Pub Date : 2023-06-01Epub Date: 2023-04-04DOI: 10.1016/j.nocx.2023.100183
D.I. Snorrason , S.M. Adalsteinsson , T.K. Tryggvason , D. Dagbjartsson , A.S. Ingason , F. Magnus
Amorphous metal coatings have great potential for corrosion protection but finding alloy compositions which form a stable amorphous structure can be an overwhelming task. We use combinatorial magnetron sputtering and X-ray analysis to map out the phase space of TaSiM (M = Al, Cr, Fe, Ti) alloys in order to identify amorphous compositions. Atomic percentages of above 10–15 at.% of each constituent yield amorphous coatings in all four systems. TaSiAl coatings are stable when annealed in air up to and including 550 °C whereas TaSiFe, TaSiCr and TaSiTi remain amorphous up to and including 750 °C. In particular, Ta35Si15Cr50 is almost unchanged at that temperature, and has a stable surface oxide shell less than 20 nm in thickness at 650 °C. The stability of these materials at high temperatures means that they could be suitable as anti-corrosion coatings in high temperature applications.
{"title":"Structural stability and oxidation resistance of amorphous TaSi-based ternary alloy coatings","authors":"D.I. Snorrason , S.M. Adalsteinsson , T.K. Tryggvason , D. Dagbjartsson , A.S. Ingason , F. Magnus","doi":"10.1016/j.nocx.2023.100183","DOIUrl":"10.1016/j.nocx.2023.100183","url":null,"abstract":"<div><p>Amorphous metal coatings have great potential for corrosion protection but finding alloy compositions which form a stable amorphous structure can be an overwhelming task. We use combinatorial magnetron sputtering and X-ray analysis to map out the phase space of TaSiM (M = Al, Cr, Fe, Ti) alloys in order to identify amorphous compositions. Atomic percentages of above 10–15 at.% of each constituent yield amorphous coatings in all four systems. TaSiAl coatings are stable when annealed in air up to and including 550 °C whereas TaSiFe, TaSiCr and TaSiTi remain amorphous up to and including 750 °C. In particular, Ta<sub>35</sub>Si<sub>15</sub>Cr<sub>50</sub> is almost unchanged at that temperature, and has a stable surface oxide shell less than 20 nm in thickness at 650 °C. The stability of these materials at high temperatures means that they could be suitable as anti-corrosion coatings in high temperature applications.</p></div>","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100183"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"44290629","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-06-10DOI: 10.1016/j.nocx.2023.100192
S.R. Elliott
Understanding the atomic structure of amorphous solids or glasses is a perennial, and ultimately insoluble, challenge, since the randomness involved means that structural information can only ever be obtained, from either experiment or structural modelling, in a statistical form, unlike the case for crystalline materials. The particular atomic structure, in a glass or crystal, is dictated by the underlying chemical bonding between the atoms. The question arises therefore, conversely, to what extent can one infer anything about the nature of the bonding in amorphous/glassy solids from some knowledge of the atomic structure? In this focused perspective article, I discuss the case of telluride glassy materials, and show that they represent a special case of bonding in chalcogenide materials. The near-linear axial structural configurations characteristic of certain telluride crystals, also prevalent in the corresponding glasses, and giving rise to a particular degree of linear medium-range structural order, are shown to arise from hyperbonding (e.g. three-centre/four-electron) interactions, rather than being associated with conventional (two-centre/two-electron) covalent bonds, as in other chalcogenide materials. These structural configurations are responsible for the unique ‘phase-change memory’ behaviour exhibited by some telluride materials. An experimental technique is proposed which should be capable of detecting such linear-character, medium-range structural order in telluride glasses.
