Pub Date : 2025-03-23DOI: 10.1134/S1087659624601096
K. Shiraishi, T. Hongo
The development of an inexpensive and environmentally friendly method for synthesis of mesoporous silica is highly desirable. In this study, mesoporous silica SBA-15 (SP-SBA-15) was synthesized using inexpensive amorphous silica powder, which is produced industrially, as the silica source. SP-SBA-15 was compared to SBA-15 (TO-SBA-15) synthesized by a conventional method using tetraethyl orthosilicate (TEOS) as the silica source. SP-SBA-15 was found to have 8.1 nm uniform mesopores arranged in a well-defined hexagonal honeycomb structure, and the mesostructure was found to be almost identical to that of TO-SBA-15. However, the specific surface area of SP-SBA-15 was found to be 525.0 m2/g, which is lower than that of TO-SBA-15. This is due to the fact that fewer micropores were formed in the SBA-15 when silica powder was used as the silica source.
{"title":"Comparison of Mesoporous Silica SBA-15 Synthesized from Amorphous Silica Powder and Silicon Alkoxide","authors":"K. Shiraishi, T. Hongo","doi":"10.1134/S1087659624601096","DOIUrl":"10.1134/S1087659624601096","url":null,"abstract":"<p>The development of an inexpensive and environmentally friendly method for synthesis of mesoporous silica is highly desirable. In this study, mesoporous silica SBA-15 (SP-SBA-15) was synthesized using inexpensive amorphous silica powder, which is produced industrially, as the silica source. SP-SBA-15 was compared to SBA-15 (TO-SBA-15) synthesized by a conventional method using tetraethyl orthosilicate (TEOS) as the silica source. SP-SBA-15 was found to have 8.1 nm uniform mesopores arranged in a well-defined hexagonal honeycomb structure, and the mesostructure was found to be almost identical to that of TO-SBA-15. However, the specific surface area of SP-SBA-15 was found to be 525.0 m<sup>2</sup>/g, which is lower than that of TO-SBA-15. This is due to the fact that fewer micropores were formed in the SBA-15 when silica powder was used as the silica source.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 5","pages":"504 - 510"},"PeriodicalIF":0.8,"publicationDate":"2025-03-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143676367","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 : 2025-03-23DOI: 10.1134/S1087659624600479
E. V. Petrova, A. F. Dresvyannikov, L. I. Kashfrazyeva
Scientific principles for the synthesis of precursors of nanostructured oxide systems Al2O3–ZrO2–LnxOy ((Ln = Dy, Nd) are developed. The features of their formation under conditions of rapid mixing of electrogenerated reagents, implemented in a diaphragm-free coaxial reactor-electrolyzer, are studied. The methods of potentiodynamic polarization curves, X-ray diffractometry, X-ray fluorescence, synchronous thermal analysis, and laser diffraction are used to study the anodic processes occurring in the electrolyzer, the morphology of particles formed in the solution and transformed during heat treatment, as well as the phase, granulometric, and elemental compositions of precursors and oxide systems. The proposed approach allows obtaining oxide systems modified with rare earth elements based on the Al2O3–ZrO2 binary system, characterized by the presence of a stabilized phase of tetragonal zirconium dioxide. REE atoms present in the studied systems—Nd and Dy—stabilize t-ZrO2 and, apparently, occupy the positions of crystal lattice nodes, isomorphically replacing Zr4+. The latter is indicated by the broadening of the corresponding reflections of X‑ray diffraction patterns. It indirectly indicates the presence of microstresses in the microcrystals of the phases. The latter can be caused by distortions of the crystal lattices of aluminum and zirconium oxides as a result of the substitution of metal atoms by REE atoms.
