{"title":"金属间体系的簇自组织:用于自组装晶体结构 Pu31Rh20-tI204、Pu20Os12-tI32、(Pu4Co)2(Pu4)-tI28、(Ti4Ni)2(Bi4)-tI28 和 Bi4-tI8 的簇-前体 K15、K6、K5 和 K4","authors":"V. Ya. Shevchenko, G. D. Ilyushin","doi":"10.1134/S1087659623600692","DOIUrl":null,"url":null,"abstract":"<p>Using the ToposPro software package, a combinatorial-topological analysis and modeling of the self-assembly of the following crystal structures with space group <i>I</i>4/<i>mcm</i> are realized: Pu<sub>31</sub>Rh<sub>20</sub>-<i>tI</i>204: <i>a</i> = 11.076 Å, <i>c</i> = 36.933 Å, <i>V</i> = 4530.86 Å<sup>3</sup>, Pu<sub>20</sub>Os<sub>12</sub>-<i>tI</i>32: <i>a</i> = 10.882 Å, <i>c</i> = 5.665 Å, <i>V</i> = 670.8 Å<sup>3</sup>. (Pu<sub>4</sub>Co)<sub>2</sub> (Pu<sub>4</sub>)-<i>tI</i>28: <i>a</i> = 10.475 Å, <i>c</i> = 5.340 Å, <i>V</i> = 585.9Å<sup>3</sup>. (Ti<sub>4</sub>Ni)<sub>2</sub>(Bi4)-<i>tI</i>28: <i>a</i> = 10.554 Å, <i>c</i> = 4.814 Å, <i>V</i> = 536.2Å<sup>3</sup>, Bi<sub>4</sub>-<i>tI</i>8: <i>a</i> = 8.518 Å, <i>c</i> = 4.164 Å, <i>V</i> = 302.15 Å<sup>3</sup>. For the crystal structure of Pu<sub>31</sub>Rh<sub>20</sub>-<i>tI</i>204, 113 variants of the cluster representation of the 3<i>D</i> atomic network with the following number of structural units are established: 4 (14 variants), 5 (61 variants), and 6 (38 variants). A variant of the self-assembly of the crystal structure with the participation of three types of framework-forming polyhedra is considered: <i>K</i>15 = Pu@14(Rh<sub>2</sub>Pu<sub>5</sub>)<sub>2</sub> with symmetry –42<i>m</i>, double pyramids <i>K</i>10 = (Rh@Pu<sub>4</sub>)<sub>2</sub> with symmetry 4, and octahedra <i>K</i>6 = 0@8(Rh<sub>2</sub>Pu<sub>6</sub>) with symmetry <i>mmm</i> and spacers Rh. For the crystal structure of Pu<sub>20</sub>Os<sub>12</sub>-<i>tI</i>32, framework-forming pyramid-shaped polyhedra <i>K</i>5 = 0@OsPu<sub>4</sub> with symmetry 4, as well as spacers Pu and Os, are defined. For the crystal structure (Ti<sub>4</sub>Ni)<sub>2</sub>(Bi4), frame-forming pyramids <i>K</i>5 = 0@Ti<sub>4</sub>Ni and tetrahedra <i>K</i>4 = 0@Bi<sub>4</sub>) are defined. For the crystal structure (Pu<sub>4</sub>Co)<sub>2</sub>(Pu<sub>4</sub>)-<i>tI</i>28, frame-forming pyramids <i>K</i>5 = 0@ Pu<sub>4</sub>Co and tetrahedra <i>K</i>4 = 0@Pu<sub>4</sub> are defined. For the crystal structure of Bi<sub>4</sub>-<i>tI</i>8, frame-forming tetrahedra <i>K</i>4 = 0@Bi<sub>4</sub> are defined. The symmetric and topological code of self-assembly processes of 3D structures is reconstructed from clusters-precursors in the following form: primary chain → layer → framework.