{"title":"What can one infer about chemical bonding in glasses from their medium-range structural order?","authors":"S.R. Elliott","doi":"10.1016/j.nocx.2023.100192","DOIUrl":"10.1016/j.nocx.2023.100192","url":null,"abstract":"<div><p>Understanding the atomic structure of amorphous solids or glasses is a perennial, and ultimately insoluble, challenge, since the randomness involved means that structural information can only ever be obtained, from either experiment or structural modelling, in a statistical form, unlike the case for crystalline materials. The particular atomic structure, in a glass or crystal, is dictated by the underlying chemical bonding between the atoms. The question arises therefore, conversely, to what extent can one infer anything about the nature of the bonding in amorphous/glassy solids from some knowledge of the atomic structure? In this focused perspective article, I discuss the case of telluride glassy materials, and show that they represent a special case of bonding in chalcogenide materials. The near-linear axial structural configurations characteristic of certain telluride crystals, also prevalent in the corresponding glasses, and giving rise to a particular degree of linear medium-range structural order, are shown to arise from hyperbonding (e.g. three-centre/four-electron) interactions, rather than being associated with conventional (two-centre/two-electron) covalent bonds, as in other chalcogenide materials. These structural configurations are responsible for the unique ‘phase-change memory’ behaviour exhibited by some telluride materials. An experimental technique is proposed which should be capable of detecting such linear-character, medium-range structural order in telluride glasses.</p></div>","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100192"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"41492020","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-03-27DOI: 10.1016/j.nocx.2023.100181
Parker T. Freudenberger, Rebekah L. Blatt, Richard K. Brow
Particles of borophosphate glasses with the nominal molar compositions 16Na2O-(24-y)CaO-ySrO-xB2O3-(60-x)P2O5 (mol%), where 0 ≤ x ≤ 60 and y = 0, 12, and 24, were reacted in deionized water and in simulated body fluid (SBF) at 37 °C. For the dissolution experiments in water, the pH of the solution at the conclusion of the experiments increased systematically, from 2.1 to 9.5, for y = 0 glasses when ‘x’ increased from 0 to 60. The reaction rates over the first 8–24 h of dissolution in both SBF and deionized water followed linear kinetics, with reaction rates dependent on glass composition. For glass particles in SBF, replacing P2O5 with up to 20 mol% B2O3 decreased the dissolution rate (fraction dissolved) by two orders of magnitude, from 7.0 × 10−3 h−1 for x = 0 to 2.0 × 10−5 h−1 for x = 20. Further replacement of P2O5 by B2O3 increased dissolution rates by three orders of magnitude, to 2.3 × 10−2 h−1 at x = 60. The compositional dependence of the dissolution rates is explained by changes in the glass structure, with the most durable glasses possessing the greatest fraction of tetrahedral borophosphate sites in the glass network. Crystalline brushite was detected on Ca-glasses with 35 and 40 mol% B2O3, but the dominant precipitation phase on both the Ca- and Sr-glasses is an x-ray amorphous material constituted from orthophosphate and pyrophosphate anions.
{"title":"Dissolution rates of borophosphate glasses in deionized water and in simulated body fluid","authors":"Parker T. Freudenberger, Rebekah L. Blatt, Richard K. Brow","doi":"10.1016/j.nocx.2023.100181","DOIUrl":"10.1016/j.nocx.2023.100181","url":null,"abstract":"<div><p>Particles of borophosphate glasses with the nominal molar compositions 16Na<sub>2</sub>O-(24-y)CaO-ySrO-xB<sub>2</sub>O<sub>3</sub>-(60-x)P<sub>2</sub>O<sub>5</sub> (mol%), where 0 ≤ x ≤ 60 and y = 0, 12, and 24, were reacted in deionized water and in simulated body fluid (SBF) at 37 °C. For the dissolution experiments in water, the pH of the solution at the conclusion of the experiments increased systematically, from 2.1 to 9.5, for