Pub Date : 2023-12-27DOI: 10.1134/S1087659623600631
G. I. Makarov, T. M. Makarova
A new method for molecular dynamics (MD) modeling of the glass structure using a crystal structural template is proposed. The template is based on the unit cell of the crystalline phase, whose composition is qualitatively similar to the modeled glass. Using this approach and multistage MD simulation, the model of the spatial structure of grade E borosilicate glass, reproducing its physicochemical characteristics, is obtained. The proposed method enables to model the glass structure using classical MD methods with greater productivity and stability.
摘要 本文提出了一种利用晶体结构模板进行玻璃结构分子动力学(MD)建模的新方法。该模板基于晶相的单胞,其组成与建模的玻璃质地相似。利用这种方法和多级 MD 仿真,获得了 E 级硼硅玻璃的空间结构模型,再现了其物理化学特性。所提出的方法能够使用经典 MD 方法建立玻璃结构模型,并具有更高的生产率和稳定性。
{"title":"Molecular Dynamics Modeling of the Grade E Borosilicate Glass Structure Using a Crystal Structural Template","authors":"G. I. Makarov, T. M. Makarova","doi":"10.1134/S1087659623600631","DOIUrl":"10.1134/S1087659623600631","url":null,"abstract":"<p>A new method for molecular dynamics (MD) modeling of the glass structure using a crystal structural template is proposed. The template is based on the unit cell of the crystalline phase, whose composition is qualitatively similar to the modeled glass. Using this approach and multistage MD simulation, the model of the spatial structure of grade E borosilicate glass, reproducing its physicochemical characteristics, is obtained. The proposed method enables to model the glass structure using classical MD methods with greater productivity and stability.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"635 - 641"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056316","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 : 2023-12-27DOI: 10.1134/S1087659623600552
V. A. Kazakov, N. P. Starovoitov, V. A. Dudkin, S. V. Korenev, P. V. Kozlov, M. B. Remizov
A technique for the experimental determination of the thermophysical characteristics of inactive aluminophosphate and borosilicate glasses by differential scanning calorimetry (DSC) is proposed and tested. The advantages of this measurement technique are shown. For glassy matrices of various compositions, the specific heat capacity and thermal conductivity coefficient are determined. The obtained experimental values make it possible to calculate the thermal conductivity values. The applicability of this method is proved by working with real samples of vitrified high-level waste to study their properties and form a database based on them.
{"title":"Study of the Thermophysical Properties of Aluminophosphate and Borosilicate Glasses by DSC","authors":"V. A. Kazakov, N. P. Starovoitov, V. A. Dudkin, S. V. Korenev, P. V. Kozlov, M. B. Remizov","doi":"10.1134/S1087659623600552","DOIUrl":"10.1134/S1087659623600552","url":null,"abstract":"<p>A technique for the experimental determination of the thermophysical characteristics of inactive aluminophosphate and borosilicate glasses by differential scanning calorimetry (DSC) is proposed and tested. The advantages of this measurement technique are shown. For glassy matrices of various compositions, the specific heat capacity and thermal conductivity coefficient are determined. The obtained experimental values make it possible to calculate the thermal conductivity values. The applicability of this method is proved by working with real samples of vitrified high-level waste to study their properties and form a database based on them.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"564 - 572"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056372","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 : 2023-12-27DOI: 10.1134/S1087659622600752
Narges Amini, Safdar Habibi, Nahid Mohammadiparsa
In this work an attempt is made to study the impact of the quenching rate upon structure, hyperfine interactions, magnetic and mechanical properties of Fe78Si9B13 metallic glasses. Other involved parameters in melt spinning method were kept invariant. Analytical techniques comprising X-ray diffraction, transmission Mössbauer spectrometry, vibration sample magnetometer, Vickers microhardness and differential scanning calorimetry were employed. Minor effect of quenching rate upon the macroscopic magnetic properties was detected. It was shown that notable changes in the local atomic arrangement, structure, and mechanical properties were unveiled, dominantly by represent the crystallization at the lowest quenching rate.
