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1.
The third-order nonlinear optical susceptibilities χ(3) of M2O-B2O3 (M = Li, Na, K, Rb, Cs, and Ag) binary borate glasses have been measured by the third harmonic generation (THG) method. It is found that the enhancement of χ(3)by the structural change of BO3 units to BO4 units is small, while the enhancement of χ(3) due to the formation of non- bridging oxygen is rather significant. The effects of alkali cations on the χ(3) of alkali borate glasses are discussed in terms of the M-O bond character, focusing on the covalency of Li2O-B2O3 glasses. Comparison of the χ(3) values for Cs2O-B2O3 and Ag2O-B2O3 glasses which contain cations of comparable polarizability reveals that the χ(3) value is much greater for Ag2O-B2O3 glasses than for Cs2O-B2O3glasses, which is possibly due to the great contribution of Ag(4 dz2 + 5 s + 5 pz ) hybrid orbitals to the nonlinear optical response.  相似文献   

2.
Bismuth borate glasses from the system: 40Bi2O3–59B2O3–1Tv2O3 (where Tv=Al, Y, Nd, Sm, and Eu) and three glasses of composition: 40Bi2O3–60B2O3, 37.5Bi2O3–62.5B2O3 and 38Bi2O3–60B2O3–2Al2O3 were prepared by melt quenching and characterized by density, UV-visible absorption spectroscopy and differential thermal analysis (DTA) studies. Bismuth borate glasses exhibit a very strong optical absorption band just below their absorption edge. Glasses were devitrified by heat treatment at temperatures above their glass transition temperatures and the crystalline phases produced in them were characterized by Fourier transform infrared (FTIR) absorption spectroscopy and X-ray diffraction (XRD). Bi3B5O12 was found to be the most abundant phase in all devitrified samples. DTA studies on glasses and FTIR and XRD analysis on crystallized samples revealed that very small amounts of trivalent ion doping causes significant changes in the devitrification properties of bismuth borate glasses; rare-earth ions promote the formation of metastable BiBO3–I and BiBO3–II phases during glass crystallization.  相似文献   

3.
Photochemical hole burning (PHB) not only can be applied for data storage systems but also serves as a powerful method for studying the local structure around optical centers. The present work investigated the effects of aluminum, magnesium, and silicon ions on hole burning and the phonon sideband for borate glasses that exhibit PHB at room temperature. Hole burning was measured for the 5 D 0−7 F 0 transition of Sm2+ and the phonon sideband spectrum for the 5 D 0-7 F 0 transition of Eu3+. The hole width was closely related to local structural change, especially as it seemed to decrease with decreases in the number of nonbridging oxygens produced around the rare-earth ions. In the case of sodium aluminoborate glasses, the hole width decreased considerably with increasing alumina content. The ratio Γihh for 85B2O3·10Al2O3·5Na2O·1Sm2O3 glass, then, was 80 at room temperature, the largest value ever reported.  相似文献   

4.
The glass transition temperature increases and the thermal expansion coefficient and density decrease with increasing B2O3 concentration in a series of (100− x )(50BaO–50P2O5)− x B2O3 where x =0–10 mol% for bulk samples. According to Raman spectroscopy, the bulk BaO–P2O5–B2O3 (BaP–B) glasses consist of metaphosphate Q 2 units with ring-type metaborate, diborate, and PO4–BO4 groups. X-ray photoelectron spectroscopy results reveal qualitatively that P–O–B bonds are formed at the surface of BaP–B glass samples ground in laboratory air over 6 mol% B2O3 only. The P–O–B bonds are related to the suppression of the crystallization of powdered BaP–B glasses with >6 mol% B2O3 during differential thermal analysis.  相似文献   

5.
Because of their thermal, dielectric, and optical properties, new glass compositions and thick-filmed transparent dielectrics containing neodymium oxide (Nd2O3) were studied as a source of purer images in plasma display panels. In the present study, PbO–B2O3–SiO2 and PbO–B2O3–SiO2–ZnO–Al2O3 were used as starting glass compositions, to which up to 25 wt% of Nd2O3 then was added. Increased amounts of Nd2O3 increased the glass transition temperature and dielectric constant of the bulk glasses and decreased the coefficient of thermal expansion. The fired thick films (around 30 μm) allowed selectively visible light to penetrate and showed deep absorption properties at 585 nm that were related to an extraneous gas from neon discharge.  相似文献   