{"title":"Precursors of Al2O3–ZrO2–LnxOy Oxide Systems Obtained Using Electrogenerated Reagents","authors":"E. V. Petrova, A. F. Dresvyannikov, L. I. Kashfrazyeva","doi":"10.1134/S1087659624600479","DOIUrl":"10.1134/S1087659624600479","url":null,"abstract":"<p>Scientific principles for the synthesis of precursors of nanostructured oxide systems Al<sub>2</sub>O<sub>3</sub>–ZrO<sub>2</sub>–Ln<sub><i>x</i></sub>O<sub><i>y</i></sub> ((Ln = Dy, Nd) are developed. The features of their formation under conditions of rapid mixing of electrogenerated reagents, implemented in a diaphragm-free coaxial reactor-electrolyzer, are studied. The methods of potentiodynamic polarization curves, X-ray diffractometry, X-ray fluorescence, synchronous thermal analysis, and laser diffraction are used to study the anodic processes occurring in the electrolyzer, the morphology of particles formed in the solution and transformed during heat treatment, as well as the phase, granulometric, and elemental compositions of precursors and oxide systems. The proposed approach allows obtaining oxide systems modified with rare earth elements based on the Al<sub>2</sub>O<sub>3</sub>–ZrO<sub>2</sub> binary system, characterized by the presence of a stabilized phase of tetragonal zirconium dioxide. REE atoms present in the studied systems—Nd and Dy—stabilize <i>t</i>-ZrO<sub>2</sub> and, apparently, occupy the positions of crystal lattice nodes, isomorphically replacing Zr<sup>4+</sup>. The latter is indicated by the broadening of the corresponding reflections of X‑ray diffraction patterns. It indirectly indicates the presence of microstresses in the microcrystals of the phases. The latter can be caused by distortions of the crystal lattices of aluminum and zirconium oxides as a result of the substitution of metal atoms by REE atoms.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 6","pages":"660 - 667"},"PeriodicalIF":0.8,"publicationDate":"2025-03-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143676411","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 : 2025-03-03DOI: 10.1134/S1087659624600224
C. John Clement Singh, S. C. Jeyakumar, S. Murugavel, Abdulrahman I. Almansour, S. Sahaya Jude Dhas, Sivakumar Aswathappa, C. S. Biju
The ability to tailor the bandgap in semiconductor nanostructures from the ultraviolet to visible range is imperative in various light-mediated optoelectronic applications. In this work, Zn-doped TiO2 nanostructures were prepared and annealed at 350°C for different time intervals such as 1, 2, and 3 h to tailor the band gap. The effects of annealing time on the structural and optical properties of Zn-doped TiO2 nanostructures were investigated. According to XRD studies, increasing the annealing time authenticates that the dislocation density in the nanostructures decreases, whereas the crystallite size increases. TEM image of the sample annealed at 350°C for 3 h shows the average grain size distribution as 12.33 ± 0.12 nm. The XPS spectrum of the nanostructures that underwent a 3 h annealing at 350°C reveals a broad peak centered at 1021.06 eV, which indicates the Zn2+ oxidation state of Zn atoms. The photoluminescence studies indicate that the intensity of UV-visible luminescence bands changes with a rise in annealing time. UV-visible spectroscopic analysis reveals that the band gap increases from 3.32 to 3.36 eV and then decreases to 3.25 eV when the annealing time is raised linearly. Moreover, Zn-doped TiO2 that has been annealed at 350°C for 3 h has a red shift in the absorption edge and a reduction in the optical band gap, suggesting that it may find application in optoelectronic devices.
{"title":"Annealing Time-Driven Steering of the Structural, Morphological and Optoelectronic Characteristics of Zn-Doped TiO2 Nanostructures","authors":"C. John Clement Singh, S. C. Jeyakumar, S. Murugavel, Abdulrahman I. Almansour, S. Sahaya Jude Dhas, Sivakumar Aswathappa, C. S. Biju","doi":"10.1134/S1087659624600224","DOIUrl":"10.1134/S1087659624600224","url":null,"abstract":"<p>The ability to tailor the bandgap in semiconductor nanostructures from the ultraviolet to visible range is imperative in various light-mediated optoelectronic applications. In this work, Zn-doped TiO<sub>2</sub> nanostructures were prepared and annealed at 350°C for different time intervals such as 1, 2, and 3 h to tailor the band gap. The effects of annealing time on the structural and optical properties of Zn-doped TiO<sub>2</sub> nanostructures were investigated. According to XRD studies, increasing the annealing time authenticates that the dislocation density in the nanostructures decreases, whereas the crystallite size increases. TEM image of the sample annealed at 350°C for 3 h shows the average grain size distribution as 12.33 ± 0.12 nm. The XPS spectrum of the nanostructures that underwent a 3 h annealing at 350°C reveals a broad peak centered at 1021.06 eV, which indicates the Zn<sup>2+</sup> oxidation state of Zn atoms. The photoluminescence studies indicate that the intensity of UV-visible luminescence bands changes with a rise in annealing time. UV-visible spectroscopic analysis reveals that the band gap increases from 3.32 to 3.36 eV and then decreases to 3.25 eV when the annealing time is raised linearly. Moreover, Zn-doped TiO<sub>2</sub> that has been annealed at 350°C for 3 h has a red shift in the absorption edge and a reduction in the optical band gap, suggesting that it may find application in optoelectronic devices.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"418 - 427"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533219","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}
Glasses containing compositions of BaO–Bi2O3–B2O3–TMI (V2O5, MnO) were prepared and subjected to thorough analysis through differential scanning calorimetry (DSC), dielectric measurements and AC conductivity studies. The DSC investigations unveiled a noteworthy trend of an increase in TMI content correlated with a decrease in the glass transition temperature. Delving deeper into the properties of the prepared samples, the frequency dependence of dielectric constant and dielectric loss were explored. The investigation uncovered that AC conductivity experiences an augmentation at low and intermediate frequencies, plateauing at higher frequencies. Addition of TMI into the glass network induced a discernible rise in AC conductivity. Further investigation of the samples revealed a non-Debye behavior, a conclusion substantiated by the suppressed Cole–Cole plots and corroborated by electric modulus studies. Intriguingly, the addition of a minute concentration of TMI, whether it is vanadium or manganese, did not exert an influence on the relaxation time of ions. However, it exerts an impact on the dissipation energy of the samples, thus attesting to the nuanced and specific role played by TMI in modulating the electrical properties of the glass network.
