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1.
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   

2.
SiO2–Al2O3–Eu2O3 glasses were prepared for the composition 50siO2·(50 – x )Al2O3·xEu2O3, and their density, sound velocity, and elastic modulus were measured. The chemical shift of the AIK a band emission spectra and the isomer shift of 151Eu by Mössbauer effect were obtained to determine the coordination states of Al3+ and Eu3+ ions in these glasses. It was found that the coordination number of Eu3+ ions was 12 and that the average coordination number of A13+ ions was almost 5 in these glasses. By introducing Eu2O3, the packing of constituent ions was strongly enhanced and the elastic modulus increased in this system. The compositional dependence of the molar volume and elastic modulus were explained by these states of high coordination number for Eu3+ and low coordination number for Al3+ ions compared with those in the corresponding M2O3 crystals.  相似文献   

3.
Borate glasses containing 0.99–30.0 mol% EuO have been prepared under a reducing atmosphere and 151Eu Mössbauer effect measurements have been carried out at room temperature in order to examine the chemical state of Eu2+ ions in these glasses. Mössbauer spectra indicate that most of the europium ions are present as the divalent oxidation state. In dilute Eu2+-containing borate glasses, spectra are split due to paramagnetic hyperfine interactions in the glasses with low and high sodium contents. In concentrated Eu2+-containing borate glasses, line broadening results from the contribution of quadrupole splitting due to asymmetrical oxygen coordination around Eu2+ and the contribution of inhomogeneous broadening due to site-to-site variation. The compositional dependence of isomer shift and quadrupole interaction parameter can be related to the structural changes in the borate glass. The variation of the isomer shift has a good correlation with the optical basicity of glass, and the trend can be explained in terms of the covalent admixture with 6 s character. The Eu-O bond in the borate glasses is more ionic than that in EuTiO3 and EuZrO3, where the oxygen coordination number for Eu2+ is 12. The average coordination number for Eu2+ is found to be 12 in all of the present glasses.  相似文献   

4.
A series of rare earth molybdates, Y2− x Eu x (MoO4)3 for x =0.4, 0.8, 1.2, 1.6 and 2.0 were prepared by solid-state method and their crystal structures, photo luminescent characteristics were investigated. The powders are mainly studied for their red light emission efficiency under near UV excitation. The crystal structures of the powders were found to depend on annealing temperature and the yttrium concentration. Mixtures of monoclinic ( C 2 /c ) and orthorhombic ( Pba 2, Pbna ) structures were formed in varying proportions depending on the value of x and annealing temperatures (700°–800°C). The luminescence behavior depended on the resultant composition of the crystal phase and the Eu3+ concentration. The excitation spectra showed the characteristic and broad O→Mo charge transfer (CT) band of the MoO4 tetrahedra and the sharp intra-configurational 4 f –4 f transitions of Eu3+ in the host lattice. The integrated emission ratio (5D07F2/5D07F1) of Eu3+ depends on the annealing temperature and reveals that the local site symmetry of Eu3+ ions decreases with increasing concentration of Eu3+. The emission spectra obtained by exciting at 396 nm, gave highest red emission intensity for Y0.4Eu1.6(MoO4)3 annealed at 700°C/6 h among this series of samples.  相似文献   

5.
Tetragonal ( t ) ZrO2 nanoparticles have been obtained by a partial Eu3+→Zr4+ substitution, synthesized using a simple oxalate method at a moderate temperature of 650°C in air. The Eu3+ additive, 2 mol% used according to the optimal photoluminescence (PL), gives small crystallites of the sample. On raising the temperature further, the average crystallite size D grows slowly from 16 nm to a value as big as 49 nm at 1200°C. The Eu3+: t -ZrO2 nanoparticles have a wide PL spectrum at room temperature in the visible to near-IR regions (550–730 nm) in the 5D07FJ (Eu3+), J =1–4, electronic transitions. The intensity of the 5D07F4 group is as large as that of the characteristic 5D07F2 group of the spectrum in the forced electric-dipole allowed transitions. The enhanced t -ZrO2 phase stability and wide PL can be attributed to the combined effects of an amorphous Eu3+-rich surface and part of the Eu3+ doping of ZrO2 of small crystallites.  相似文献   