摘要 在这项工作中,我们尝试研究淬火率对 Fe78Si9B13 金属玻璃的结构、超线性相互作用、磁性和机械性能的影响。熔融纺丝法中的其他相关参数保持不变。分析技术包括 X 射线衍射、透射莫斯鲍尔光谱仪、振动样品磁力计、维氏显微硬度和差示扫描量热仪。检测了淬火率对宏观磁性能的微小影响。结果表明,在最低淬火速率下,局部原子排列、结构和机械性能发生了显著变化,主要表现为结晶。
{"title":"Effects of Different Quenching Rate on the Various Properties of Fe–Si–B Amorphous Alloy Prepared by Melt Spinning Method","authors":"Narges Amini, Safdar Habibi, Nahid Mohammadiparsa","doi":"10.1134/S1087659622600752","DOIUrl":"10.1134/S1087659622600752","url":null,"abstract":"<p>In this work an attempt is made to study the impact of the quenching rate upon structure, hyperfine interactions, magnetic and mechanical properties of Fe<sub>78</sub>Si<sub>9</sub>B<sub>13</sub> metallic glasses. Other involved parameters in melt spinning method were kept invariant. Analytical techniques comprising X-ray diffraction, transmission Mössbauer spectrometry, vibration sample magnetometer, Vickers microhardness and differential scanning calorimetry were employed. Minor effect of quenching rate upon the macroscopic magnetic properties was detected. It was shown that notable changes in the local atomic arrangement, structure, and mechanical properties were unveiled, dominantly by represent the crystallization at the lowest quenching rate.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"617 - 624"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056579","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 : 2023-12-27DOI: 10.1134/S1087659623600035
Yosuke Uchida, Takumi Iwaki, Teruhisa Hongo
Blast furnace slag is produced in large quantities as a by-product in the steel manufacturing process. In this study, a method for synthesizing lead ion adsorbent with high adsorption ability was investigated by alkali activation of the blast furnace slag. A sodium hydroxide aqueous solution was used as an alkali activator, and silica was added to the aqueous solution to improve the adsorption capacity. Alkali activation of the blast furnace slag with the sodium hydroxide aqueous solution yielded lead ion adsorbent. Addition of silica to the sodium hydroxide aqueous solution further increased the lead ion adsorption capacity. Langmuir adsorption isotherms revealed that the highest maximum adsorption capacity of 1658.1 mg-Pb/g was obtained when 5 g of silica was added to 50 mL of the sodium hydroxide aqueous solution. The adsorption capacity for lead ion decreased when more than 10 g of silica was added to the sodium hydroxide aqueous solution.
{"title":"Effect of Silica Addition on Lead Ion Adsorption Ability of Alkali-Activated Blast Furnace Slag","authors":"Yosuke Uchida, Takumi Iwaki, Teruhisa Hongo","doi":"10.1134/S1087659623600035","DOIUrl":"10.1134/S1087659623600035","url":null,"abstract":"<p>Blast furnace slag is produced in large quantities as a by-product in the steel manufacturing process. In this study, a method for synthesizing lead ion adsorbent with high adsorption ability was investigated by alkali activation of the blast furnace slag. A sodium hydroxide aqueous solution was used as an alkali activator, and silica was added to the aqueous solution to improve the adsorption capacity. Alkali activation of the blast furnace slag with the sodium hydroxide aqueous solution yielded lead ion adsorbent. Addition of silica to the sodium hydroxide aqueous solution further increased the lead ion adsorption capacity. Langmuir adsorption isotherms revealed that the highest maximum adsorption capacity of 1658.1 mg-Pb/g was obtained when 5 g of silica was added to 50 mL of the sodium hydroxide aqueous solution. The adsorption capacity for lead ion decreased when more than 10 g of silica was added to the sodium hydroxide aqueous solution.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"651 - 656"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056192","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 : 2023-12-27DOI: 10.1134/S1087659623600679
D. S. Ershov, N. V. Besprozvannykh, O. Yu. Sinelshchikova
The article presents the results of a study of new ceramic materials φ-Bi8Pb5O17 obtained by pyrolysis using mannitol C6H14O6 as a reducing fuel. The values of the band gap of the obtained compositions are determined by analyzing the diffuse reflectance spectra using the Tauc construction. They are in the range from 2.57 to 2.67 eV, which corresponds to visible light photocatalysts. The degree of degradation of methylene orange when using synthesized samples ranged from 95 to 99% when irradiated for 3 h with a fluorescent mercury lamp.