6.
Crystallization of the poorly durable Na2MoO4 phase able to incorporate radioactive cesium must be avoided in SiO2–Al2O3–B2O3–Na2O–CaO glasses developed for the immobilization of Mo-rich nuclear wastes. Increasing amounts of B2O3 and MoO3 were added to a SiO2–Na2O–CaO glass, and crystallization tendency was studied. Na2MoO4 crystallization tendency decreased with the increase of B2O3 concentration whereas the tendency of CaMoO4 to crystallize increased due to preferential charge compensation of BO4 entities by Na+ ions. 29Si MAS NMR showed that molybdenum acts as a reticulating agent in glass structure. Trivalent actinides surrogate (Nd3+) were shown to enter into CaMoO4 crystals formed in glasses.  相似文献   

7.
The infrared absorption spectra of fused B2O3 and of a series of soda borate glasses are presented. These spectra were obtained using vacuum-pressed briquettes of the powdered glass and powdered KBr. The spectrum of fused B2O3 shows quite definitely that this glass does not consist of a completely continuous triangularly coordinative network. It is shown that hydrogen bonds play an important part in the atomic arrangement of the glasses of zero or low soda content. The B2O3 glass apparently consists of complexes of an approximate unit (B9O14)- held together by hydrogen bonds. One in nine borons is tetrahedrally coordinated. The glasses of low soda content are similar. The spectra for soda concentrations greater than 15% did not permit the determination of the atomic arrangement with exactitude, but it is shown to be quite different from that found in glasses with 10% Na2O or less.  相似文献   

8.
Glass formation in the system Ln2O3-B2O3 (Ln = Nd, Sm) was studied. Glasses could be formed in the range from 0 to -28 mol% rare-earth oxide (Ln2O3), but liquid immiscibility in these systems limits the range of homogeneous glasses to 0 to 1.5 and 25 to 28 mol% Ln2O3. The infrared spectra indicate that the rare-earth-rich glasses are structurally similar to rare-earth metaborates (LnB3O6) which contain (B3O6)- chains. The variation in density, transformation temperature, thermal expansion coefficient, and transformation-range viscosity of these glasses with the size of the rare-earth ion is discussed. Glasses near the metaborate composition have a transformation temperature of =700°C, which is high for binary borate glasses. Glasses could not be formed in the systems EU2O3-, Gd2O3-, HO2O3-, and Er2O3-B2O3, even by quenching at =1300°C/s. The sudden lack of glass formation in the system Ln2O3-B2O3 with Ln3+ ions smaller than Sm3+ is explained on the basis of the size effect of the Ln3+ ion on the stability of (B3O6)- chains in these metaborates.  相似文献   

9.
A molecular dynamic simulation was performed for sodium borate glasses containing a small amount of Eu2O3 to investigate the local structures of cations in glass. A new potential VB-B in the form -A exp[-C(r - 0.239)2] was added to the regular modified Born-Mayer-Huggins-type potentials, ΦB-B, ΦB-O, and ΦO-O, to account for the directional tendency of the borate network structure. With this potential added, both the radial distribution of sodium borate glasses observed by small-angle X-ray diffraction and the change in coordination number of boron with sodium content obtained by NMR agreed well with the simulation. The average coordination number of Ed3+ ions in the simulated glasses varied from 7.5 to 8.6, depending on the composition of the host sodium borate glasses. The inhomogeneous line width of the 5D0-7Fz emission peak also changed, depending on the sodium content, with a maximum at 18 mol% NazO content; this result agrees well with experimental data obtained from laser-induced fluorescence spectra.  相似文献   

10.
Glasses with compositions x Bi2O3(75− x )B2O325Li2O3 for 0≤ x ≤40 mol% have been prepared using the normal melt-quenching technique. The optical absorption and reflection spectra were recorded at room temperature in the wavelength range 190–1100 nm. From the absorption edge studies, the values of the optical band gap ( E opt) and Urbach energy (Δ E ) have been evaluated. Optical parameters such as refractive index and complex dielectric constant have been determined. The dispersion of the refractive index is discussed in terms of the single-oscillator Wemple–DiDomenico model. Color parameters and color difference data L *, U *, V *, C *, h ue, W , Y e, Δ L *, Δ U *, Δ V *, Δ C *, and Δ E have been calculated.  相似文献   

