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1.
Phosphate glasses having composition, 40Na 2O-10BaO-xB 2O 3-(50- x)P 2O 5, where x = 0–20 mol% were prepared using conventional melt quench technique. Density of these glasses was measured using Archimedes
principle. Microhardness (MH) was measured by Vicker’s indentation technique. Structural studies were carried out using IR
spectroscopy and 31P and 11B MAS NMR. Density was found to vary between 2.62 and 2.77 g/cc. MH was found to increase with the increase in boron content. 31P MAS NMR spectra showed the presence of middle Q 2 groups and end Q 1 and Q 0 groups with P-O-B linkages. FTIR studies showed the presence of BO 3 and BO 4 structural units along with the depolymerization of phosphate chains in conformity with 31P MAS NMR. 11B NMR spectra showed increase in BO 4 structural units with increasing boron content. The increase in MH with B 2O 3 content is due to the increase of P-O-B linkages and BO 4 structural units as observed from MAS NMR studies resulting in a more rigid borophosphate glass networks. 相似文献
2.
IR and Raman spectra of glass ceramics based on PbO-Cr 2O 3-B 2O 3glass composition system have been studied. The bands characteristic of BO 3. and BO 4 functional groups are present in all the samples. An incorporation of Al 2O 3(up to 5 mol%) in the initial glass composition considerably changes the glass network structure and relative concentrations of BO 3 and BO 4 groups. The composition 50 PbO-20 Cr 2O 3-25 B 2O 3-5 Al 2O 3(in mol%) reveals a maximum fraction of boron in the BO 4 group. A sample of this composition heat treated at 850° C for 25 h shows a maximum crystallization fraction with Pb 2O · CrO 4 as a prominent crystalline phase. The glasses irradiated with rays inhibit the crystallization into the Pb 2O · CrO 4 phase. They also show relatively smaller thermal conductivity. 相似文献
3.
A glass system was prepared according to the formula 75 mol % B 2O 3-(25 – x) mol % BaO – x mol % Fe 2O 3, where x = 0, 1, 2.5, 5, 7.5 and 10. The glasses were subjected to heat treatment at 550° C for 2, 6, 12, 18 and 24 h. The glasses were also irradiated using -rays at a dose of 4.805 × 10 4 rad h –1 for 12, 18 and 24 h. An X-ray diffraction technique was used to identify the separated crystalline phases. The electrical conductivity and activation energy of untreated, heat-treated and irradiated samples were measured and calculated. The rate and the dimensions of crystallization were also calculated by using the Avrami equation. It was found that -Fe 2O 3 is the separated phase when a sample containing 7.5 mol% Fe 2O 3 is heat treated for 24h; -Fe 2O 3 and Fe 2O 3 are the separated phases when the sample containing 10 mol% Fe 2O 3 is heat treated for 6, 12 and 18 h, with the addition of BaO when the sample is heat treated for 24 h. A miminum value for the electrical conductivity of glass samples was found to occur around an Fe 2O 3/BaO ratio of 0.425. The rate of crystallization in the sample containing 10 mol% Fe 2O 3 is 1.30607 × 10 –3 and the geometry of crystallization n is 1.2238, which indicates that the crystallization was in one dimension. 相似文献
4.
X-ray diffraction and infrared measurements were performed on vanadium borophosphate glass containing different amounts of
iron ranging from 0–7.5 mol % and heat treated at 300 °C for various times. The structure and phase separation could be determined
for each glass composition. V 2O 5 was the main precipitated phase in all heat-treated samples, and its amount was dependent on the heat-treatment time and
Fe 2O 3 content. Also FeP was detected in samples heat treated for 24 h. The infrared measurements showed the presence of both V 4+ and V 5+. The symmetry of V 2O
7
4−
and VO
4
3−
groups was found to increase with increasing Fe 2O 3 content. It was also found that some PO 4 changed to BO 3, forming a non-bridging oxygen. 相似文献
5.
