Pub Date : 2023-07-01DOI: 10.1134/S108765962360014X
M. V. Timoshenko, S. V. Balabanov, M. M. Sychov, K. S. Koshevaya, V. Yu. Dolmatov, V. P. Britov
Thermoplastic elastomers (TPEs) reinforced with detonation nanodiamonds (DNDs) based on styrene-butadiene rubber are developed. The mechanical characteristics of the reinforced compounds with different DND contents are investigated. The developed material shows a 30% increase in compressive strength compared to the unfilled composite and a 10% increase in the tensile strength of the material with the introduction of 0.1% DND.
{"title":"The Effect of the Introduction of Detonation Nanodiamonds on the Physical and Mechanical Characteristics of Thermoplastic Elastomers","authors":"M. V. Timoshenko, S. V. Balabanov, M. M. Sychov, K. S. Koshevaya, V. Yu. Dolmatov, V. P. Britov","doi":"10.1134/S108765962360014X","DOIUrl":"10.1134/S108765962360014X","url":null,"abstract":"<p>Thermoplastic elastomers (TPEs) reinforced with detonation nanodiamonds (DNDs) based on styrene-butadiene rubber are developed. The mechanical characteristics of the reinforced compounds with different DND contents are investigated. The developed material shows a 30% increase in compressive strength compared to the unfilled composite and a 10% increase in the tensile strength of the material with the introduction of 0.1% DND.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4031835","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-07-01DOI: 10.1134/S1087659623600084
V. Ya. Shevchenko, G. D. Ilyushin
With the help of computer methods (ToposPro software package), a combinatorial topological analysis and modeling of the self-assembly of Lu4Te4-oF8 (Fm-3m, V = 211.0 Å3), Te4Lu28-oC32 (Cmcm, V = 908.3 Å3), Lu3(TeLu3)Lu2-hP9 (P-62m, V = 908.3 Å3), and Lu66Te24-mC90 (C12/m1, V = 2467.2 Å3) crystal structures are carried out. For the crystal structure of Lu4Te4-oF8, cluster precursors K8 = 0@Te4Lu4 with symmetry –43m; for Te4Lu28-oC32, tetrahedral cluster precursors K4 = 0@Lu4 and K4 = 0@TeLu3 with symmetry 2 and m; and for Lu3(TeLu3)Lu2, cluster precursors K7 = 0@Lu3(TeLu3) with symmetry 3m and spacers Lu are established. For the crystal structure of Lu66Te24-mC90, pyramid-shaped cluster precursors K5 = 0@Lu5 with symmetry 2, tetrahedra K4 = 0@Lu4 with symmetry 2, tetrahedra K4 = 0@TeLu3, and tetrahedra K4 = 0@Te2Lu2 are established, and rings K3 = 0@TeLu2 are involved in the formation of supraclusters-trimers. The symmetry and topological code of the processes of self-assembly of 3D structures from cluster precursors is reconstructed in the following form: primary chain → layer → framework.