6.
Tm3+-Ho3+- and Tm3+-Ho3+-Eu3+-ion-codoped oxyfluoride transparent glass-ceramics containing PbF2 nanocrystals were prepared, and the near-infrared fluorescence properties of the Tm3+ ions were investigated for their potential use as a 1.4 μm amplifier. For all samples, the lifetime of the Tm3+:3 H 4 level increased with heat treatment because of the decrease of the phonon energy as PbF2 crystals were formed. Moreover, it was revealed that codoping with Ho3+ or Eu3+ was effective in suppressing the lifetime of the Tm3+:3 F 4 level by energy transfer to the Ho3+:5 I 7 or Eu3+:7 F 6 level. For the codoped samples, the heat treatments decreased the Tm3+:3 F 4 lifetime and increased the Tm3+:3 H 4 lifetime. This was attributed to the concentration of rare-earth ions in the fluoride crystallites. These properties improved the population inversion of the 1.4 μm transition.  相似文献   

7.
Orange- and Violet-Emitting Long-Lasting Phosphors   总被引:1,自引:0,他引:1  
Orange phosphorescence from Eu3+-activated CaO and SrO and violet phosphorescence from Pb2+-activated SrO were clearly observed after the materials had been excited with ultraviolet light. The orange phosphorescence resulted from 5 D 0 to 7 F 1 transitions of the Eu3+ ions and the violet from 3 P 0 to 1 S 0 transitions of the Pb2+ ions. The phosphorescence lasted >1 h. Trapped-electron centers and hole centers introduced into the CaO and SrO hosts by the ultraviolet light appear to have been responsible for generating the long-lasting phosphorescence.  相似文献   

8.
We report here the processing and properties of transparent glass and glass–ceramic nanocomposites in the Li2O–Ta2O5–SiO2–Al2O3 system in the presence of Eu2O3 as luminescent probe. The formation of the LiTaO3 crystal phase, the crystallite size, and the morphology with the progression of heat treatment have been examined by X-ray diffraction (XRD), transmission electron microscopy (TEM), and Fourier transformed infrared reflectance spectroscopy measurements. The crystallite sizes obtained from XRD and TEM are found to increase with heat-treatment time and vary in the range of 2–20 nm. The measured photoluminescence spectra exhibit emission transitions of 5D0,17F j ( j =0, 1, 2, 3, and 4) of Eu3+ ions. From the nature of the emission transitions, the site symmetry in the vicinity of Eu3+ ions has been found to be near C3v in the glass–ceramic nanocomposites. An inverse correlation has been observed between the asymmetric ratio ( I ED/ I MD) of Eu3+ ions and the dielectric constant (ɛr), with an increase in the heat-treatment time of glass, which is caused by the dipole–dipole interaction.  相似文献   

9.
Fluorescence emissions at both 1.31 and 1.55 μm communication windows were observed from Pr3+/Er3+ codoped Ge-As-Ga-S glasses with a single wavelength pumping at 986 nm. The lifetime of the Er3+:4 I 11/2 level decreased as the Pr3+ concentration increased, and that of the Pr3+:1 G 4 level increased as the Er3+ concentration increased. Energy transfer from the Er3+:4 I 11/2 level to the Pr3+:1 G 4 level was responsible for emission of the 1.31 μm fluorescence from the Pr3+:1 G 4 level. Ge-As-Ga-S glasses that have been doped with Pr3+ and Er3+ cations are promising amplifier materials for both 1.31 and 1.55 μm communication windows.  相似文献   