{"title":"Thermal, Dielectric and AC Conductivity Studies of Alkaline Earth Borobismuthate Glasses Doped with Transition Metal Ions","authors":"Pavan Kumar Pothuganti, Ashok Bhogi, Boora Srinivas, Muralidhara Reddy Kalimi, Padmasuvarna Renuguntla","doi":"10.1134/S1087659624600133","DOIUrl":"10.1134/S1087659624600133","url":null,"abstract":"<p>Glasses containing compositions of BaO–Bi<sub>2</sub>O<sub>3</sub>–B<sub>2</sub>O<sub>3</sub>–TMI (V<sub>2</sub>O<sub>5</sub>, MnO) were prepared and subjected to thorough analysis through differential scanning calorimetry (DSC), dielectric measurements and AC conductivity studies. The DSC investigations unveiled a noteworthy trend of an increase in TMI content correlated with a decrease in the glass transition temperature. Delving deeper into the properties of the prepared samples, the frequency dependence of dielectric constant and dielectric loss were explored. The investigation uncovered that AC conductivity experiences an augmentation at low and intermediate frequencies, plateauing at higher frequencies. Addition of TMI into the glass network induced a discernible rise in AC conductivity. Further investigation of the samples revealed a non-Debye behavior, a conclusion substantiated by the suppressed Cole–Cole plots and corroborated by electric modulus studies. Intriguingly, the addition of a minute concentration of TMI, whether it is vanadium or manganese, did not exert an influence on the relaxation time of ions. However, it exerts an impact on the dissipation energy of the samples, thus attesting to the nuanced and specific role played by TMI in modulating the electrical properties of the glass network.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"374 - 389"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533045","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 : 2025-03-03DOI: 10.1134/S1087659624600972
V. Ya. Shevchenko, A. S. Oryschenko, S. N. Perevislov
If we assume that two bodies are in contact and only the pressure between them changes, then the deformation of the material changes proportionally to the cube root of our pressure (Heinrich Hertz, 18841). The convergence of elastic bodies is proportional to the pressure to the power of 2/3, and not to the pressure to the power of one (M.S. Leibenson, 19472). Let us point out that the dependence of the form h = const F2/3 or F = const h3/2 occurs not only for balls but also when other finite bodies come into contact (L.D. Landau and E.M. Lifshitz, 19533).