利用计算机方法(ToposPro软件包),对Lu4Te4-oF8 (Fm-3m, V = 211.0 Å3)、Te4Lu28-oC32 (Cmcm, V = 908.3 Å3)、Lu3(TeLu3)Lu2-hP9 (P-62m, V = 908.3 Å3)和Lu66Te24-mC90 (C12/m1, V = 2467.2 Å3)晶体结构的自组装进行了组合拓扑分析和建模。对于Lu4Te4-oF8的晶体结构,团簇前驱体K8 = 0@Te4Lu4,对称性为-43m;对于Te4Lu28-oC32,四面体簇前体K4 = 0@Lu4和K4 = 0@TeLu3,对称为2和m;对于Lu3(TeLu3)Lu2,建立了对称性为3m的簇前体K7 = 0@Lu3(TeLu3)和间隔子Lu。对于Lu66Te24-mC90的晶体结构,建立了对称2的金字塔形簇前体K5 = 0@Lu5,对称2的四面体K4 = 0@Lu4,对称2的四面体K4 = 0@TeLu3,四面体K4 = 0@Te2Lu2,环K3 = 0@TeLu2参与了超簇-三聚体的形成。从聚簇前驱体中重构三维结构自组装过程的对称性和拓扑代码,其形式为:主链→层→框架。
{"title":"Cluster Self-Organization of Intermetallic Systems: Cluster Precursors K3, K4, K5, K7, and K8 for the Self-Assembly of Lu66Te24-mC90, Te4Lu28-oC32, Lu3(TeLu3)Lu2-hP9, and Lu4Te4-cF8 Crystal Structures","authors":"V. Ya. Shevchenko, G. D. Ilyushin","doi":"10.1134/S1087659623600084","DOIUrl":"10.1134/S1087659623600084","url":null,"abstract":"<p>With the help of computer methods (ToposPro software package), a combinatorial topological analysis and modeling of the self-assembly of Lu<sub>4</sub>Te<sub>4</sub>-<i>oF</i>8 (<i>Fm</i>-3<i>m</i>, V = 211.0 Å<sup>3</sup>), Te<sub>4</sub>Lu<sub>28</sub>-<i>oC</i>32 (<i>Cmcm</i>, V = 908.3 Å<sup>3</sup>), Lu<sub>3</sub>(TeLu<sub>3</sub>)Lu<sub>2</sub>-<i>hP</i>9 (<i>P</i>-62<i>m</i>, V = 908.3 Å<sup>3</sup>), and Lu<sub>66</sub>Te<sub>24</sub>-<i>mC</i>90 (<i>C</i>12/<i>m</i>1, V = 2467.2 Å<sup>3</sup>) crystal structures are carried out. For the crystal structure of Lu<sub>4</sub>Te<sub>4</sub>-<i>oF</i>8, cluster precursors <i>K</i>8 = 0@Te<sub>4</sub>Lu<sub>4</sub> with symmetry –43<i>m</i>; for Te<sub>4</sub>Lu<sub>28</sub>-<i>oC</i>32, tetrahedral cluster precursors <i>K</i>4 = 0@Lu<sub>4</sub> and <i>K</i>4 = 0@TeLu<sub>3</sub> with symmetry 2 and <i>m</i>; and for Lu<sub>3</sub>(TeLu<sub>3</sub>)Lu<sub>2</sub>, cluster precursors <i>K</i>7 = 0@Lu<sub>3</sub>(TeLu<sub>3</sub>) with symmetry 3<i>m</i> and spacers Lu are established. For the crystal structure of Lu<sub>66</sub>Te<sub>24</sub>-<i>mC</i>90, pyramid-shaped cluster precursors <i>K</i>5 = 0@Lu<sub>5</sub> with symmetry 2, tetrahedra <i>K</i>4 = 0@Lu<sub>4</sub> with symmetry 2, tetrahedra <i>K</i>4 = 0@TeLu<sub>3</sub>, and tetrahedra <i>K</i>4 = 0@Te<sub>2</sub>Lu<sub>2</sub> are established, and rings <i>K</i>3 = 0@TeLu<sub>2</sub> are involved in the formation of supraclusters-trimers. The symmetry and topological code of the processes of self-assembly of 3D structures from cluster precursors is reconstructed in the following form: primary chain → layer → framework.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4030948","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-07-01DOI: 10.1134/S1087659623600151
I. Nuritdinov, A. A. Eshbekov, B. N. Tuymanov
The low-temperature heat treatment of K8 glass is carried out at temperatures of 350–500°C in alkaline melts of NaNO3 and CsNO3 salts in the field of gamma radiation from the 60Co source at the dose rate of 3000 R/s and also outside the field. Under the influence of thermoradiation treatment due to the ({text{Na}}_{{{text{glass}}}}^{ + }) ↔ ({text{Cs}}_{{{text{melt}}}}^{ + }) ion-exchange diffusion, mechanical compressive stresses are created in the surface layer of the glass, which lead to the formation of a waveguide layer of the given thickness and an increase in the refractive index (RI) increment, the number of waveguide modes, and the depth of the waveguide layer.