Structural investigation of xFe 2O 3·(100 − x)[3B 2O 3·SrO] glass system, with 0 ≤ x ≤ 40 mol%, was performed by means of X-Ray diffraction (XRD), Fourier transform infrared (FTIR) and Raman spectroscopies.
The purpose of this work was to investigate the structural changes that appear in the 3B 2O 3·SrO glass matrix with the addition and increasing of iron ions content. The XRD pattern for the prepared samples shows that
vitreous phase is present only for x ≤ 40 mol%. For sample containing 50 mol% Fe 2O 3 was evidenced the presence of a unique crystalline phase, Fe 2O 3, embedded in an amorphous matrix. FTIR data show that BO 3 and BO 4 are the main structural units of the glass system and the iron ions are located in the network. The Raman spectrum of glass
matrix indicates a structure with several borate groups (di-, meta-, pyro-borate, etc.). In higher concentrations the iron
ions break the regulate glass network and determines the appearance of BO 4 isolated units. 相似文献
6.
FT-IR, Raman and UV–VIS experimental results were presented for xCuO·(100- x)[3Bi 2O 3·B 2O 3] glass system, where 0 ≤ x ≤ 50 mol%. The FT-IR measurements indicate the presence in xCuO·(100- x)[3Bi 2O 3·B 2O 3] glasses of BO 3, BO 4 units, BiO 3 pyramidal and distorted BiO 6 octahedral units and their dependence of CuO content. The Raman scattering data indicate that for 0 ≤ x ≤ 10 mol% the structure of studied glasses consist from BiO 3 pyramidal and distorted BiO 6 octahedral units, ring and chain type of metaborate groups, ortoborate and pyroborate groups. For higher concentration the
Raman spectra suggest that the structure become more disordered. The FT-IR and Raman bands characteristic for CuO were not
directly evidenced, but the absorption bands specific for the glass matrix are influenced by the presence of copper ions in
the glass network structure. The optical absorption confirms the presence of Cu 2+ in the CuO doped 3Bi 2O 3·B 2O 3 glass matrix. 相似文献
7.
Mixed lithium–zinc borophosphate glasses were prepared and studied in three compositional series xLi 2O–(50− x)ZnO–50P 2O 5, xLi 2O–(50− x)ZnO–10B 2O 3–40P 2O 5 and xLi 2O–(50− x)ZnO–20B 2O 3–30P 2O 5 with x = 0, 10, 20, 30, 40 and 50 mol% Li 2O. The obtained glasses were characterized by the measurements of the density (ρ), molar volume ( V
M), glass transition temperature ( T
g) and thermal expansion coefficient (α). For the investigation of structural changes 11B and 31P MAS NMR and Raman spectroscopy were applied. The replacement of zinc by lithium in borophosphate glasses slightly decreases V
M and T
g, while α increases. In Li–Zn metaphosphate glasses the compositional dependence of T
g reveals a minimum, while at the borophosphate series T
g decreases monotonously with increasing Li 2O content. Chemical stability of Li–Zn borophosphate glasses is very good for glasses with x = 0 –30 mol% Li 2O. Spectral studies showed in the glass series with 10 mol% B 2O 3 only the presence of BO 4 sites. In the glasses with 20 mol% B 2O 3 the presence of BO 3 and two BO 4 sites was revealed in ZnO-rich glasses and only one BO 4 site in Li 2O-rich glasses; the number of BO 3 groups decreases with increasing Li 2O content which is ascribed to the formation of P–O–Zn covalent bonds in ZnO-rich glasses. 相似文献
8.
Borosilicate glasses have been prepared using the high-temperature melt components of ingredients Gd 2O 3 doped borosilicate glasses. FTIR spectra were measured in the wavenumber range (4000–400 cm −1) to explore the state and influence of Gd 3+ ions in the structure of the glasses. Data indicated that B 2O 3 is acting as dual network formers (BO 3) and (BO 4) structural units whereas the gadolinium ions playing the role of network modifier in these glasses. Optical transmission spectra were recorded in the range 190–2500 nm and different optical parameters such as the direct and the indirect optical band gap, Urbach energy, refractive index and optical dielectric constant, have been determined. The molar refraction, electronic polarizability and the optical basicity results have been determined using the measured glass refractive indices. Gadolinium-doped borosilicate glasses are found to be characterized by different optical parameters. 相似文献
9.