{"title":"Effect of Conditions of Mannitol-Nitrate Synthesis on Photocatalytic Properties of φ-Bi8Pb5O17","authors":"D. S. Ershov, N. V. Besprozvannykh, O. Yu. Sinelshchikova","doi":"10.1134/S1087659623600679","DOIUrl":"10.1134/S1087659623600679","url":null,"abstract":"<p>The article presents the results of a study of new ceramic materials φ-Bi<sub>8</sub>Pb<sub>5</sub>O<sub>17</sub> obtained by pyrolysis using mannitol C<sub>6</sub>H<sub>14</sub>O<sub>6</sub> as a reducing fuel. The values of the band gap of the obtained compositions are determined by analyzing the diffuse reflectance spectra using the Tauc construction. They are in the range from 2.57 to 2.67 eV, which corresponds to visible light photocatalysts. The degree of degradation of methylene orange when using synthesized samples ranged from 95 to 99% when irradiated for 3 h with a fluorescent mercury lamp.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"680 - 686"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056315","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 : 2023-12-27DOI: 10.1134/S1087659623600734
N. Yu. Ul’yanova, E. Yu. Brazovskaya, O. Yu. Golubeva
The stability of synthetic and natural zeolites in model biological media simulating the environment of the stomach (pH 1.8), blood plasma (pH 6.9), and intestines (pH 8) is studied. The effect of long-term exposure (up to 7 days) to biological media on the crystal structure of Beta, Rho, Y, and clinoptilolite zeolites is studied. The degree of degradation of the crystal structure of zeolites is controlled by X-ray phase analysis. Based on the results obtained, conclusions are drawn on the prospects for the use of synthetic and natural zeolites as drug carriers.
{"title":"Study of the Stability of Zeolites in Model Biological Environments","authors":"N. Yu. Ul’yanova, E. Yu. Brazovskaya, O. Yu. Golubeva","doi":"10.1134/S1087659623600734","DOIUrl":"10.1134/S1087659623600734","url":null,"abstract":"<p>The stability of synthetic and natural zeolites in model biological media simulating the environment of the stomach (pH 1.8), blood plasma (pH 6.9), and intestines (pH 8) is studied. The effect of long-term exposure (up to 7 days) to biological media on the crystal structure of Beta, Rho, Y, and clinoptilolite zeolites is studied. The degree of degradation of the crystal structure of zeolites is controlled by X-ray phase analysis. Based on the results obtained, conclusions are drawn on the prospects for the use of synthetic and natural zeolites as drug carriers.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"706 - 708"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056574","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 : 2023-12-27DOI: 10.1134/S1087659623600655
O. L. Belousova, V. A. Kuznetsova, N. Yu. Fedorenko, V. L. Ugolkov, T. V. Khamova, O. A. Shilova
By using the method of coprecipitation of hydroxides in the ZrO2–CaO–MgO system, xerogels, powders, and ceramics based on them are obtained. The effect of low temperatures during the preparation of precursors on the phase composition and physicochemical properties of the materials is studied. It is shown that the use of precipitate’s cryotreatment makes it possible to reduce the open porosity and water absorption of the ceramics.
{"title":"Study on the Influence of Low Temperatures on the Physicochemical Properties of Xerogels, Powders and Ceramics Based on ZrO2","authors":"O. L. Belousova, V. A. Kuznetsova, N. Yu. Fedorenko, V. L. Ugolkov, T. V. Khamova, O. A. Shilova","doi":"10.1134/S1087659623600655","DOIUrl":"10.1134/S1087659623600655","url":null,"abstract":"<p>By using the method of coprecipitation of hydroxides in the ZrO<sub>2</sub>–CaO–MgO system, xerogels, powders, and ceramics based on them are obtained. The effect of low temperatures during the preparation of precursors on the phase composition and physicochemical properties of the materials is studied. It is shown that the use of precipitate’s cryotreatment makes it possible to reduce the open porosity and water absorption of the ceramics.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"687 - 692"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139189908","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 : 2023-12-27DOI: 10.1134/S1087659623600667
O. L. Belousova, A. N. Parunova, N. Yu. Fedorenko, V. L. Ugolkov, T. V. Khamova, O. A. Shilova
Xerogels and powders of a solid solution based on zirconium dioxide are synthesized by the method of coprecipitation of hydroxides from aqueous solutions of salts of zirconium nitrate ZrO(NO3)2⋅2H2O, aluminum Al(NO3)3⋅9H2O, and cerium Ce(NO3)3⋅9H2O with an aqueous 1 M solution of ammonia NH4OH. A dense ceramic with low porosity and water absorption is obtained. The effect of the ultrasonic treatment of the precipitate and mechanical treatment of the xerogel on the physicochemical properties of the obtained materials is evaluated.