{"title":"Formation of Waveguide Layers on the Surface of K8 Glass Produced by Thermoradiation Ion Exchange","authors":"I. Nuritdinov, A. A. Eshbekov, B. N. Tuymanov","doi":"10.1134/S1087659623600151","DOIUrl":"10.1134/S1087659623600151","url":null,"abstract":"<p>The low-temperature heat treatment of K8 glass is carried out at temperatures of 350–500°C in alkaline melts of NaNO<sub>3</sub> and CsNO<sub>3</sub> salts in the field of gamma radiation from the <sup>60</sup>Co source at the dose rate of 3000 R/s and also outside the field. Under the influence of thermoradiation treatment due to the <span>({text{Na}}_{{{text{glass}}}}^{ + })</span> ↔ <span>({text{Cs}}_{{{text{melt}}}}^{ + })</span> ion-exchange diffusion, mechanical compressive stresses are created in the surface layer of the glass, which lead to the formation of a waveguide layer of the given thickness and an increase in the refractive index (RI) increment, the number of waveguide modes, and the depth of the waveguide layer.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4031841","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-07-01DOI: 10.1134/S1087659623600126
A. S. Mysovsky, A. S. Paklin
Molecular dynamics (MD) with ReaxFF potentials is used to study the melting process of quartz and cristobalite together with the amorphous structures obtained at different stages of melting by cooling the melt. The long-term preservation of an excess of eight-membered rings inherited from the crystalline phase is found in the quartz melts, while in the cristobalite melts, the similar preservation of six-membered rings is not observed. Thus, it can be stated that the quartz melts and glasses obtained from them have structural memory, in contrast to cristobalite melts. An increase in the number of four-membered rings with increasing temperature is revealed. A number of other features of the obtained amorphous structures, which we consider as models for glasses, are discussed.
{"title":"Molecular Dynamics Modeling of SiO2 Melts and Glass Formation Processes","authors":"A. S. Mysovsky, A. S. Paklin","doi":"10.1134/S1087659623600126","DOIUrl":"10.1134/S1087659623600126","url":null,"abstract":"<p>Molecular dynamics (MD) with ReaxFF potentials is used to study the melting process of quartz and cristobalite together with the amorphous structures obtained at different stages of melting by cooling the melt. The long-term preservation of an excess of eight-membered rings inherited from the crystalline phase is found in the quartz melts, while in the cristobalite melts, the similar preservation of six-membered rings is not observed. Thus, it can be stated that the quartz melts and glasses obtained from them have structural memory, in contrast to cristobalite melts. An increase in the number of four-membered rings with increasing temperature is revealed. A number of other features of the obtained amorphous structures, which we consider as models for glasses, are discussed.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4031994","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-05-24DOI: 10.1134/S1087659622600132
Amarkumar Malge, T. Sankarappa, G. B. Devidas, T. Sujatha, Mohansingh Heerasingh, Ashwini Devidas
Effect of Dy2O3 on the properties of borotellurite glasses, (B2O3)0.2–(TeO2)0.22 – x–(ZnO)0.28–(Li2O)0.20–(WO3)0.10–(Dy2O3)x; x = 0.01 to 0.06 has been investigated. Density increased and molar volume decreased with increase of Dy2O3 and they were explained in terms of composition. Glass transition temperature increased and thermal stability decreased with increase of Dy2O3 content. Conductivity increased and its activation energy decreased up to 0.04 mole fraction of Dy2O3 and behaved in opposite way for higher amounts of Dy2O3. These results are ascribed to network changes occurring around 0.04 mole fractions of Dy2O3. For the first time the effect of Dy2O3 on conductivity has been reflected in this fashion. Polaron hopping distance, polaron radius and Debye’s temperature were determined and discussed appropriately.
