Thermodynamic modeling and Raman spectroscopy study of Na2O-TiO2-SiO2 glasses
Introduction
The main oxidation state of titanium in oxide glassy matrix prepared by conventional melt quenching is Ti4+, whereas the coordination number of the titanium ions can be 4, 5 or 6. When the coordination number is 4, Ti4+ ion is surrounded by oxygen tetrahedron. Five-fold coordinated Ti4+ ion occurs inside a square-based pyramid, where four oxygen atoms at an average distance of ∼1.9−2.0 Å from titanium form the base of the pyramid and fifth oxygen is at the apex of the pyramid at the shorter distance from titanium, ∼1.7 Å, (so-called titanyl bond) [1,2]. Finally, six-fold coordination of Ti4+ corresponds to an octahedral oxygen environment around titanium. Since an addition of TiO2 to oxide glasses significantly affects the physical and chemical glass properties (density, viscosity, heat capacity, thermal expansion, etc.), much attention has been paid to the study of the coordination state of titanium as a function of glass composition and temperature in different glass-forming systems, in particular to the Na2O-TiO2-SiO2 system [[2], [3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13]]. There is still no consensus, however, on the structure of Ti-containing glasses and structural role of Ti4+ ions in melts.
Raman spectroscopy is one of the powerful tools for structural characterizations of various (including non-crystalline) materials. In case of non-crystalline materials, structural assignment of Raman bands is usually based on comparison of spectra of glassy materials with those of crystalline compounds with well-known structure, which are formed in the system under consideration. In other words, the Raman spectra of crystalline materials are used as a benchmark for the identification of specific atomic groups in glassy material. This approach, however, does not necessarily yield an unambiguous result with respect to titanium coordination in silicotitanates [14]. This is due to the fact that the characteristic bands of TiO6 groups can be observed (or not be observed at all) at different frequency ranges of Raman spectra depending on the local bonding configurations around titanium. Therefore, as it was mentioned in Ref. [14], Raman spectroscopy does not represent a “stand-alone” technique for determining structure of silicotitanates. The more detail study of the structure of Ti-containing glasses requires the application of other experimental or theoretical methods along with Raman technique.
We previously reported the results of studying of xTiO2-(100-x)[40Na2O-60SiO2] (0 ≤ x ≤ 30 mol%) glasses based on qualitative analysis of the Raman spectra [13]. In this paper, more in-depth analysis of these glasses was carried out using deconvolution of the measured spectra in combination with a thermodynamic approach to modeling the structure of oxide glasses developed by Shahkmatkin and Vedishcheva [15,16].
Section snippets
Thermodynamic model of Shakhmatkin and Vedishcheva
The thermodynamic model of Shakhmatkin and Vedishcheva (SVTDM) considers the oxide glasses and melts as a medium formed from salt-like products of equilibrium chemical reactions between the initial reagents (oxides) and unreacted original oxides [15,16]. It is assumed that the salt-like products (so-called chemical groupings) have the same stoichiometry as the crystalline compounds existing in the equilibrium phase diagram of the system under consideration. The glass chemical structure is
SVTDM
Twenty following stable crystalline compounds in Na2O-TiO2-SiO2 system (Na2O, TiO2, SiO2, 3Na2O⋅8SiO2, Na2O⋅2SiO2, Na2O⋅SiO2, 3Na2O⋅2SiO2, 2Na2O⋅SiO2, 5Na2O⋅SiO2, Na2O⋅6TiO2, Na2O⋅3TiO2, Na2O⋅2TiO2, 4Na2O⋅5TiO2, Na2O⋅TiO2, 2Na2O⋅TiO2, Na2O⋅TiO2⋅4SiO2, Na2O⋅TiO2⋅2SiO2, Na2O⋅2TiO2⋅2SiO2, Na2O⋅2TiO2⋅SiO2, and Na2O⋅TiO2⋅SiO2) were taken into account for calculating the chemical structure of glasses in question. The molar Gibbs energies of pure oxides and binary compounds were taken from the FACT
Discussion
The structure of binary alkali silicate glasses has extensively been studied by many researchers using Raman spectroscopy. Therefore, the structural interpretation of the Raman bands for these systems is well developed [[25], [26], [27], [28], [29], [30], [31], [32]]. The low-frequency band at 595 cm−1 is due to the symmetric stretching and partially bending vibrational modes of Si-O-Si bridges. The other two high-frequency bands, 953 and 1090 cm−1, are due to the vibrations of terminal oxygen
Conclusions
A set of NTS glasses with composition xTiO2-(100-x)[40Na2O-60SiO2] (0 ≤ x ≤ 30 mol%) was studied by thermodynamic modeling and Raman spectroscopy. The results of thermodynamic modeling in the framework of the SVTDM model have shown that the chemical structure of the studied glasses contains seven different chemical groupings (TiO2, SiO2, Na2O⋅2SiO2, Na2O⋅SiO2, Na2O⋅3TiO2, Na2O⋅TiO2, Na2O⋅TiO2⋅SiO2) and five SRO structures (TiO5, TiO6, Q4, Q3 and Q2). The coexistence of all the predicted SRO
CRediT authorship contribution statement
Armenak A. Osipov: Methodology, Investigation, Writing - original draft. Marek Liška: Conceptualization, Software, Writing - review & editing. Leyla M. Osipova: Investigation, Formal analysis, Writing - review & editing. Mária Chromčiková: Data curation, Formal analysis. Branislav Hruška: Validation, Visualization.
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
This study was supported by the Ministry of Science and Higher Education of the Russian Federation “Physico-chemical problems of the synthesis of technological materials and natural and synthetic minerals” (AAAA-A19-119042590024-1) as well as the Slovak Grant Agency for Science (grant No. VEGA 1/0064/18).
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