11.
A glass scintillator which can be used as one of the main components of a slow-neutron time-of-flight spectrometer has been developed. This sodium aluminoborate glass containing 73 mole % B2O3 and 8.0 mole % Ce was melted under highly reducing conditions in a series of cerium-activated very high boron-containing glasses. This glass is water white with very high light transmittance for wave lengths greater than 3800 a. u. It has a neutron-detection efficiency which is 25 to 30% greater than any other known glass scintillator in the energy range 102 to 104 e.v. and is considerably better than any other type of detector. It was found that the neutron pulse height increases with increasing cerium content up to a maximum and then decreases with further increases in the cerium content. The molar content of cerium required to obtain a maximum pulse height for each B2O3 concentration increases linearly with the increase in the B2O3 content. However, the maximum pulse height decreases gradually with the B2O3 content from 17.0 arbitrary units at 54.5 mole % to 6.7 at 73.4 mole %. This lower pulse height is still considerably above the photomultiplier noise at room temperature.  相似文献   

12.
Polyhedral Arrangements in Lanthanum Aluminoborate Glasses   总被引:3,自引:0,他引:3  
We have used magic-angle spinning nuclear magnetic resonance (MAS NMR) and Raman spectroscopy to examine the polyhedral arrangements in ternary lanthanum aluminoborate glasses. We have characterized two glass-forming series: x Al2O3·(1− x )LaB3O6 and 0.25La2O3· y Al2O3(1− y )-B2O3. 11B MAS NMR reveals a decrease in the fraction of four-coordinated boron atoms with increases in the Al2O3 content in both series. 27Al MAS NMR has detected four-, five- and six-coordinated aluminum atoms in complex aluminoborate networks similar to those reported elsewhere for alkaline-earth aluminoborate glasses. Raman spectroscopy reveals a variety of borate and aluminoborate moieties, including isolated groups as well as methaborate chains and rings. These results indicate that the La3+ ion acts as a modifier to the aluminoborate network.  相似文献   

13.
Third-Harmonic Generation from Some Chalcogenide Glasses   总被引:1,自引:0,他引:1  
Third-order optical nonlinear susceptibilities (χ(3)) of some high-refractive-index chalcogenide glasses were evaluated from third-harmonic generation. Compared with oxide glasses whose χ(3) has been known, χ(3) of the present glasses was higher by an order of magnitude. The addition of selenium drastically increased χ(3). The highest χ(3) was 1.4 × 10–11 esu, being comparable with those of high-χ(3)-organic compounds. Further, χ(3) generally increased with increasing density in the present glasses.  相似文献   

14.
Transparent surface-crystallized glass-ceramics with molar compositions of 43SiO2–2B2O3–30SrO–25MgO–0.05Eu2O3–0.8Dy2O3 (sample GC-A) and 43SiO2–2B2O3–24SrO–6CaO–25MgO–0.05Eu2O3–0.8Dy2O3 (sample GC-B) were prepared by heat-treating the mother glasses at 850°C for 10 h. The precipitated phases in both glass-ceramics were (Sr1− x Ca x )2MgSi2O7, in which Eu2+ and Dy3+ ions were incorporated. Phosphorescence with emission peaks at 470 and 480 nm that is due to the 4 f 65 d –4 f 7 transition of Eu2+ ions was observed from samples GC-A and GC-B, respectively. The phosphorescence lasted for >5 h at room temperature.  相似文献   

15.
Eu2O3-doped aluminoborosilicate glasses were prepared in air at high temperature. Luminescence measurements were used to investigate a valence change from Eu3+ to Eu2+ ions in the aluminoborosilicate glasses. The results showed that the doped Eu3+ ions were partially reduced to Eu2+ in the Eu2O3:RO–Al2O3–B2O3–SiO2 (RO=CaO, SrO, BaO, Li2O) glasses, but not in the Eu2O3:RO–Al2O3–B2O3–SiO2 (RO=Na2O, K2O) glasses. The changes of Eu reduction with different RO components were discussed with the variation of optical basicity of RO and with different valency of R cations. The effects of co-doping BaO and ZnO in aluminoborosilicate glasses on Eu reduction were also investigated and discussed.  相似文献   