The xSnO·(100 ? x)B 2O 3 (0 ≦ x ≦ 80) glasses were successfully prepared by a mechanical milling technique. The glass with 40 mol% SnO showed the maximum glass transition temperature of 347°C. The SnO-B 2O 3 milled glasses consisted of both BO 3 and BO 4 units, and the fraction of BO 4 units was maximized at the composition of 50 mol% SnO. The electrochemical properties of the milled glasses were examined using a simple three electrodes cell with a conventional liquid electrolyte. The glasses with high SnO content exhibited high charge capacities more than 1100 mAh g ?1 and discharge capacities more than 700 mAh g ?1 at the first cycle. The SnO-B 2O 3 milled glasses proved to work as anode materials for rechargeable lithium batteries. 相似文献
10.
(10Li 2O–20GeO 2–30ZnO–(40- x)Bi 2O 3– xFe 2O 3 where x = 0.0, 3, 6, and 9 mol%) glasses were prepared. A number of studies, viz. density, differential thermal analysis, FT-IR spectra,
DC and AC conductivities, and dielectric properties (constant ε′, loss tan δ, AC conductivity, σ
ac, over a wide range of frequency and temperature) of these glasses were carried out as a function of iron ion concentration.
The analysis of the results indicate that, the density and molar volume decrease with an increasing of iron content indicates
structural changes of the glass matrix. The glass transition temperature T
g and onset of crystallization temperature T
x increase with the variation of concentration of Fe 2O 3 referred to the growth in the network connectivity in this concentration range, while glass-forming ability parameter Δ T decrease with increase Fe 2O 3 content, indicates an increasing concentration of iron ions that take part in the network-modifying positions. The FT-IR
spectra evidenced that the main structural units are BiO 3, BiO 6, ZnO 4, GeO 4, and GeO 6. The structural changes observed by varying the Fe 2O 3 content in these glasses and evidenced by FTIR investigation suggest that the iron ions play a network modifier role in these
glasses while Bi 2O 3, GeO 2, and ZnO play the role of network formers. The temperature dependence of DC and AC conductivities at different frequencies
was analyzed using Mott’s small polaron hopping model and, the high temperature activation energies have been estimated and
discussed. The dielectric constant and dielectric loss increased with increase in temperature and Fe 2O 3 content. 相似文献
11.
Glasses of the xFe 2O 3·(100− x)[B 2O 3·SrO] system, with 0 ≤ x ≤ 30 mol% were studied by X-ray diffraction, density, optical microscopy and FT-IR spectroscopy measurements. The X-ray patterns
for the prepared system show that vitreous phase is present only in the sample with x < 40 mol%. For x ≥ 40 mol% in the studied samples is evidenced crystalline phase of Fe 2O 3. SEM measurements for the sample with x = 40 mol% shows that there are formed Fe 2O 3 microcrystallites with 10–20 μm dimension. FT-IR spectroscopy measurements shown that BO 3 and BO 4 are the main structural units of the glass system and the iron ions are located in the glass network. 相似文献
12.
