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The Effect of the Introduction of Detonation Nanodiamonds on the Physical and Mechanical Characteristics of Thermoplastic Elastomers 爆轰纳米金刚石的引入对热塑性弹性体物理力学特性的影响
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-07-01 DOI: 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.

研制了基于丁苯橡胶的爆轰纳米金刚石增强热塑性弹性体(TPEs)。研究了不同DND含量的增强材料的力学特性。与未填充的复合材料相比,所开发的材料的抗压强度增加了30%,当引入0.1% DND时,材料的抗拉强度增加了10%。
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引用次数: 0
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 金属间化合物体系的团簇自组织:团簇前体K3、K4、K5、K7和K8对Lu66Te24-mC90、Te4Lu28-oC32、Lu3(TeLu3)Lu2-hP9和Lu4Te4-cF8晶体结构的自组装
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-07-01 DOI: 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。
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引用次数: 0
Formation of Waveguide Layers on the Surface of K8 Glass Produced by Thermoradiation Ion Exchange 热辐射离子交换制备K8玻璃表面波导层的形成
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-07-01 DOI: 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.

在60Co源3000 R/s γ辐射场和场外,在350 ~ 500℃的温度下,在NaNO3和cno3盐的碱性熔体中对K8玻璃进行低温热处理。在({text{Na}}_{{{text{glass}}}}^{ + })↔({text{Cs}}_{{{text{melt}}}}^{ + })离子交换扩散引起的热辐射处理的影响下,在玻璃的表层产生机械压应力,导致形成给定厚度的波导层,并增加折射率(RI)增量、波导模式数和波导层的深度。
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引用次数: 0
Molecular Dynamics Modeling of SiO2 Melts and Glass Formation Processes SiO2熔体和玻璃形成过程的分子动力学建模
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-07-01 DOI: 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.

利用ReaxFF电位的分子动力学(MD)研究了石英和方石英的熔融过程,并对熔融过程中不同阶段的非晶态结构进行了研究。在石英熔体中发现了从结晶相继承的过量八元环的长期保存,而在方英石熔体中,没有观察到类似的六元环的保存。因此,与方英石熔体相比,石英熔体和从中获得的玻璃具有结构记忆性。四元环的数目随温度的升高而增加。所获得的非晶结构的许多其他特征,我们认为是玻璃模型,讨论。
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引用次数: 0
Effect of Dy2O3 on Physical, Properties of B2O3–TeO2–ZnO–Li2O–WO3 Glasses Dy2O3对b2o3 - teo2 - zno - li20 - wo3玻璃物理性能的影响
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-05-24 DOI: 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.

Dy2O3对硼碲酸盐玻璃(B2O3)0.2 - (TeO2)0.22 - x - (ZnO)0.28 - (Li2O)0.20 - (WO3)0.10 - (Dy2O3)x性能的影响研究了X = 0.01至0.06。随着Dy2O3含量的增加,密度增大,摩尔体积减小,这可以从组成上解释。随着Dy2O3含量的增加,玻璃化转变温度升高,热稳定性降低。当Dy2O3的摩尔分数为0.04时,电导率增加,活化能降低,而当Dy2O3含量较高时,电导率则相反。这些结果归因于发生在0.04摩尔分数的Dy2O3的网络变化。Dy2O3对电导率的影响第一次以这种方式反映出来。确定了极化子跳跃距离、极化子半径和德拜温度,并进行了适当的讨论。
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引用次数: 0
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 晶体形成体系的簇状自组织:自组装 Pd112Co204Al684-cP1000 晶体结构的新型三层(K155 = Al@Al6Pd8@Pd12Al30@Pd8Сo18Al72)和双层(K55 = Co@Al12@Co12Al30)前驱体簇
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-05-24 DOI: 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.

利用 ToposPro 软件包对 Pd112Co204Al684-cP1000 晶体结构(sp. gr. Pa-3、a = 24.433 Å 和 V = 14587.24 Å3)进行了几何和拓扑分析。晶体结构的金属前驱体簇是使用一种将结构图分解为簇结构的算法,并通过以图的形式构建结构的基本网格来确定的,该图的节点与前驱体簇中心的位置相对应 (S_{3}^{0}.)。三维原子网格的簇表示共有 26 906 种变体,结构单元数从 3 到 12 不等。研究考虑了对称性为 g = -3 的新型三层 K155(4a) = Al@Al6Pd8)@Pd12Al30@Pd8Co18Al72 和双层前驱体簇 K55(4b) = Co@Al12@Co12Al30 晶体结构的自组装。在单位晶胞中,4a 位置由 Al 原子占据,它们是 15 原子多面体 K15(4a) = Al@Al8Pd6 的中心原子;4b 位置由 Co 原子占据,它们是 13 原子二十面体 K13(4b) = Co@Al12 的中心原子。前驱体簇 K155 和 K55 的三维结构自组装过程的对称和拓扑代码重构如下:主链 → 微层 → 微框架。在 K155 和 K55 纳米团簇的三维框架中,铝原子被确立为占据空隙的间隔物。
{"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,&nbsp;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}
引用次数: 0
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 燃料电池正极La2O3-SrO-Ni (Co,Fe)2O3 -δ体系中钙钛矿结构固溶体的电物理性质研究
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-05-24 DOI: 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.