{"title":"On One Fundamental Property of the Contact (Impact) of Rigid Elastic Bodies","authors":"V. Ya. Shevchenko, A. S. Oryschenko, S. N. Perevislov","doi":"10.1134/S1087659624600972","DOIUrl":"10.1134/S1087659624600972","url":null,"abstract":"<p>If we assume that two bodies are in contact and only the pressure between them changes, then the deformation of the material changes proportionally to the cube root of our pressure (Heinrich Hertz, 1884<sup>1</sup>). The convergence of elastic bodies is proportional to the pressure to the power of 2/3, and not to the pressure to the power of one (M.S. Leibenson, 1947<sup>2</sup>). Let us point out that the dependence of the form <i>h</i> = const <i>F</i> <sup>2/3</sup> or <i>F</i> = const <i>h</i><sup>3/2</sup> occurs not only for balls but also when other finite bodies come into contact (L.D. Landau and E.M. Lifshitz, 1953<sup>3</sup>).</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"341 - 346"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533042","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 : 2025-03-03DOI: 10.1134/S1087659624600492
E. A. Balabanova, S. I. Lopatin, N. G. Tyurnina, Z. G. Tyurnina, S. M. Shugurov, I. G. Polyakova, D. A. Repin
The processes of vaporization and thermodynamic properties of melts of the BaO–Al2O3–SiO2 system are studied using the method of high-temperature differential mass spectrometry in the concentration range from 90 to 10 mol % BaO and molar ratio of x(Al2O3) : y(SiO2), equal to 3 : 2, 1 : 1, and 1 : 2. The samples are evaporated from Knudsen effusion cells made of tungsten. The partial pressures of gaseous species, activities of condensed phase components, Gibbs energies, and excess Gibbs energies are determined. It is established that the studied system is characterized by a negative deviation from ideal behavior.
{"title":"Vapor Formation and Thermodynamic Properties of Melts of the BaO–Al2O3–SiO2 System","authors":"E. A. Balabanova, S. I. Lopatin, N. G. Tyurnina, Z. G. Tyurnina, S. M. Shugurov, I. G. Polyakova, D. A. Repin","doi":"10.1134/S1087659624600492","DOIUrl":"10.1134/S1087659624600492","url":null,"abstract":"<p>The processes of vaporization and thermodynamic properties of melts of the BaO–Al<sub>2</sub>O<sub>3</sub>–SiO<sub>2</sub> system are studied using the method of high-temperature differential mass spectrometry in the concentration range from 90 to 10 mol % BaO and molar ratio of <i>x</i>(Al<sub>2</sub>O<sub>3</sub>) : <i>y</i>(SiO<sub>2</sub>), equal to 3 : 2, 1 : 1, and 1 : 2. The samples are evaporated from Knudsen effusion cells made of tungsten. The partial pressures of gaseous species, activities of condensed phase components, Gibbs energies, and excess Gibbs energies are determined. It is established that the studied system is characterized by a negative deviation from ideal behavior.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"402 - 410"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533221","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 : 2025-03-03DOI: 10.1134/S1087659624600960
T. A. Tsyganova, A. Sokolov, Ya. P. Lushankin, M. V. Staritsyn, L. N. Kurilenko, I. N. Anfimova
This paper presents the results of a study of the toxicity of high-silica quartzoid glasses (QGs) containing cesium, obtained on the basis of two-phase alkali borosilicate glass. It is established that the toxicity of the studied QGs in relation to Paramecium caudatum does not exceed the permissible level and varies depending on the content of alkaline ions in the QG and the time of contact of fine QG powder with water. It is assumed that the identified toxicity is associated primarily with the extraction of sodium and cesium ions into the aqueous solution.
{"title":"Toxicity of Quartzoid Glasses Containing Cesium","authors":"T. A. Tsyganova, A. Sokolov, Ya. P. Lushankin, M. V. Staritsyn, L. N. Kurilenko, I. N. Anfimova","doi":"10.1134/S1087659624600960","DOIUrl":"10.1134/S1087659624600960","url":null,"abstract":"<p>This paper presents the results of a study of the toxicity of high-silica quartzoid glasses (QGs) containing cesium, obtained on the basis of two-phase alkali borosilicate glass. It is established that the toxicity of the studied QGs in relation to <i>Paramecium caudatum</i> does not exceed the permissible level and varies depending on the content of alkaline ions in the QG and the time of contact of fine QG powder with water. It is assumed that the identified toxicity is associated primarily with the extraction of sodium and cesium ions into the aqueous solution.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"398 - 401"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533220","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 : 2025-03-03DOI: 10.1134/S1087659623601120
Madival Harish, M. Chethan, M. Sudhakara Reddy, Asha Rajiv
Bioactive glasses with a composition of (80 – x)NaPO3–xB2O3–5CaF2–15MgO, where x varies from 20 to 40 mol % were prepared through the melt quench technique. To examine the amorphous characteristics of the glasses and any structural modifications, X-ray diffraction (XRD) and Fourier-transform infrared spectroscopy (FTIR) analysis were conducted, respectively. The density of the fabricated glasses decreased as the B2O3 composition ranged from 20 to 40 mol %. Furthermore, the glasses were immersed in simulated body fluid (SBF) solution for 21 days for in vitro bioactivity studies. After this period, the development of apatite on the glass surfaces was assessed through XRD, FTIR, scanning electron microscope (SEM), and energy dispersive X-ray spectroscopy (EDX) technique. The EDX analysis reveals an elevation in the levels of boron and calcium in the glasses that were immersed in the SBF solution for 21 days. This increase underscores the material’s bioactivity and its potential to facilitate bone regeneration and ensure long-term stability. These findings position it as a promising material for use in applications related to bone regeneration and tissue engineering. The thermal properties of the glasses were analyzed through differential scanning calorimetry (DSC), and the glass transition temperature (Tg) was determined. Interestingly, the prepared glasses revealed the presence of a boron anomaly. By systematically varying the level of B2O3 to NaPO3 substitutions in the glass system, the effect of composition on several important properties is elucidated.