Raman spectra of sodium borosilicate glasses with a wide range of Na 2O/B 2O 3 ratios were systematically measured. Variations of the spectra with glass composition were studied to interpret the implied
distribution of Na + ions between silicate and borate units. When Na 2O/B 2O 3 is less than 1, all Na + ions are associated with borate units as indicated by the absence of the 1100 cm −1 band of Si-O − non-bridging bond stretching. For the (1− x)Na 2O · SiO 2 · xB 2O 3 glass with x≦0.4 the peak-height ratio of the 950 cm −1 band to the 1080 cm −1 band was used to analyse semiquantitatively the distribution of the Na + ions between silicate and borate units. Sodium ions are divided between silicate and borate units approximately in proportion
to the amount of SiO 2 and B 2O 3 present in these glasses. Some of the high sodium content glasses were crystallized and their spectra were compared with
the bulk glass spectra. The distribution of Na + ions in the glass was quite different from their distribution after crystallization. Spectra of high silica glasses that
had been heat-treated for phase separation indicated exclusion of borate units from the silica network and the formation of
borate groups. For high boron content glasses, no change was observed on heat treatment. Raman bands due to borate groups
seem to be little affected by their environments.
Also affiliated with the Department of Geosciences. 相似文献
13.
A process has been proposed for the preparation of oxyfluoride glasses based on the SiO 2–B 2O 3–Bi 2O 3–ZnO–CaF 2 system at various ratios of batch components, and transparent glasses have been obtained at a temperature below 1000°C. According to X-ray diffraction data, all of the glasses are X-ray amorphous. The surface morphology of the glasses has been examined and their glass transition temperatures have been determined. Their local structure has been studied by IR spectroscopy and it has been shown that, independent of composition, the glasses contain complex polyborate anions formed by [BO 3] and [BO 4] groups. Bismuth is incorporated into the glass network to form Bi–O–Si bonds and [BiO 6] network-formers. 相似文献
14.
Pure and copper doped glasses with composition, x
Li
2
O-(40- x) Na
2
O-50 B
2
O
3-10 Bi
2
O
3, have been prepared over the range 0 ≤
x ≤ 40. The electron paramagnetic resonance (EPR) spectra of Cu 2+ ions of these glasses have been recorded in the X-band at room temperature. Spin Hamiltonian parameters have been calculated.
The molecular bonding coefficients, α 2 and β 2, have been calculated by recording the optical absorption spectra in the wavelength range 200–1200 nm. It has been observed
that the site symmetry around Cu 2+ ions is tetragonally distorted octahedral. The density and glass transition temperature variation with alkali content shows
non-linear behaviour. The IR studies show that the glassy system contains BO 3 and BO 4 units in the disordered manner. 相似文献
15.
Two different glass ceramics with the composition of the (Fe 2O 3) x·(B 2O 3) (60−x)·(ZnO) 40, where x = 12.5 and 15 mol%, have been synthesized using the melt-quench method. The X-ray diffraction (XRD) patterns show the presence
of nanometric zinc ferrite (ZnFe 2O 4) crystals, with spinel structure, in a glassy matrix after cooling from melting temperature. The estimated amount of crystallized
zinc ferrite varies between 16 and 35%, as a function of the chemical composition. Glass transition (T g), crystallization (T p) and melting (T m) temperatures were determined by differential thermal analysis (DTA) investigations. Fourier transform infrared (FTIR) data
revealed that the BO 3 and BO 4 are the main structural units of these glass ceramics network. FTIR spectra of these samples show features at characteristic
vibration frequencies of ZnFe 2O 4. Electron paramagnetic resonance (EPR) measurements show the presence of isolated Fe 3+ ions predominantly situated in rhombic vicinities and as well as the Fe 3+ species interacting by dipole–dipole interaction or to their superexchange coupled pairs in clustered formations. The magnetic
properties of the studied glass ceramics were investigated by vibrating sample magnetometer (VSM). From the magnetization
curves for glass ceramic containing 15 mol% Fe 2O 3 it was found that the nanoparticles exhibit ferromagnetic interactions combined with superparamagnetism with a blocking temperature,
T B. For studied samples the hysteresis is present. The coercive field is dependent on composition and magnetic field being around
0.05 μ B/f.u for measurements performed in maximum 0.4 T. 相似文献
16.