采用硝酸盐超声共晶法制备了La1-xSrxNiO3 -δ、La1-xSrxCoO3 -δ和La1-xSrxFe0.7Ni0.3O3 -δ (x = 0.30;0.40)。在此基础上,获得了具有~65 ~ 69 nm(1300°С)相干散射区域(CSR)的陶瓷纳米材料。在1300℃下烧制的陶瓷为单相,具有La2O3-SrO-Ni (Co,Fe)2O3 -δ体系的四方和正交钙钛矿型结构。固溶体具有混合电子-离子电导率,传递数te = 0.98-0.90, ti = 0.02-0.10。具有四方钙钛矿型晶体结构的陶瓷比具有正交钙钛矿型晶体结构的材料具有更高的导电性。根据其与固溶体结构特征相关的电物理性质,在此基础上制备的陶瓷材料有望作为平均温度燃料电池的固体氧化物阴极。
{"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,&nbsp;D. A. Dyuskina,&nbsp;I. G. Polyakova,&nbsp;M. Yu. Arsent’ev,&nbsp;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}
引用次数: 0
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 金属间化合物的结构化学:新簇状前驱体 K46 = 0@Hg6@Pu4Hg36 和 K26 = 0@Pu4@Pu4Hg18 对 Pu56Hg352-cF408 晶体结构的影响,以及 K17= Zr@Pu16 对 Zr4Pu112-tI116 晶体结构的影响
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-05-24 DOI: 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.

利用计算机方法(ToposPro 软件包)对 Pu56Hg352-cF408 (a = 21.780 Å,V = 10331.75 Å3,空间群 F-43m)和 Zr4Pu112-tI116 ((a = b = 18.189 Å,c = 7.857 Å,V = 2599.86 Å3,空间群 I41/a)晶体结构的自组装进行了组合拓扑分析和建模。采用将三维结构图完全分解为团簇结构的方法来确定形成框架的纳米团簇。对于 Pu56Hg352-cF408,确定了三维结构图分解的 88 种变体,簇数从 2 到 6 不等。发现新的两层纳米团簇 K26 = 0@Pu4@Pu4Hg18 和 K46 = 0@Hg6@Pu4Hg36,对称性为 -43m,形成三维堆积。框架空隙包含 Hg4 四面体团簇和 Hg 间距原子。对于 Zr4Pu112-tI116,框架形成的纳米团簇 K17 = Zr@Pu16 具有 -4 对称性。框架空隙包含 Pu4 四面体和 Pu 空间原子。
{"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,&nbsp;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}
引用次数: 0
Forecast of Crystallizing Phases and Modeling of Chemical Interaction in the System CaO–MgO–SiO2 CaO-MgO-SiO2体系结晶相预测及化学相互作用模拟
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-05-24 DOI: 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.

构建了先前研究的СаO-MgO-SiO2系统的相树。相位树包括三个循环。相树由15个简单点表示,由15个稳定的割线分隔。在该体系中发现了6种完全熔融和4种完全熔融的二元化合物和4种完全熔融的三元化合物。在相树的基础上,结合面元数据,对稳定割线和相中二次三角形的结晶相进行了预测。对于组成的图示点,即稳定割线和不稳定割线的交点,根据热力学数据描述了化学相互作用。已经证明,三元化合物可以通过几种反应合成。
{"title":"Forecast of Crystallizing Phases and Modeling of Chemical Interaction in the System CaO–MgO–SiO2","authors":"I. K. Garkushin,&nbsp;O. V. Lavrent’eva,&nbsp;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}
引用次数: 0
Speed of Sound and Bulk Modulus of Diamond: An Ab Initio Study 金刚石的声速和体积模量:从头算研究
IF 0.7 4区 材料科学 Q4 Materials Science Pub Date : 2023-05-24 DOI: 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.

对大多数科学家来说,材料力学性能的研究具有相当大的基础和实际意义。本文利用密度泛函理论(DFT)方法计算了金刚石的平衡胞参数、体积模量、体积模量对压力的一阶导数和声速分别为3.570 Å、433.2 GPa、3.71和17731.2 m/s。这些参数与实验值吻合较好。研究结果表明,利用DFT方法可以高精度地预测材料的力学性能。
{"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}
引用次数: 0
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Glass Physics and Chemistry
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