Oriented lithium disilicate glass–ceramics prepared by electrochemically induced nucleation

Glasses with the compositions Li₂Si₂O₅ and 9Li₂Si₂O₅ · BaSiO₃ were crystallized using electrochemically induced nucleation. A platinum wire was inserted into the melt. A dc-current was supplied between the platinum wire (cathode) and the crucible (anode) at various temperatures below the liquidus temperature. This led to nucleation at the cathode and subsequently to radial growth of lithium disilicate crystals. The crystals exhibit dendritic growth. The main crystal growth direction is the crystallographic c-axis of lithium disilicate. This axis is oriented perpendicular to the electrode surface. A crystal growth selection near the cathode results in a highly textured glass–ceramics. The electrochemically induced nucleation is based on the reduction of the silicate glass to elementary silicon and an alloy formation between Si and Pt with a depletion of Si in the melt near the cathode. The crystalline products were characterized and the effects of experimental parameters were studied.     

Studies of crystal phase formations in high-strength lithium disilicate glass–ceramics

The objective of the study was to analyze the nucleation, primary phase formation and solid state reaction to form lithium disilicate glass–ceramics derived from the SiO₂–Li₂O–Al₂O₃–K₂O–ZrO₂–P₂O₅ system. The concentration of P₂O₅ was increased from zero up to 3.2 wt%. Thermal analysis, scanning electron microscopy and X-ray diffraction were used to characterize the microstructure formation, the nucleation process and the solid state reaction of the crystal phase precipitation in the glass–ceramics. Additives of P₂O₅ allowed the control of bulk crystallization. Nucleation was catalyzed by nano-scaled Li₃PO₄ phases, visualized by HR-SEM. Li₃PO₄ reacts most probably as the heterogeneous catalyst, acting by epitaxy, of both Li₂SiO₃ and Li₂Si₂O₅ crystals. Based on the discussion of the main results, the authors deduced a four-step reaction mechanism. This mechanism demonstrated that after nucleation of lithium metasilicate and lithium disilicate, the latter phase grows as agglomerated nanocrystals, but remained in a relative small amount. By contrast, lithium metasilicate grows rapidly and decomposes at 780–820 °C with the result of a drastic increase of lithium disilicate phase. This was a result of a solid state reaction with the SiO₂-rich glassy phase. In a parallel reaction, cristobalite was formed as a preliminary phase. The final product of a glass–ceramic with 3.2 wt% P₂O₅ shows a highly crystalline interlocking microstructure demonstrating a high-strength of 726 ± 63 MPa and translucency.     

A test of classical nucleation theory: crystal nucleation of lithium disilicate glass

For several inorganic glasses predictions have been made of the homogeneous crystal nucleation rate using classical nucleation theory. However, in none of these cases were comparisons made with experiment, due primarily to the inability of being able to guarantee homogeneous conditions. Evidence has been provided that crystalline formation in Li₂O · 2 SiO₂ glass may initiate by a homogeneous mechanism. Thus, we have computed the nucleation rate curve of lithium disilicate crystals in this glass. It is found that not only do all forms of the classical theory predict nucleation rates many orders of magnitude smaller than those observed, but also that the temperature dependence of the theoretical rate is quite different from that observed.     

In situ crystallization of lithium disilicate glass: Effect of pressure on crystal growth rate

Crystallization of a Li₂O · 2SiO₂ (LS₂) glass subjected to a uniform hydrostatic pressure of 4.5 and 6 GPa was investigated up to a temperature of 750 °C. The density of the compressed glass is ∼2% greater at 4.5 GPa than 1 atm and, depending on the processing temperature, up to 10% greater at 6 GPa. Crystal growth rates investigated as a function of temperature and pressure show that lithium disilicate crystal growth is an order of magnitude slower at 4.5 GPa than 1 atm resulting in a shift of +45 °C (±10 °C) in the growth rate curve at high pressure compared to 1 atm conditions. At 6 GPa lithium disilicate crystallization is suppressed entirely, while a new high pressure lithium metasilicate crystallizes at temperatures 95 °C (±10 °C) higher than those reported for lithium disilicate crystallization at 1 atm. The observed decrease in crystal growth rate with increasing pressure for the lithium disilicate glass up to 750 °C is attributed to an increase in viscosity with pressure associated with fundamental changes in glass structure accommodating densification.     