Some ternary Gd 2O 3–Bi 2O 3–B 2O 3 glasses are prepared, and crystallization behavior and second harmonic intensity are examined to develop new non-linear optical crystallized glasses. The glasses with Gd 2O 3 contents of 8–14 mol% have large densities of over 6 g/cm 3 and large refractive indices of ~ 1.9. Transparent surface crystallized glasses consisting of two kinds of crystalline phases with different morphologies, i.e. plate shape and needle shape crystals, are fabricated by heat-treatment at temperatures between glass transition and crystallization temperatures. From second harmonic generation microscope observations, micro-Raman scattering spectra and XRD analyses, plate shape crystals are determined to be non-linear optical Gd xBi 1KxBO 3 and needle shape crystals are Bi 3B 5O 12 having no second-order optical non-linearity. Since crystallized glasses consisting of Gd xBi 1KxBO 3 crystals exhibit relatively strong SHGs, they have a high potential for application to light control devices. 相似文献
17.
The induced optical absorption spectra of 70GeO 2 ⋅ 10Ga 2O 3 ⋅ 20Li 2O glasses are measured. A process is described for producing photosensitive layers on alkali germanate glasses using ion-exchange diffusion from salt melts containing silver nitrate. The effects of the sensitizer (Ce 3+, Fe 3+, and Fe 2+) and preparation, UV irradiation, and heat treatment conditions on the mechanisms of silver reduction in the surface layer of germanate glasses are examined. The results demonstrate that colloidal silver particles can be produced via ion exchange at 350°C in glasses containing 0.1 wt % Fe 2O 3. The particle diameter in a glass prepared under reducing conditions is estimated at 2.5 nm.__________Translated from Neorganicheskie Materialy, Vol. 41, No. 6, 2005, pp. 753–761.Original Russian Text Copyright © 2005 by Bocharova. 相似文献
18.
Structural properties of lead vanadate glasses containing La 3+ or Fe 3+ ions were investigated using X-ray diffraction, Fourier transform infrared spectroscopy and laser Raman spectroscopy. Crystalline Pb 2V 2O 7 was formed for the molar composition 66.7PbO-33.3V 2O 5. Incorporation of greater quantities of La 3+ into lead metavanadate glass caused the crystallization of Pb 2V 2O 7. Fourier transform infrared and laser Raman spectra also suggested the presence of LaVO 4. Incorporation of Fe 3+ ions into lead metavanadate glass, up to 20 wt% Fe 2O 3, did not cause crystallization inside the glass matrix. Changes in the vibrational spectra are discussed. 相似文献
19.
Glasses of the xEu 2O 3 · (100 − x)[4Bi 2O 3 · B 2O 3] system, with 0 ≤ x ≤ 40 mol% were studied by FT-IR spectroscopy and density measurements. FT-IR spectroscopy and density data suggest that the
europium ions play the network modifier role in the studied glasses. These data show that the glass structure consists on
the BiO 3, BiO 6, BO 3 and BO 4 units, and the conversion among these units mainly depends on the Eu 2O 3 content. 相似文献
20.
A series of (50 ? x) P2O5–20B2O3–20CaO–10Na2O (x?=?0–15 mol% MoO3) glass composition was prepared. Glass structure was analyzed using infrared absorption, UV–visible spectroscopy, electron spin resonance, density, and molar volume calculations. FTIR confirmed that Mo ions are contributed as MoO6 octahedral units in the glassy matrix, resulting in an increase in the pyrophosphate and BO3 groups at the expense of metaphosphate and BO4 units. UV–visible and ESR spectra detected Mo3+ and Mo5+ ions as species in the host glass due to the increase in MoO3 content. Broadband dielectric spectroscopy investigation on a broad range of frequencies and at different temperatures indicated that the enhancement of electrical conductivity of the prepared glasses due to molybdenum doping was prevented using confinement effect at the wells, causing demobilization of the charge carriers. Hence the dielectric spectra were caused by the mobility of charge carriers rather than the dynamics at the molecular scale. There is a clear correlation between the transport mechanism and dynamics at the interface of the charge carriers. Presently, the challenge is to understand if optimizing the accumulation of charges at the interfaces and electrodes is the origin of electrical storage energy. 相似文献
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