y = 0 glasses when ‘x’ increased from 0 to 60. The reaction rates over the first 8–24 h of dissolution in both SBF and deionized water followed linear kinetics, with reaction rates dependent on glass composition. For glass particles in SBF, replacing P<sub>2</sub>O<sub>5</sub> with up to 20 mol% B<sub>2</sub>O<sub>3</sub> decreased the dissolution rate (fraction dissolved) by two orders of magnitude, from 7.0 × 10<sup>−3</sup> h<sup>−1</sup> for x = 0 to 2.0 × 10<sup>−5</sup> h<sup>−1</sup> for x = 20. Further replacement of P<sub>2</sub>O<sub>5</sub> by B<sub>2</sub>O<sub>3</sub> increased dissolution rates by three orders of magnitude, to 2.3 × 10<sup>−2</sup> h<sup>−1</sup> at x = 60. The compositional dependence of the dissolution rates is explained by changes in the glass structure, with the most durable glasses possessing the greatest fraction of tetrahedral borophosphate sites in the glass network. Crystalline brushite was detected on Ca-glasses with 35 and 40 mol% B<sub>2</sub>O<sub>3</sub>, but the dominant precipitation phase on both the Ca- and Sr-glasses is an x-ray amorphous material constituted from orthophosphate and pyrophosphate anions.</p></div>","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100181"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"41321287","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-06-06DOI: 10.1016/j.nocx.2023.100152
U. Hoppe , R.K. Brow , A.C. Hannon , M.V. Zimmermann
{"title":"Erratum to “Structure of tin phosphate glasses by neutron and X-ray diffraction” [Journal of Non crystalline solids:X 2C (2019) 100017]","authors":"U. Hoppe , R.K. Brow , A.C. Hannon , M.V. Zimmermann","doi":"10.1016/j.nocx.2023.100152","DOIUrl":"10.1016/j.nocx.2023.100152","url":null,"abstract":"","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100152"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"47692072","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-06-09DOI: 10.1016/j.nocx.2022.100144
Kacper Januchta, Morten M. Smedskjaer
{"title":"Erratum to indentation deformation in oxide glasses: Quantification, structural changes, and relation to cracking [Journal of Non crystalline solids:X 1C (2019) 100007]","authors":"Kacper Januchta, Morten M. Smedskjaer","doi":"10.1016/j.nocx.2022.100144","DOIUrl":"10.1016/j.nocx.2022.100144","url":null,"abstract":"","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100144"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"44955614","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-06-06DOI: 10.1016/j.nocx.2023.100158
Doris Möncke , Hellmut Eckert
{"title":"Erratum to “Review on the structural analysis of fluoride-phosphate and fluoro-phosphate glasses” [Journal of Non Crystalline Solids:X 3C (2019) 100026]","authors":"Doris Möncke , Hellmut Eckert","doi":"10.1016/j.nocx.2023.100158","DOIUrl":"10.1016/j.nocx.2023.100158","url":null,"abstract":"","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100158"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"43100075","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-05-18DOI: 10.1016/j.nocx.2023.100190
Hyun Kim, Il Jung Yoon, Yong Gyu Choi
After assessing compositional dependence of thermal and optical properties of Ge-Ga-Se glasses, we introduce Te, via replacing Se, into Ge25Ga5Se70 and Ge35Ga5Se60 (mol%) glasses in an attempt to enhance their refractive index. In the case of Se-deficient Ge35Ga5Se60 composition, vitrification is achieved for Te content up to 20 mol%. In the case of Se-sufficient Ge25Ga5Se70 composition, however, formation of bulk glass is realized only when Te content ranges from 25 to 45 mol%. Being proportional to Te content, refractive index of Ge25Ga5Se30Te40 glass is measured to approach 2.855 at 10 μm, which is far superior to that of any commercialized selenide glasses for infrared-imaging applications. This compositionally tailored Ge25Ga5Se30Te40 glass is further verified to be compatible with the conventional precision glass molding process, and infrared-imaging performance of the resulting molded lens is as excellent as the existing selenide-glass-based lenses.