Ex situ XRD,TEM, IR,Raman and NMR spectroscopy of crystallization of lithium disilicate glass at high pressure

The structure of Li₂O · 2SiO₂ (LS₂) glass was investigated as a function of pressure and temperature up to 6 GPa and 750 °C, respectively, using XRD, TEM, IR, Raman and NMR spectroscopy. Glass densified at 6 GPa has an average Si–O–Si bond angle ∼7° lower than that found in glass processed at 4.5 GPa. At 4.5 GPa, lithium disilicate crystallizes from the glass, while at 6 GPa new high pressure form of lithium metasilicate crystallizes. This new phase, while having lithium metasilicate crystal symmetry, contains at least four different Si sites. NMR results for 6 GPa indicate the presence of Q⁴ species with (Q⁴)Si–O–Si(Q⁴) bond angles of ∼157°. This is the first reported occurrence of Q⁴ species with such large bond angles in alumina free alkali silicate glass. No five- or six-coordinated Si are found.     

Crystallization kinetics of lithium niobate films from limited volume of melt solution

The growth kinetics of LiNbO₃ films from a limited volume of melt solution is observed. We developed crystallization models describing the character of mass transfer in the liquid phase for isothermal and non-isothermal epitaxy. Analytical expressions have been derived connecting the film thickness with the system growth parameters. The experimental values being in good agreement with the calculated ones.     

Crystallization of a niobium phosphate glass

Niobium phosphate glasses with composition 37P₂O₅ · 23K₂O · 40Nb₂O₅ are stable in relation to crystallization during the heating process, exhibit a low critical cooling rate, and are potentially good for nuclear wasteforms. The crystallization of these glasses was evaluated by optical microscopy after proper heat treatments, showing that surface crystallization is the main process occurring during the heat treatment. Two main crystalline phases were observed. These crystalline phases were KNb₃O₈ and K₃NbP₂O₉. Surface crystal growth rates were measured in the temperature range of 806–972 °C (T_g = 683 °C) for both crystalline phases. Apparent crystallization enthalpies were determined through the Arrhenius plots of lnU vs. 1/T. The enthalpies are 496 kJ/mol and 513 kJ/mol for each crystalline phase, respectively. The surface density of nucleation sites (N_s) on 3 μm diamond paste polished surfaces is (2.4 ± 0.7) × 10⁸ nuclei/m² for one crystalline phase and (9.8 ± 0.8) × 10⁹ nuclei/m² for the other crystalline phase, when revealed at 838 °C/17.5 h, and these values show a slight variation depending on the time and the temperature. At the tested temperatures, only one crystal phase appeared inside the volume, and a volume density of nucleation sites N_v = 5 × 10⁶ nuclei/m³ was measured.     

Crystallization kinetic of glass particles prepared from a mixture of coal ash and soda-lime cullet glass

The crystallization capability of a parent glass made from a mixture of coal ash (40 wt%) and soda-lime glass was investigated using differential thermal analysis (DTA), X-ray diffraction (XRD) and scanning electron microscopy. Different glass particle size distributions were considered in the range 20-500 μm. Two crystallization exotherms in DTA were attributed to the formation of both pyroxenes (diopside Ca(Mg,Al)(Si,Al)₂O₆ and augite Ca(Mg,Fe)Si₂O₆) and plagioclase (Na,Ca)(Si,Al)₄O₈. These phases were confirmed by XRD analyses. Analysis of non-isothermal DTA data yielded values of 545 kJ/mol and 1.8 for the activation energy of crystallization and the Avrami exponent, respectively. This value for the Avrami exponent was consistent with a decreasing nucleation rate and the observed dendritic morphology. The data on crystallization kinetics obtained in this study are relevant for the production of glass-ceramic materials by a sintering/crystallization method from powder compacts made of this parent glass.     