{"title":"Structural Characteristics and Thermal Properties of Bioactive Glasses Doped with Boron Oxide","authors":"Madival Harish, M. Chethan, M. Sudhakara Reddy, Asha Rajiv","doi":"10.1134/S1087659623601120","DOIUrl":"10.1134/S1087659623601120","url":null,"abstract":"<p>Bioactive glasses with a composition of (80 – <i>x</i>)NaPO<sub>3</sub>–<i>x</i>B<sub>2</sub>O<sub>3</sub>–5CaF<sub>2</sub>–15MgO, where <i>x</i> varies from 20 to 40 mol % were prepared through the melt quench technique. To examine the amorphous characteristics of the glasses and any structural modifications, X-ray diffraction (XRD) and Fourier-transform infrared spectroscopy (FTIR) analysis were conducted, respectively. The density of the fabricated glasses decreased as the B<sub>2</sub>O<sub>3</sub> composition ranged from 20 to 40 mol %. Furthermore, the glasses were immersed in simulated body fluid (SBF) solution for 21 days for in vitro bioactivity studies. After this period, the development of apatite on the glass surfaces was assessed through XRD, FTIR, scanning electron microscope (SEM), and energy dispersive X-ray spectroscopy (EDX) technique. The EDX analysis reveals an elevation in the levels of boron and calcium in the glasses that were immersed in the SBF solution for 21 days. This increase underscores the material’s bioactivity and its potential to facilitate bone regeneration and ensure long-term stability. These findings position it as a promising material for use in applications related to bone regeneration and tissue engineering. The thermal properties of the glasses were analyzed through differential scanning calorimetry (DSC), and the glass transition temperature (<i>T</i><sub>g</sub>) was determined. Interestingly, the prepared glasses revealed the presence of a boron anomaly. By systematically varying the level of B<sub>2</sub>O<sub>3</sub> to NaPO<sub>3</sub> substitutions in the glass system, the effect of composition on several important properties is elucidated.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"363 - 373"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533263","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 : 2025-03-03DOI: 10.1134/S1087659624600947
O. A. Golovanova
Substituted apatites with a varying content of La3+ and Ce3+ ions are synthesized. The formation of substituted hydroxyapatite (La-HA, Ce-HA) is proved by XRD and IR spectroscopy. The change in the crystal lattice parameters of the synthesized phases is shown, which indicates the replacement of Ca2+ ions by REE ions in the hydroxyapatite structure. The presence of REE ions in solid phases is proved by ICP–AES. When studying the resorption of the synthesized samples, it is found that cation-substituted hydroxyapatites are less soluble than undoped HA.