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"544 - 556"},"PeriodicalIF":0.8000,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Cluster Self-Organization of Intermetallic Systems: Clusters-Precursors K15, K6, K5, and K4 for the Self-Assembly of Crystal Structures Pu31Rh20-tI204, Pu20Os12-tI32, (Pu4Co)2(Pu4)-tI28, (Ti4Ni)2(Bi4)-tI28, and Bi4-tI8\",\"authors\":\"V. Ya. Shevchenko, G. D. Ilyushin\",\"doi\":\"10.1134/S1087659623600692\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Using the ToposPro software package, a combinatorial-topological analysis and modeling of the self-assembly of the following crystal structures with space group <i>I</i>4/<i>mcm</i> are realized: Pu<sub>31</sub>Rh<sub>20</sub>-<i>tI</i>204: <i>a</i> = 11.076 Å, <i>c</i> = 36.933 Å, <i>V</i> = 4530.86 Å<sup>3</sup>, Pu<sub>20</sub>Os<sub>12</sub>-<i>tI</i>32: <i>a</i> = 10.882 Å, <i>c</i> = 5.665 Å, <i>V</i> = 670.8 Å<sup>3</sup>. (Pu<sub>4</sub>Co)<sub>2</sub> (Pu<sub>4</sub>)-<i>tI</i>28: <i>a</i> = 10.475 Å, <i>c</i> = 5.340 Å, <i>V</i> = 585.9Å<sup>3</sup>. (Ti<sub>4</sub>Ni)<sub>2</sub>(Bi4)-<i>tI</i>28: <i>a</i> = 10.554 Å, <i>c</i> = 4.814 Å, <i>V</i> = 536.2Å<sup>3</sup>, Bi<sub>4</sub>-<i>tI</i>8: <i>a</i> = 8.518 Å, <i>c</i> = 4.164 Å, <i>V</i> = 302.15 Å<sup>3</sup>. For the crystal structure of Pu<sub>31</sub>Rh<sub>20</sub>-<i>tI</i>204, 113 variants of the cluster representation of the 3<i>D</i> atomic network with the following number of structural units are established: 4 (14 variants), 5 (61 variants), and 6 (38 variants). A variant of the self-assembly of the crystal structure with the participation of three types of framework-forming polyhedra is considered: <i>K</i>15 = Pu@14(Rh<sub>2</sub>Pu<sub>5</sub>)<sub>2</sub> with symmetry –42<i>m</i>, double pyramids <i>K</i>10 = (Rh@Pu<sub>4</sub>)<sub>2</sub> with symmetry 4, and octahedra <i>K</i>6 = 0@8(Rh<sub>2</sub>Pu<sub>6</sub>) with symmetry <i>mmm</i> and spacers Rh. For the crystal structure of Pu<sub>20</sub>Os<sub>12</sub>-<i>tI</i>32, framework-forming pyramid-shaped polyhedra <i>K</i>5 = 0@OsPu<sub>4</sub> with symmetry 4, as well as spacers Pu and Os, are defined. For the crystal structure (Ti<sub>4</sub>Ni)<sub>2</sub>(Bi4), frame-forming pyramids <i>K</i>5 = 0@Ti<sub>4</sub>Ni and tetrahedra <i>K</i>4 = 0@Bi<sub>4</sub>) are defined. For the crystal structure (Pu<sub>4</sub>Co)<sub>2</sub>(Pu<sub>4</sub>)-<i>tI</i>28, frame-forming pyramids <i>K</i>5 = 0@ Pu<sub>4</sub>Co and tetrahedra <i>K</i>4 = 0@Pu<sub>4</sub> are defined. For the crystal structure of Bi<sub>4</sub>-<i>tI</i>8, frame-forming tetrahedra <i>K</i>4 = 0@Bi<sub>4</sub> are defined. The symmetric and topological code of self-assembly processes of 3D structures is reconstructed from clusters-precursors in the following form: primary chain → layer → framework.</p>\",\"PeriodicalId\":580,\"journal\":{\"name\":\"Glass Physics and Chemistry\",\"volume\":\"49 6\",\"pages\":\"544 - 556\"},\"PeriodicalIF\":0.8000,\"publicationDate\":\"2023-12-27\",\"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/S1087659623600692\",\"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/S1087659623600692","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}