Fabrication of a high lithium ion conducting lithium borosilicate glass

A lithium ion conducting glass, Li₂O-B₂O₃-SiO₂, is fabricated by the conventional melt and quenching technique from a mixture of Li₂CO₃, B₂O₃ and SiO₂ powders. It appears that B₂O₃ decreases the crystallization tendency of the Li₂O-SiO₂ binary glass, resulting in an expanded glass forming region in the Li₂O-B₂O₃-SiO₂ ternary glass. The maximum conductivity is 2 × 10^− 6 S cm^− 1 at 25 °C for the 50Li₂O-38B₂O₃-12SiO₂ glass sample. The observed high conductivity is due to the mixed former effect. The conductivity strongly depends on the Li₂O content, but not on K (SiO₂/B₂O₃) in the Li₂O-B₂O₃-SiO₂ ternary glass.     

Crystallization of glass fibers of the system Zn---Fe---Mn---oxides---alumina---silica

A glass composition based on the Zn---Al---silicate ternary system was modified with the addition of Fe and Mn oxides in order to test its feasibility to be drawn as alkaline-corrosion resistant glass fibers.

Their devitrification trend was studied, under dynamic thermal conditions, in order to define after which ternary diagram the resulting phases could be best described.

A beta-quartz structured silica rich phase, alpha-willemite and magnetite have been detected both in the fibers and in the bulk mass after crystallization. However, the differential thermal analysis patterns and the microstructures of the samples revealed very noticeable differences.     

Crystallization statistics,thermal history and glass formation

The formal theory of transformation kinetics describes the volume fraction of a phase transformed in a given time at a given temperature. The basic concepts are extended for isotropic crystal growth in a material having a known thermal history T(r, t). A crystal distribution function ψ(r, t, R) is defined such that the number of crystallites in a volume dυ at r having radii between R and R + dR at time t is ψ(r, t, R) dυ dR. The function ψ contains essentially complete statistical information about the state of crystallinity of a material. Formal expressions for ψ are obtained. Applications are discussed, including predictions of crystallinity when T(r, t) is known; predictions of glass-forming tendencies; experimental determination of nucleation rates; and the determination of the thermal history of a sample from post mortem crystallinity measurements. As an example, ψ(r, t, R) is calculated for a lunar glass composition subjected to a typical laboratory heat treatment.     

New insights on the thermodynamic barrier for nucleation in glasses: The case of lithium disilicate

An analysis is performed of the temperature dependence of the thermodynamic barrier to nucleation, W*(T), calculated from a fit of lithium disilicate glass data to the classical theory of nucleation. It is shown that, in order to obtain a satisfactory agreement between experimental and theoretical determinations of W*(T), lower values must be assigned to both the thermodynamic driving force and the surface energy as compared with the corresponding macroscopic values. This finding is consistent with theoretical considerations taking into account the effect that, in general, both the bulk and surface properties of the critical nuclei differ considerably from the respective properties of the newly evolving macroscopic phases. In addition, an anomalous increase of W*(T) with decreasing temperature is found near the glass transition interval. This increase is interpreted as a result of the effect of elastic strain on the thermodynamic driving force. The values of elastic strain energy estimated from the low temperature behavior of W*(T) are congruent with those calculated using the elastic constants of glass and crystal.     

The preparation and properties of cerium-activated lithium glass scintillators

We report the preparation of cerium activated lithium glass scintillators for thermal neutron detection and their properties. The technological requirements and appropriate compositions are proposed, by which high detection efficiency of lithium glass scintillators for thermal neutrons can be obtained. When used as neutron detectors, the ⁶Li glass ST-602 affords excellent pulse height discrimination against gamma radiation, particularly in the case of thin ⁶Li glass.     