{"title":"Synthesis of Hydroxyapatite Substituted by REE Ions (La3+, Ce3+), and Study of the Composition, Structure, and Properties of the Obtained Samples","authors":"O. A. Golovanova","doi":"10.1134/S1087659624600947","DOIUrl":"10.1134/S1087659624600947","url":null,"abstract":"<p>Substituted apatites with a varying content of La<sup>3+</sup> and Ce<sup>3+</sup> ions are synthesized. The formation of substituted hydroxyapatite (La-HA, Ce-HA) is proved by XRD and IR spectroscopy. The change in the crystal lattice parameters of the synthesized phases is shown, which indicates the replacement of Ca<sup>2+</sup> ions by REE ions in the hydroxyapatite structure. The presence of REE ions in solid phases is proved by ICP–AES. When studying the resorption of the synthesized samples, it is found that cation-substituted hydroxyapatites are less soluble than undoped HA.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"444 - 452"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533044","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 : 2025-03-03DOI: 10.1134/S1087659624600984
V. Ya. Shevchenko, G. D. Ilyushin
Using computer methods (ToposPro software package), a combinatorial-topological analysis and modeling of the self-assembly of Li40P4Ge20-oP64 (V = 1082.85 Å3, Pnma) and Ti40P24-oP64 (V = 955.14 Å3, Pnma) crystalline structures is carried out. For the crystal structure of Li40P4Ge20-oP64, 36 variants of the identification of cluster structures with the number of clusters N = 2, 3, and 4 are established. The self-assembly of a crystal structure with the participation of clusters-precursors K11 = 0@11(Li5(LiGe5)) is considered in the form of pentagonal pyramids LiGe5 with five Li atoms located on five faces of the pyramid, rings K3 = @3(Li2P), and Li spacer atoms. For the crystal structure of Ti40P24-oP64, 55 variants of the identification of cluster structures with the number of clusters N = 2, 3, 4, and 6 are established. The self-assembly of a crystal structure involving clusters-precursors in the form of six-atom double tetrahedra, K6(4a) = 0@6(Ti4P2), K6(4b) = 0@6 (Ti4P2), three-atom rings K3 = 0@3(TiP2) and K3 = 0@3(Ti2P), and tetrahedrons K4 = 0@4 (Ti3P) is considered. The symmetric and topological code of the self-assembly processes of 3D Li40P4Ge20-oP64 and Ti40P24-oP64 structures from clusters-precursors is reconstructed in the following form: primary chain → layer → framework.
{"title":"Cluster Self-Organization of Intermetallic Systems: New Clusters-Precursors K3, K4, K6, and K11 for the Self-Assembly of Crystal Structures of the Li40P4Ge20-oP64 and Ti40P24-oP64 Families","authors":"V. Ya. Shevchenko, G. D. Ilyushin","doi":"10.1134/S1087659624600984","DOIUrl":"10.1134/S1087659624600984","url":null,"abstract":"<p>Using computer methods (ToposPro software package), a combinatorial-topological analysis and modeling of the self-assembly of Li<sub>40</sub>P<sub>4</sub>Ge<sub>20</sub>-<i>oP</i>64 (<i>V</i> = 1082.85 Å<sup>3</sup>, <i>Pnma</i>) and Ti<sub>40</sub>P<sub>24</sub>-<i>oP</i>64 (<i>V</i> = 955.14 Å<sup>3</sup>, <i>Pnma</i>) crystalline structures is carried out. For the crystal structure of Li<sub>40</sub>P<sub>4</sub>Ge<sub>20</sub>-<i>oP64</i>, 36 variants of the identification of cluster structures with the number of clusters <i>N</i> = 2, 3, and 4 are established. The self-assembly of a crystal structure with the participation of clusters-precursors <i>K</i>11 = 0@11(Li<sub>5</sub>(LiGe<sub>5</sub>)) is considered in the form of pentagonal pyramids LiGe<sub>5</sub> with five Li atoms located on five faces of the pyramid, rings <i>K</i>3 = @3(Li<sub>2</sub>P), and Li spacer atoms. For the crystal structure of Ti<sub>40</sub>P<sub>24</sub>-<i>oP64</i>, 55 variants of the identification of cluster structures with the number of clusters <i>N</i> = 2, 3, 4, and 6 are established. The self-assembly of a crystal structure involving clusters-precursors in the form of six-atom double tetrahedra, <i>K</i>6(4a) = 0@6(Ti<sub>4</sub>P<sub>2</sub>), <i>K</i>6(4b) = 0@6 (Ti<sub>4</sub>P<sub>2</sub>), three-atom rings <i>K</i>3 = 0@3(TiP<sub>2</sub>) and <i>K</i>3 = 0@3(Ti<sub>2</sub>P), and tetrahedrons <i>K</i>4 = 0@4 (Ti<sub>3</sub>P) is considered. The symmetric and topological code of the self-assembly processes of 3D Li<sub>40</sub>P<sub>4</sub>Ge<sub>20</sub>-<i>oP</i>64 and Ti<sub>40</sub>P<sub>24</sub>-<i>oP64</i> structures from clusters-precursors is reconstructed in the following form: primary chain → layer → framework.</p>","PeriodicalId":580,"journal":{"name":"Glass Physics and Chemistry","volume":"50 4","pages":"331 - 340"},"PeriodicalIF":0.8,"publicationDate":"2025-03-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"143533043","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}