16.
A series of La2O3–HfO2–SiO2 glasses, approximately along the join 0.73SiO2–0.27( x HfO2–(1− x )La2O3), 0< x <0.3), was prepared using containerless processing techniques (aerodynamic levitation combined with laser heating in oxygen). The enthalpy of formation and enthalpy of vitrification at 25°C were obtained from drop solution calorimetry of these glasses and appropriate crystalline compounds in a molten lead borate (2PbO–B2O3) solvent at 702°C. The enthalpy of formation from crystalline oxides was exothermic and became less exothermic with increasing HfO2 content. Heat contents were measured by transposed temperature drop calorimetry and depended linearly on the HfO2 content. Differential scanning calorimetry showed that both the onset glass transition and the onset crystallization temperature of these glasses increased with increasing HfO2 content. Upon slow cooling in air, the glasses crystallized to a mixture of baddeleyite, cristobalite, lanthanum disilicate, and hafnon.  相似文献   

17.
The ultraviolet absorption of vanadium(V) in R2O-B2O3 glasses (R represents Li, Na, or K) and in aqueous buffer solutions was investigated. In glasses of variable R2O:B2O3 ratio, a change in the absorption spectra similar to the [VO4]3- → [VO3(OH)]2- change in aqueous solution was observed. It is suggested that vanadium(V) in these glasses may be present as either [VO4]3- or [VO3O1/2]2- (O1/2 indicates a bridging oxygen ion), depending on the basicity of the melt. The critical R2O concentration, above which this change in vanadium(V) environment occurs with increasing alkalinity, is 24, 26, and ≅30 mol%, for K2O, Na2O, and Li2O, respectively.  相似文献   

18.
The effects of various components on the thermal expansion coefficient of low-expansion Cu2O-Al2O3-SiO2 glasses were examined. When a component of glass was substituted by another oxide, the expansion coefficient always increased, except for substitution of Al2O3 by B2O3. This result indicates that the essential components to maintain the low expansivity are Cu2O, such trivalent oxides as Al2O3 and B2O3, and tetravalent oxide SiO2. Glasses of the systems Cu2O-Al2O3-B2O3, Cu2O-Al2O3-GeO2, and Cu2O-Al2O3-P2O5, which were derived by replacing SiO2 by other network-forming oxides, showed fairly low expansion coefficients compared with other conventional borate, germanate, and phosphate glasses. It was also found that the valence state of copper ions is important for the thermal expansion characteristics of these glasses; Cu+ ions contribute to the low expansion coefficient.  相似文献   

19.
High-speed photography (framing rate of 106 s-1) has been used to follow the formation and growth of damage in a number of oxide glasses when impacted with 1-mm-diameter steel balls at velocities of 150 m· s-1 or higher. Silicate, germanate, and borate glasses were studied in order to clarify the importance of "anomalous" vs "normal" elastic characteristics on their impact behavior. As expected it was found that glasses in these systems which are "anomalous" showed impact behavior which had earlier been seen in silica and borosilicate glass, whiie those glasses which are "normal" showed behavior similar to that shown by soda-lime silica glass. On the other hand, although B2O3 has been characterized as "normal," its impact, as well as its quasi-static behavior, appears to put it in a class by itself. In this case, no cracking is observed during loading up to 150 m·s-1, while radial and lateral cracking are seen during unloading.  相似文献   

20.
The integrated absorption cross section, the spontaneous emission probability, and the stimulated emission cross section of Yb3+ were determined in silicate, phosphate, borate, germanate, aluminate, gallate, and ZBLAN host glasses. The compositional dependence of the stimulated emission cross section of the 2F5/22F7/2 transition is determined mainly by the integrated absorption cross section in the glasses. A peak stimulated emission cross section above 1 pm2, which is the highest value in glasses, was obtained in a gallate glass with a composition of 40K2O·20Ta2O5. 40Ga2O3. The factors affecting the integrated absorption cross section are discussed using the Judd-Ofelt parameters of Er3+ calculated in previous studies.  相似文献   

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