{"title":"Effect of Dy2O3 on Physical, Properties of B2O3–TeO2–ZnO–Li2O–WO3 Glasses","authors":"Amarkumar Malge, T. Sankarappa, G. B. Devidas, T. Sujatha, Mohansingh Heerasingh, Ashwini Devidas","doi":"10.1134/S1087659622600132","DOIUrl":"10.1134/S1087659622600132","url":null,"abstract":"<p>Effect of Dy<sub>2</sub>O<sub>3</sub> on the properties of borotellurite glasses, (B<sub>2</sub>O<sub>3</sub>)<sub>0.2</sub>–(TeO<sub>2</sub>)<sub>0.22 – <i>x</i></sub>–(ZnO)<sub>0.28</sub>–(Li<sub>2</sub>O)<sub>0.20</sub>–(WO<sub>3</sub>)<sub>0.10</sub>–(Dy<sub>2</sub>O<sub>3</sub>)<sub><i>x</i></sub>; <i>x</i> = 0.01 to 0.06 has been investigated. Density increased and molar volume decreased with increase of Dy<sub>2</sub>O<sub>3</sub> and they were explained in terms of composition. Glass transition temperature increased and thermal stability decreased with increase of Dy<sub>2</sub>O<sub>3</sub> content. Conductivity increased and its activation energy decreased up to 0.04 mole fraction of Dy<sub>2</sub>O<sub>3</sub> and behaved in opposite way for higher amounts of Dy<sub>2</sub>O<sub>3</sub>. These results are ascribed to network changes occurring around 0.04 mole fractions of Dy<sub>2</sub>O<sub>3</sub>. For the first time the effect of Dy<sub>2</sub>O<sub>3</sub> on conductivity has been reflected in this fashion. Polaron hopping distance, polaron radius and Debye’s temperature were determined and discussed appropriately.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4942619","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-05-24DOI: 10.1134/S108765962260065X
V. Ya. Shevchenko, G. D. Ilyushin
Geometric and topological analysis of the Pd112Co204Al684-cP1000 crystal structure with the sp. gr. Pa-3, a = 24.433 Å, and V = 14587.24 Å3 is performed using the ToposPro software package. Metal precursor clusters of crystalline structures are determined using an algorithm for decomposing structural graphs into cluster structures and by constructing a basic grid of the structure in the form of a graph whose nodes correspond to the position of the centers of precursor clusters (S_{3}^{0}.) A total of 26 906 variants of the cluster representation of a 3D atomic mesh with the number of structural units ranging from 3 to 12 are established. The self-assembly of the crystal structure from new three-layer K155(4a) = Al@Al6Pd8)@Pd12Al30@Pd8Co18Al72 and bilayer precursor clusters K55(4b) = Co@Al12@Co12Al30 with symmetry g = –3 is considered. In the unit cell, positions 4a are occupied by Al atoms, which are the central atoms of the 15-atom polyhedron K15(4a) = Al@Al8Pd6, and positions 4b are occupied by Co atoms, which are the central atoms of the 13-atom icosahedron K13(4b) = Co@Al12. The symmetric and topological code of the processes of self-assembly of 3D structures from precursor clusters K155 and K55 is reconstructed as follows: primary chain → microlayer → microframework. Al atoms are established as spacers occupying voids in the 3D framework of the K155 and K55 nanoclusters.
