b><sub><b>8</b></sub><b>-</b><b><i>oP</i></b><b>24</b> (<i>a</i> = 7.503 Å, <i>b</i> = 4.619 Å, <i>c</i> = 17.473 Å, <i>V</i> = 605.6 Å<sup>3</sup>, <i>Pnma</i>). For the <b>RbNa</b><sub><b>8</b></sub><b>Ga</b><sub><b>3</b></sub><b>As</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>72</b> crystal structure, 93 variants of a cluster representation of a 3D atomic mesh with the number of structural units of 3, 4, and 6 are established. A variant of self-assembly involving three types of clusters-precursors is considered: double tetrahedra K6(4a) = 0@6 (Rb<sub>2</sub>Na<sub>2</sub>As<sub>2</sub>) and K6(4b) = 0@6 (Na<sub>4</sub>As<sub>2</sub>) with symmetry <i>g</i> = –1, tetrahedron K4(8d) = 0@4(Na<sub>3</sub>As), two triple rings K3-1 = 0@3(NaGaAs), and Ga and As spacer atoms. For the <b>Sr</b><sub><b>2</b></sub><b>Ca</b><sub><b>4</b></sub><b>In</b><sub><b>3</b></sub><b>Ge</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>56</b> crystal structure, 43 variants of a cluster representation of a 3D atomic mesh with the number of structural units of 3, 4, and 6 are established. A variant of self-assembly of a crystal structure involving three types of clusters-precursors from double tetrahedra K6(4a) = 0@6 (Sr) <sub>2</sub>In<sub>2</sub>Ge<sub>2</sub>) and K6(4b) = 0@6 (Ca<sub>2</sub>In<sub>2</sub>Ge<sub>2</sub>) with symmetry g = –1, double tetrahedra K6(4c) = 0@6 (SrCa<sub>2</sub>InGe<sub>2</sub>), and Ge2 and Ge4 spacer atoms is considered. For the <b>Sr</b><sub><b>8</b></sub><b>Li</b><sub><b>4</b></sub><b>In4Ge</b><sub><b>8</b></sub><b>-</b><b><i>oP</i></b><b>24</b> crystal structure, three variants of a cluster representation of a 3D atomic mesh with two structural units are established. A variant of the self-assembly of a crystal structure involving two types of clusters-precursors in the form of double tetrahedra K6 = (Sr<sub>2</sub>Li<sub>2</sub>Ge<sub>2</sub>) with symmetry <i>g</i> = –1 and triple rings <i>K</i>3 = 0@3 (SrInGe) is considered. The symmetry and topological code of the processes of self-assembly of 3D structures from clusters-precursors are reconstructed in the following form: primary chain → layer → framework.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 2","pages":"87 - 100"},"PeriodicalIF":0.8000,"publicationDate":"2024-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Cluster Self-Organization of Intermetallic Systems: Clusters-Precursors K3, K4, and K6 for the Self-Assembly of RbNa8Ga3As6-oP72, Sr2Ca4In3Ge6-oP56, and Sr8Li4In4Ge8-oP24 Crystal Structures\",\"authors\":\"V. Ya. Shevchenko, G. D. Ilyushin\",\"doi\":\"10.1134/S1087659624600273\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Using computer methods (the ToposPro software package), combinatorial-topological analysis and modeling of self-assembly of the following crystal structures are carried out: <b>RbNa</b><sub><b>8</b></sub><b>Ga</b><sub><b>3</b></sub><b>As</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>72</b> (<i>a</i> = 22.843Å, <i>b</i> = 4.789 <i>c</i> = 16.861 Å, <i>V</i> = 1844.6 Å<sup>3</sup>, <i>Pnma</i>), <b>Sr</b><sub><b>2</b></sub><b>Ca</b><sub><b>4</b></sub><b>In</b><sub><b>3</b></sub><b>Ge</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>56</b> (<i>a</i> = 13.243 Å, <i>b</i> = 4.460 Å, <i>c</i> = 23.505 Å, <i>V</i> = 1388.47 Å<sup>3</sup>, <i>Pnma</i>), and <b>Sr</b><sub><b>8</b></sub><b>Li</b><sub><b>4</b></sub><b>In4Ge</b><sub><b>8</b></sub><b>-</b><b><i>oP</i></b><b>24</b> (<i>a</i> = 7.503 Å, <i>b</i> = 4.619 Å, <i>c</i> = 17.473 Å, <i>V</i> = 605.6 Å<sup>3</sup>, <i>Pnma</i>). For the <b>RbNa</b><sub><b>8</b></sub><b>Ga</b><sub><b>3</b></sub><b>As</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>72</b> crystal structure, 93 variants of a cluster representation of a 3D atomic mesh with the number of structural units of 3, 4, and 6 are established. A variant of self-assembly involving three types of clusters-precursors is considered: double tetrahedra K6(4a) = 0@6 (Rb<sub>2</sub>Na<sub>2</sub>As<sub>2</sub>) and K6(4b) = 0@6 (Na<sub>4</sub>As<sub>2</sub>) with symmetry <i>g</i> = –1, tetrahedron K4(8d) = 0@4(Na<sub>3</sub>As), two triple rings K3-1 = 0@3(NaGaAs), and Ga and As spacer atoms. For the <b>Sr</b><sub><b>2</b></sub><b>Ca</b><sub><b>4</b></sub><b>In</b><sub><b>3</b></sub><b>Ge</b><sub><b>6</b></sub><b>-</b><b><i>oP</i></b><b>56</b> crystal