Crystallization of CoFeSiB metallic glass induced by long-time ball milling

Milling up to 800 h causes amorphous Co_70.3Fe_4.7Si₁₀B₁₅ alloy, prepared in the form of thin ribbon, to partially crystallize thus forming a powder material consisting of an amorphous phase and fcc-Co nanocrystals with an average grain size of about 10 nm. A gradual increase of the nanocrystalline fcc-Co fraction, produced by ball milling, was detected. Prolonged milling results in destabilization of the fcc-Co phase and oxidation of the powder material (presence of CoO phase after 1500 h of milling). The thermal stability studies of as-quenched and milled Co_70.3Fe_4.7Si₁₀B₁₅ alloy emphasized a two step crystallization behavior. During the first crystallization event, cobalt rich phases, i.e., fcc-Co and hcp-Co crystallize, whereas after the second crystallization event, Co₂B and Co₂Si are formed.     

Investigation of the conductivity of the lithium borosilicate glass system

The lithium borosilicate system (Li₂O)_0.4(B₂O)_(0.6x)(Si₂O₄)_0.6(1−x) with x = 0, 0.2, 0.3, 0.4, 0.6, and 0.8 was investigated using impedance spectroscopy. Impedance spectra were taken in the frequency range from 50 Hz to 1 MHz and in the temperature range from 100 to 280 °C. The ac- and dc-conductivity, relaxation frequency and activation energy of the dc-conductivity were extracted from the impedance spectra. The dc-conductivity of the investigated glass samples increases almost linearly from silica rich (x = 0) to the boron rich (x = 0.8) samples. Activation energy (E_a) was found to be 0.65 eV for high conducting sample and 0.8 eV for low conducting sample, respectively. The mixed glass-former effect was not observed on the samples studied. The effect of temperature scaling of ac-conductivity was observed, which indicates, that ionic conductivity relaxation mechanism is temperature independent for samples with x = 0, 0.2, 0.3. However, some deviations from scaling were found for the samples with higher x (x = 0.4, 0.6, 0.8).     

Crystallization behavior in a highly driven marginal glass forming alloy

Al₉₀Sm₁₀, a marginal glass former, was rapidly solidified using Cu-block single roller melt spinning at wheel speeds of 30 and 40 m/s. The product phases of rapid solidification were identified and analyzed using high energy synchrotron X-ray diffraction (HEXRD), high resolution transmission electron microscopy, and atom probe tomography. The as-quenched structure consists of a saturated amorphous phase and nanocrystalline Al with typical length scale of about 5 nm. The appearance of a pre-peak on HEXRD diffraction patterns and a low activation energy for first crystallization as determined using the Kissinger and Ozawa methods indicate some local ordering in the amorphous phase. The devitrification phase transformation path was determined using in situ high energy synchrotron radiation. Three phases, MS1, H1, and Al₄Sm, were identified during decomposition of the amorphous phase. MS1, H1 and Al₄Sm are cubic, hexagonal and orthorhombic metastable phases, respectively.     

Further investigations of the effect of replacing lithium by sodium on lithium silicate scintillating glass efficiency

Ce³⁺ doped lithium (⁶Li) silicate glasses are thermal neutron detectors. Prior work showed that when sodium (Na) is substituted for Li the scintillation efficiency, under beta particle stimulation, increased and then decreased as the sodium (Na) content was increased. When all the ⁶Li was replaced by Na no scintillation was observed. Raman spectra, acquired using a visible excitation source, provided no evidence of anomalous behavior. SEM microscopy did show some phase separation, but there was no obvious correlation with the scintillation efficiency. We have reexamined these glass samples using deep UV Raman excitation which reduces fluorescence interference. The newly acquired spectra show evidence of phase separation in the glasses. Specifically we see a peak at 800 cm^? 1 Raman shift which can be assigned to a vitreous silica moiety that results from phase separation. There is a strong correlation between this peak's area, the scintillation efficiency, and the Na content. The observed trend suggests that phase separation enhances scintillation and addition of Na reduces the amount of phase separation. We also see evidence of at least two defect structures that can be tentatively assigned to a three-membered ring structure and an oxygen vacancy. The latter is fairly strongly correlated with enhanced scintillation efficiency.