{"title":"Adjustment of refractive index of Ge-Ga-Se glass via Te addition for infrared-imaging applications","authors":"Hyun Kim, Il Jung Yoon, Yong Gyu Choi","doi":"10.1016/j.nocx.2023.100190","DOIUrl":"10.1016/j.nocx.2023.100190","url":null,"abstract":"<div><p>After assessing compositional dependence of thermal and optical properties of Ge-Ga-Se glasses, we introduce Te, via replacing Se, into Ge<sub>25</sub>Ga<sub>5</sub>Se<sub>70</sub> and Ge<sub>35</sub>Ga<sub>5</sub>Se<sub>60</sub> (mol%) glasses in an attempt to enhance their refractive index. In the case of Se-deficient Ge<sub>35</sub>Ga<sub>5</sub>Se<sub>60</sub> composition, vitrification is achieved for Te content up to 20 mol%. In the case of Se-sufficient Ge<sub>25</sub>Ga<sub>5</sub>Se<sub>70</sub> composition, however, formation of bulk glass is realized only when Te content ranges from 25 to 45 mol%. Being proportional to Te content, refractive index of Ge<sub>25</sub>Ga<sub>5</sub>Se<sub>30</sub>Te<sub>40</sub> glass is measured to approach 2.855 at 10 μm, which is far superior to that of any commercialized selenide glasses for infrared-imaging applications. This compositionally tailored Ge<sub>25</sub>Ga<sub>5</sub>Se<sub>30</sub>Te<sub>40</sub> glass is further verified to be compatible with the conventional precision glass molding process, and infrared-imaging performance of the resulting molded lens is as excellent as the existing selenide-glass-based lenses.</p></div>","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100190"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"44247989","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-06-06DOI: 10.1016/j.nocx.2023.100154
Philip S. Salmon , Gregory S. Moody , YoshikiIshii , Keiron J. Pizzey , Annalisa Polidori , Mathieu Salanne , Anita Zeidler , Michela Buscemi , Henry E. Fischer , Craig L. Bull , Stefan Klotz , Richard Weber , Chris J. Benmore , Simon G. MacLeod
{"title":"Erratum to “Pressure induced structural transformations in amorphous MgSiO3 and CaSiO3” [Journal of Non crystalline solids:X 3C (2019) 100024]","authors":"Philip S. Salmon , Gregory S. Moody , YoshikiIshii , Keiron J. Pizzey , Annalisa Polidori , Mathieu Salanne , Anita Zeidler , Michela Buscemi , Henry E. Fischer , Craig L. Bull , Stefan Klotz , Richard Weber , Chris J. Benmore , Simon G. MacLeod","doi":"10.1016/j.nocx.2023.100154","DOIUrl":"10.1016/j.nocx.2023.100154","url":null,"abstract":"","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100154"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"43869659","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2023-06-01Epub Date: 2023-05-02DOI: 10.1016/j.nocx.2023.100185
Claudia Borredon , Luis A. Miccio , Silvina Cerveny , Gustavo A. Schwartz
Quantitative structure-property relationship (QSPR) is a powerful analytical method to find correlations between the structure of a molecule and its physicochemical properties. The glass transition temperature (Tg) is one of the most reported properties, and its characterisation is critical for tuning the physical properties of materials. In this work, we explore the use of machine learning in the field of QSPR by developing a recurrent neural network (RNN) that relates the chemical structure and the glass transition temperature of molecular glass formers. In addition, we performed a chemical embedding from the last hidden layer of the RNN architecture into an m-dimensional Tg-oriented space. Then, we test the model to predict the glass transition temperature of essential amino acids and peptides. The results are very promising and they can open the door for exploring and designing new materials.
{"title":"Characterising the glass transition temperature-structure relationship through a recurrent neural network","authors":"Claudia Borredon , Luis A. Miccio , Silvina Cerveny , Gustavo A. Schwartz","doi":"10.1016/j.nocx.2023.100185","DOIUrl":"https://doi.org/10.1016/j.nocx.2023.100185","url":null,"abstract":"<div><p>Quantitative structure-property relationship (QSPR) is a powerful analytical method to find correlations between the structure of a molecule and its physicochemical properties. The glass transition temperature (T<sub>g</sub>) is one of the most reported properties, and its characterisation is critical for tuning the physical properties of materials. In this work, we explore the use of machine learning in the field of QSPR by developing a recurrent neural network (RNN) that relates the chemical structure and the glass transition temperature of molecular glass formers. In addition, we performed a chemical embedding from the last hidden layer of the RNN architecture into an <em>m</em>-dimensional <em>T</em><sub><em>g</em></sub>-oriented space. Then, we test the model to predict the glass transition temperature of essential amino acids and peptides. The results are very promising and they can open the door for exploring and designing new materials.</p></div>","PeriodicalId":37132,"journal":{"name":"Journal of Non-Crystalline Solids: X","volume":"18 ","pages":"Article 100185"},"PeriodicalIF":0.0,"publicationDate":"2023-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"50186007","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}