structure, 43 variants of a cluster representation of a 3D atomic mesh with the number of structural units of 3, 4, and 6 are established. A variant of self-assembly of a crystal structure involving three types of clusters-precursors from double tetrahedra K6(4a) = 0@6 (Sr) <sub>2</sub>In<sub>2</sub>Ge<sub>2</sub>) and K6(4b) = 0@6 (Ca<sub>2</sub>In<sub>2</sub>Ge<sub>2</sub>) with symmetry g = –1, double tetrahedra K6(4c) = 0@6 (SrCa<sub>2</sub>InGe<sub>2</sub>), and Ge2 and Ge4 spacer atoms is considered. For the <b>Sr</b><sub><b>8</b></sub><b>Li</b><sub><b>4</b></sub><b>In4Ge</b><sub><b>8</b></sub><b>-</b><b><i>oP</i></b><b>24</b> crystal structure, three variants of a cluster representation of a 3D atomic mesh with two structural units are established. A variant of the self-assembly of a crystal structure involving two types of clusters-precursors in the form of double tetrahedra K6 = (Sr<sub>2</sub>Li<sub>2</sub>Ge<sub>2</sub>) with symmetry <i>g</i> = –1 and triple rings <i>K</i>3 = 0@3 (SrInGe) is considered. The symmetry and topological code of the processes of self-assembly of 3D structures from clusters-precursors are reconstructed in the following form: primary chain → layer → framework.</p>\",\"PeriodicalId\":580,\"journal\":{\"name\":\"Glass Physics and Chemistry\",\"volume\":\"50 2\",\"pages\":\"87 - 100\"},\"PeriodicalIF\":0.8000,\"publicationDate\":\"2024-09-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Glass Physics and Chemistry\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://link.springer.com/article/10.1134/S1087659624600273\",\"RegionNum\":4,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"MATERIALS SCIENCE, CERAMICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Glass Physics and Chemistry","FirstCategoryId":"88","ListUrlMain":"https://link.springer.com/article/10.1134/S1087659624600273","RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"MATERIALS SCIENCE, CERAMICS","Score":null,"Total":0}
Cluster Self-Organization of Intermetallic Systems: Clusters-Precursors K3, K4, and K6 for the Self-Assembly of RbNa8Ga3As6-oP72, Sr2Ca4In3Ge6-oP56, and Sr8Li4In4Ge8-oP24 Crystal Structures
Using computer methods (the ToposPro software package), combinatorial-topological analysis and modeling of self-assembly of the following crystal structures are carried out: RbNa8Ga3As6-oP72 (a = 22.843Å, b = 4.789 c = 16.861 Å, V = 1844.6 Å3, Pnma), Sr2Ca4In3Ge6-oP56 (a = 13.243 Å, b = 4.460 Å, c = 23.505 Å, V = 1388.47 Å3, Pnma), and Sr8Li4In4Ge8-oP24 (a = 7.503 Å, b = 4.619 Å, c = 17.473 Å, V = 605.6 Å3, Pnma). For the RbNa8Ga3As6-oP72 crystal structure, 93 variants of a cluster representation of a 3D atomic mesh with the number of structural units of 3, 4, and 6 are established. A variant of self-assembly involving three types of clusters-precursors is considered: double tetrahedra K6(4a) = 0@6 (Rb2Na2As2) and K6(4b) = 0@6 (Na4As2) with symmetry g = –1, tetrahedron K4(8d) = 0@4(Na3As), two triple rings K3-1 = 0@3(NaGaAs), and Ga and As spacer atoms. For the Sr2Ca4In3Ge6-oP56 crystal structure, 43 variants of a cluster representation of a 3D atomic mesh with the number of structural units of 3, 4, and 6 are established. A variant of self-assembly of a crystal structure involving three types of clusters-precursors from double tetrahedra K6(4a) = 0@6 (Sr) 2In2Ge2) and K6(4b) = 0@6 (Ca2In2Ge2) with symmetry g = –1, double tetrahedra K6(4c) = 0@6 (SrCa2InGe2), and Ge2 and Ge4 spacer atoms is considered. For the Sr8Li4In4Ge8-oP24 crystal structure, three variants of a cluster representation of a 3D atomic mesh with two structural units are established. A variant of the self-assembly of a crystal structure involving two types of clusters-precursors in the form of double tetrahedra K6 = (Sr2Li2Ge2) with symmetry g = –1 and triple rings K3 = 0@3 (SrInGe) is considered. The symmetry and topological code of the processes of self-assembly of 3D structures from clusters-precursors are reconstructed in the following form: primary chain → layer → framework.
期刊介绍:
Glass Physics and Chemistry presents results of research on the inorganic and physical chemistry of glass, ceramics, nanoparticles, nanocomposites, and high-temperature oxides and coatings. The journal welcomes manuscripts from all countries in the English or Russian language.