{"title":"Cluster Self-Organization of Crystal-Forming Systems: New Three-Layer (K155 = Al@Al6Pd8@Pd12Al30@Pd8Сo18Al72) and Double-Layer (K55 = Co@Al12@Co12Al30) Precursor Clusters for the Self-Assembly of the Pd112Co204Al684-cP1000 Crystal Structure","authors":"V. Ya. Shevchenko, G. D. Ilyushin","doi":"10.1134/S108765962260065X","DOIUrl":"10.1134/S108765962260065X","url":null,"abstract":"<p>Geometric and topological analysis of the Pd<sub>112</sub>Co<sub>204</sub>Al<sub>684</sub>-cP1000 crystal structure with the sp. gr. <i>Pa</i>-3, <i>a</i> = 24.433 Å, and <i>V</i> = 14587.24 Å<sup>3</sup> is performed using the ToposPro software package. Metal precursor clusters of crystalline structures are determined using an algorithm for decomposing structural graphs into cluster structures and by constructing a basic grid of the structure in the form of a graph whose nodes correspond to the position of the centers of precursor clusters <span>(S_{3}^{0}.)</span> A total of 26 906 variants of the cluster representation of a 3D atomic mesh with the number of structural units ranging from 3 to 12 are established. The self-assembly of the crystal structure from new three-layer <i>K</i>155(4a) = Al@Al<sub>6</sub>Pd<sub>8</sub>)@Pd<sub>12</sub>Al<sub>30</sub>@Pd<sub>8</sub>Co<sub>18</sub>Al<sub>72</sub> and bilayer precursor clusters <i>K</i>55(4b) = Co@Al<sub>12</sub>@Co<sub>12</sub>A<sub>l30</sub> with symmetry <i>g</i> = –3 is considered. In the unit cell, positions 4a are occupied by Al atoms, which are the central atoms of the 15-atom polyhedron <i>K</i>15(4a) = Al@Al<sub>8</sub>Pd<sub>6</sub>, and positions 4b are occupied by Co atoms, which are the central atoms of the 13-atom icosahedron <i>K</i>13(4b) = Co@Al<sub>12</sub>. The symmetric and topological code of the processes of self-assembly of 3D structures from precursor clusters <i>K</i>155 and <i>K</i>55 is reconstructed as follows: primary chain → microlayer → microframework. Al atoms are established as spacers occupying voids in the 3D framework of the <i>K</i>155 and <i>K</i>55 nanoclusters.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4944122","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-05-24DOI: 10.1134/S1087659622601046
M. V. Kalinina, D. A. Dyuskina, I. G. Polyakova, M. Yu. Arsent’ev, O. A. Shilova
Finely dispersed mesoporous powders of the following composition are synthesized by the method of cocrystallization of nitrate salts with ultrasonic treatment: La1–xSrxNiO3–δ, La1–xSrxCoO3–δ, and La1–xSrxFe0.7Ni0.3O3–δ (x = 0.30; 0.40). Based on them, ceramic nanomaterials of the given composition with a coherent scattering region (CSR) of ~65–69 nm (1300°С) are obtained. Ceramics fired at 1300°C are single-phase and have a tetragonal and orthorhombic perovskite-type structure in the La2O3‒SrO‒Ni(Co,Fe)2O3–δ system. Solid solutions have mixed electron–ion conductivity with transfer numbers te = 0.98–0.90 and ti = 0.02–0.10. Ceramics with a tetragonal perovskite-type crystal structure exhibit higher electrical conductivity than materials having an orthorhombic perovskite-type crystal structure. According to their electrophysical properties related to the structural features of solid solutions, ceramic materials obtained based on them are promising as solid oxide cathodes for average-temperature fuel cells.