{"title":"Effect of Xerogel and Powder Synthesis Conditions on the Properties of Ceramics Based on t-ZrO2 in the ZrO2–СeO2–Al2O3 System","authors":"O. L. Belousova, A. N. Parunova, N. Yu. Fedorenko, V. L. Ugolkov, T. V. Khamova, O. A. Shilova","doi":"10.1134/S1087659623600667","DOIUrl":"10.1134/S1087659623600667","url":null,"abstract":"<p>Xerogels and powders of a solid solution based on zirconium dioxide are synthesized by the method of coprecipitation of hydroxides from aqueous solutions of salts of zirconium nitrate ZrO(NO<sub>3</sub>)<sub>2</sub>⋅2H<sub>2</sub>O, aluminum Al(NO<sub>3</sub>)<sub>3</sub>⋅9H<sub>2</sub>O, and cerium Ce(NO<sub>3</sub>)<sub>3</sub>⋅9H<sub>2</sub>O with an aqueous 1 M solution of ammonia NH<sub>4</sub>OH. A dense ceramic with low porosity and water absorption is obtained. The effect of the ultrasonic treatment of the precipitate and mechanical treatment of the xerogel on the physicochemical properties of the obtained materials is evaluated.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"664 - 671"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139191487","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 : 2023-12-27DOI: 10.1134/S1087659622600636
J. Anjaiah
The dielectric constant (ε'), loss factor (tanδ), and ac conductivity (σac) of 30 Li2O–10CdO–(60 – x)-B2O3:xLn2O3, where (x = 0 and 1) and (Ln = Pr, Nd, Sm, and Eu) were investigated using a frequency range of 102–105 Hz and temperature ranging from 30 to 250°C in this work. The differential scanning calorimetry (DSC) technique was employed to confirm the glassy nature of the materials under study. The dielectric parameters ε', tan δ, and σac rise when rare-earth ions are added to the glass matrix at any frequency or temperature. Dielectric breakdown and activation energies are lower in doped than in undoped glasses while ac current flows through them at room temperature. Rare-earth ion doping’s dielectric parameter values decrease with temperature as atomic number (Z) rises. The dielectric parameter values for the Pr3+ doped glass matrix is the highest. QM tunnelling model was used to describe the ac conduction behaviour of these glasses.
{"title":"Effect of Rare Earth Ion Doping on ac Conductivity and Dielectric Properties of Lithium Cadmium Borate Glasses","authors":"J. Anjaiah","doi":"10.1134/S1087659622600636","DOIUrl":"10.1134/S1087659622600636","url":null,"abstract":"<p>The dielectric constant (ε'), loss factor (tanδ), and ac conductivity (σ<sub>ac</sub>) of 30 Li<sub>2</sub>O–10CdO–(60 – <i>x</i>)-B<sub>2</sub>O<sub>3</sub>:<i>x</i>Ln<sub>2</sub>O<sub>3</sub>, where (<i>x</i> = 0 and 1) and (Ln = Pr, Nd, Sm, and Eu) were investigated using a frequency range of 10<sup>2</sup>–10<sup>5</sup> Hz and temperature ranging from 30 to 250°C in this work. The differential scanning calorimetry (DSC) technique was employed to confirm the glassy nature of the materials under study. The dielectric parameters ε', tan δ, and σ<sub>ac</sub> rise when rare-earth ions are added to the glass matrix at any frequency or temperature. Dielectric breakdown and activation energies are lower in doped than in undoped glasses while ac current flows through them at room temperature. Rare-earth ion doping’s dielectric parameter values decrease with temperature as atomic number (<i>Z</i>) rises. The dielectric parameter values for the Pr<sup>3+</sup> doped glass matrix is the highest. QM tunnelling model was used to describe the ac conduction behaviour of these glasses.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"49 6","pages":"584 - 592"},"PeriodicalIF":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056194","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 : 2023-12-27DOI: 10.1134/S1087659623600692
V. Ya. Shevchenko, G. D. Ilyushin
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.
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。
{"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":"10.1134/S1087659623600692","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":0.8,"publicationDate":"2023-12-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139056620","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}