引用次数: 0
摘要
摘要 利用 ToposPro 软件包,实现了空间群为 I4/mcm 的下列晶体结构的组合-拓扑分析和自组装建模:Pu31Rh20-tI204: a = 11.076 Å, c = 36.933 Å, V = 4530.86 Å3, Pu20Os12-tI32: a = 10.882 Å, c = 5.665 Å, V = 670.8 Å3. (Pu4Co)2 (Pu4)-tI28: a = 10.(Ti4Ni)2(Bi4)-tI28: a = 10.554 Å, c = 4.814 Å, V = 536.2 Å3, Bi4-tI8: a = 8.518 Å, c = 4.164 Å, V = 302.15 Å3.就 Pu31Rh20-tI204 晶体结构而言,三维原子网络的簇表示法有 113 个变体,其结构单元数目如下:4(14 个变体)、5(61 个变体)和 6(38 个变体)。考虑了三种框架形成多面体参与的晶体结构自组装变体:对称性为 -42m 的 K15 = Pu@14(Rh2Pu5)2,对称性为 4 的双金字塔 K10 = (Rh@Pu4)2,对称性为 mmm 的八面体 K6 = 0@8(Rh2Pu6)和间隔物 Rh。对于 Pu20Os12-tI32 晶体结构,定义了对称性为 4 的框架形成金字塔形多面体 K5 = 0@OsPu4,以及间隔物 Pu 和 Os。对于晶体结构 (Ti4Ni)2(Bi4),定义了形成框架的金字塔形多面体 K5 = 0@Ti4Ni 和四面体 K4 = 0@Bi4)。对于 (Pu4Co)2(Pu4)-tI28 晶体结构,定义了框架形成金字塔 K5 = 0@ Pu4Co 和四面体 K4 = 0@Pu4。对于 Bi4-tI8 的晶体结构,定义了框架形成的四面体 K4 = 0@Bi4。三维结构自组装过程的对称和拓扑代码是按以下形式从簇-前驱体重建的:主链→层→框架。
Cluster Self-Organization of Intermetallic Systems: Clusters-Precursors K15, K6, K5, and K4 for the Self-Assembly of Crystal Structures Pu31Rh20-tI204, Pu20Os12-tI32, (Pu4Co)2(Pu4)-tI28, (Ti4Ni)2(Bi4)-tI28, and Bi4-tI8
Using the ToposPro software package, a combinatorial-topological analysis and modeling of the self-assembly of the following crystal structures with space group I4/mcm are realized: Pu31Rh20-tI204: a = 11.076 Å, c = 36.933 Å, V = 4530.86 Å3, Pu20Os12-tI32: a = 10.882 Å, c = 5.665 Å, V = 670.8 Å3. (Pu4Co)2 (Pu4)-tI28: a = 10.475 Å, c = 5.340 Å, V = 585.9Å3. (Ti4Ni)2(Bi4)-tI28: a = 10.554 Å, c = 4.814 Å, V = 536.2Å3, Bi4-tI8: a = 8.518 Å, c = 4.164 Å, V = 302.15 Å3. For the crystal structure of Pu31Rh20-tI204, 113 variants of the cluster representation of the 3D atomic network with the following number of structural units are established: 4 (14 variants), 5 (61 variants), and 6 (38 variants). A variant of the self-assembly of the crystal structure with the participation of three types of framework-forming polyhedra is considered: K15 = Pu@14(Rh2Pu5)2 with symmetry –42m, double pyramids K10 = (Rh@Pu4)2 with symmetry 4, and octahedra K6 = 0@8(Rh2Pu6) with symmetry mmm and spacers Rh. For the crystal structure of Pu20Os12-tI32, framework-forming pyramid-shaped polyhedra K5 = 0@OsPu4 with symmetry 4, as well as spacers Pu and Os, are defined. For the crystal structure (Ti4Ni)2(Bi4), frame-forming pyramids K5 = 0@Ti4Ni and tetrahedra K4 = 0@Bi4) are defined. For the crystal structure (Pu4Co)2(Pu4)-tI28, frame-forming pyramids K5 = 0@ Pu4Co and tetrahedra K4 = 0@Pu4 are defined. For the crystal structure of Bi4-tI8, frame-forming tetrahedra K4 = 0@Bi4 are defined. The symmetric and topological code of self-assembly processes of 3D structures is reconstructed from clusters-precursors 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.