{"title":"Study of the Electrophysical Properties of Solid Solutions with a Perovskite Structure in La2O3–SrO–Ni(Co,Fe)2O3–δ Systems for Cathode Electrodes for Fuel Cells","authors":"M. V. Kalinina, D. A. Dyuskina, I. G. Polyakova, M. Yu. Arsent’ev, O. A. Shilova","doi":"10.1134/S1087659622601046","DOIUrl":"10.1134/S1087659622601046","url":null,"abstract":"<p>Finely dispersed mesoporous powders of the following composition are synthesized by the method of cocrystallization of nitrate salts with ultrasonic treatment: La<sub>1–<i>x</i></sub>Sr<sub><i>x</i></sub>NiO<sub>3–δ</sub>, La<sub>1–<i>x</i></sub>Sr<sub><i>x</i></sub>CoO<sub>3–δ</sub>, and La<sub>1–<i>x</i></sub>Sr<sub><i>x</i></sub>Fe<sub>0.7</sub>Ni<sub>0.3</sub>O<sub>3–δ</sub> (<i>x</i> = 0.30; 0.40). Based on them, ceramic nanomaterials of the given composition with a coherent scattering region (CSR) of ~65–69 nm (1300°С) are obtained. Ceramics fired at 1300°C are single-phase and have a tetragonal and orthorhombic perovskite-type structure in the La<sub>2</sub>O<sub>3</sub>‒SrO‒Ni(Co,Fe)<sub>2</sub>O<sub>3–δ</sub> system. Solid solutions have mixed electron–ion conductivity with transfer numbers <i>t</i><sub>e</sub> = 0.98–0.90 and <i>t</i><sub>i</sub> = 0.02–0.10. Ceramics with a tetragonal perovskite-type crystal structure exhibit higher electrical conductivity than materials having an orthorhombic perovskite-type crystal structure. According to their electrophysical properties related to the structural features of solid solutions, ceramic materials obtained based on them are promising as solid oxide cathodes for average-temperature fuel cells.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4944603","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-05-24DOI: 10.1134/S1087659622600624
V. Ya. Shevchenko, G. D. Ilyushin
The combinatorial topological analysis and modeling of self-assembly of the Pu56Hg352-cF408 (a = 21.780 Å, V = 10331.75 Å3, space group F-43m) and Zr4Pu112-tI116 ((a = b = 18.189 Å, c = 7.857 Å, V = 2599.86 Å3, space group I41/a) crystal structures are performed by computer methods (the ToposPro software package). The method of complete decomposition of the 3D structure graph into cluster structures was used to determine the framework-forming nanoclusters. For Pu56Hg352-cF408, 88 variants of decomposition of the 3D structure graph with the number of clusters from 2 to 6 were determined. New two-layer nanoclusters K26 = 0@Pu4@Pu4Hg18 and K46 = 0@Hg6@Pu4Hg36 with ‑43m symmetry were found to form a 3D packing. The framework voids contain Hg4 tetrahedral clusters and Hg spacer atoms. For Zr4Pu112-tI116, framework-forming nanoclusters K17 = Zr@Pu16 with -4 symmetry are installed. The framework voids contain Pu4 tetrahedra and Pu spacer atoms.
{"title":"Structural Chemistry of Intermetallides: New Cluster Precursors K46 = 0@Hg6@Pu4Hg36 and K26 = 0@Pu4@Pu4Hg18 for the Crystal Structure of Pu56Hg352-cF408 and K17= Zr@Pu16 for the Crystal Structure of Zr4Pu112-tI116","authors":"V. Ya. Shevchenko, G. D. Ilyushin","doi":"10.1134/S1087659622600624","DOIUrl":"10.1134/S1087659622600624","url":null,"abstract":"<p>The combinatorial topological analysis and modeling of self-assembly of the Pu<sub>56</sub>Hg<sub>352</sub>-<i>cF</i>408 (<i>a</i> = 21.780 Å, <i>V</i> = 10331.75 Å<sup>3</sup>, space group <i>F</i>-43<i>m</i>) and Zr<sub>4</sub>Pu<sub>112</sub>-<i>tI</i>116 ((<i>a</i> = <i>b</i> = 18.189 Å, <i>c</i> = 7.857 Å, <i>V</i> = 2599.86 Å<sup>3</sup>, space group <i>I</i>4<sub>1</sub>/<i>a</i>) crystal structures are performed by computer methods (the ToposPro software package). The method of complete decomposition of the 3D structure graph into cluster structures was used to determine the framework-forming nanoclusters. For Pu<sub>56</sub>Hg<sub>352</sub>-<i>cF</i>408, 88 variants of decomposition of the 3D structure graph with the number of clusters from 2 to 6 were determined. New two-layer nanoclusters <i>K</i>26 = 0@Pu<sub>4</sub>@Pu<sub>4</sub>Hg<sub>18</sub> and <i>K</i>46 = 0@Hg6@Pu<sub>4</sub>Hg<sub>36</sub> with ‑43<i>m</i> symmetry were found to form a 3D packing. The framework voids contain Hg<sub>4</sub> tetrahedral clusters and Hg spacer atoms. For Zr<sub>4</sub>Pu<sub>112</sub>-<i>tI</i>116, framework-forming nanoclusters <i>K</i>17 = Zr@Pu16 with -4 symmetry are installed. The framework voids contain Pu<sub>4</sub> tetrahedra and Pu spacer atoms.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4942605","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-05-24DOI: 10.1134/S1087659622601058
I. K. Garkushin, O. V. Lavrent’eva, A. M. Shterenberg
The phase tree of the previously studied СаO–MgO–SiO2 system was constructed. The phase tree includes three cycles. The phase tree is represented by fifteen simplices separated by fifteen stable secants. The formation of six double and four ternary compounds of congruent and incongruent melting was noted in the system. On the basis of the phase tree, taking into account the data on faceting elements, a forecast of crystallizing phases in stable secants and in phase secondary triangles was carried out. For the figurative points of the composition, corresponding to the intersections of stable and unstable secants, the chemical interaction is described on the basis of thermodynamic data. It has been shown that ternary compounds can be synthesized by several reactions.
{"title":"Forecast of Crystallizing Phases and Modeling of Chemical Interaction in the System CaO–MgO–SiO2","authors":"I. K. Garkushin, O. V. Lavrent’eva, A. M. Shterenberg","doi":"10.1134/S1087659622601058","DOIUrl":"10.1134/S1087659622601058","url":null,"abstract":"<p>The phase tree of the previously studied СаO–MgO–SiO<sub>2</sub> system was constructed. The phase tree includes three cycles. The phase tree is represented by fifteen simplices separated by fifteen stable secants. The formation of six double and four ternary compounds of congruent and incongruent melting was noted in the system. On the basis of the phase tree, taking into account the data on faceting elements, a forecast of crystallizing phases in stable secants and in phase secondary triangles was carried out. For the figurative points of the composition, corresponding to the intersections of stable and unstable secants, the chemical interaction is described on the basis of thermodynamic data. It has been shown that ternary compounds can be synthesized by several reactions.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4944125","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-05-24DOI: 10.1134/S1087659622600739
M. Yu. Arsentev
The study of the mechanical properties of materials is of considerable fundamental and practical interest to most scientists. In this work the values of the equilibrium cell parameter, bulk modulus, its first derivative with respect to the pressure, and the speed of sound for diamond were calculated using the density functional theory (DFT) method and are 3.570 Å, 433.2 GPa, 3.71 and 17731.2 m/s. These parameters are found to be in good agreement with the experimental ones. The results of the study show that the mechanical properties of materials can be predicted with a high precision using the DFT method.
{"title":"Speed of Sound and Bulk Modulus of Diamond: An Ab Initio Study","authors":"M. Yu. Arsentev","doi":"10.1134/S1087659622600739","DOIUrl":"10.1134/S1087659622600739","url":null,"abstract":"<p>The study of the mechanical properties of materials is of considerable fundamental and practical interest to most scientists. In this work the values of the equilibrium cell parameter, bulk modulus, its first derivative with respect to the pressure, and the speed of sound for diamond were calculated using the density functional theory (DFT) method and are 3.570 Å, 433.2 GPa, 3.71 and 17731.2 m/s. These parameters are found to be in good agreement with the experimental ones. The results of the study show that the mechanical properties of materials can be predicted with a high precision using the DFT method.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":null,"pages":null},"PeriodicalIF":0.7,"publicationDate":"2023-05-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"4942617","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}