10.
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   

11.
Eu2+-complex-doped SiO2 gels were prepared and their fluorescence properties were studied. SiO2 gels were obtained by the reactions of silicon tetrachloride, tert -butyl alcohol, and methyl alcohol under nitrogen. Both to protect Eu2+ against oxidation and to enhance the emission intensity of Eu2+, Eu2+ was complexed with 15-crown-5 or its derivative. Samples showed blue emission. Fluorescence lifetimes of samples varied from 690 to 955 ns depending on the Eu2+ concentration at 290 K. After drying of samples, 50-70% of Eu2+ remained in the divalent state without oxidation in the samples. It was found that Eu2+ complexes inside gels were stable against oxidation in air.  相似文献   

12.
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   

13.
A feasible doping strategy is introduced to synthesize Eu2+-doped α-Si3N4 nanowires coated with a thin BN film. The nanowires were characterized by X-ray diffraction, scanning electron microscopy, high-resolution transmission electron microscopy, and a fluorescence spectrophotometer. The Eu2+-doped α-Si3N4 nanowires emitted strong yellow light, which is related to the 4 f 65 d –4 f 7 transition of Eu2+, upon a broad excitation wavelength range between 250 and 450 nm. The obtained nanowires provided a potential candidate for application in optical nanodevices, as well as in white LEDs.  相似文献   

14.
Emission properties of PbO–Bi2O3–Ga2O3 glasses doped with Ho3+ were investigated for fiber-optic amplification at the 1.18 μm wavelength region. When the glasses were doped with Ho3+ ions only, there was a weak emission at 1.18 μm with a lifetime of ∼200 μs. However, when Yb3+ ions were codoped, the lifetime of the 1.18 μm emission increased to 630 μs together with a significant increase in intensity. A similar enhancement in the intensity and lifetimes was realized for the 2.05 μm emission. These effects are due to energy transfer from the Yb3+:2F5/2 to the Ho3+:5I6 level. Devitrification of the ternary PbO–Bi2O3–Ga2O3 glasses was efficiently suppressed by adding 10 mol% GeO2. Optimum Ho3+ concentration was ∼0.4 mol%, whereas Yb3+ ions can be added up to the solubility limit.  相似文献   

15.
Fluoroaluminate glasses containing various concentrations of Eu2+ were prepared under a reducing atmosphere for the present study, and the wavelength dependence of the Faraday rotation angle was examined. The magnitude of the Verdet constant (Vc) increased as the concentration of Eu2+ increased. In addition, the Verdet constant of glasses containing 5 cat.% Eu2+ was larger than that of fluoroaluminate glasses containing the same concentration of Tb3+ in the wavelength region from 400 to 600 nm. The effective transition wavelength, λt, for glasses containing Eu2+ as well as those containing Tb3+ was evaluated based on the Van Vleck and Hebb theory. Factors dominating the Verdet constant of those glasses are discussed in this report.  相似文献   

16.
Emission properties and energy transfer of PbO–Bi2O3–Ga2O3–GeO2 glasses codoped with Tm3+ and Tb3+ ions were investigated. The 1.48-μm emission due to the Tm3+:3H43F4 transition can be used to amplify the S-band (1460–1530-nm) signal light. With Tb3+ addition, the lifetime and emission intensity of the Tm3+:3F4 level decreased sharply via the Tm3+:3F4→Tb3+:7F0,1,2 energy transfer. Population densities of the 3F4 and 3H4 levels in Tm3+ calculated from rate equations clearly verified that population inversion in Tm3+ ions became possible with as little as 0.1 mol% of Tb3+ addition.  相似文献   

17.
Glasses with compositions Li1.2M0.2Ge1.8(PO4)3 (M = Al, Ga, Y, Gd, Dy, and La) were prepared and converted to glass-ceramics by heat treatment. The effects of the M3+ ions on the conductivity of the glasses and glass-ceramics were studied. The main phase present in the glass-ceramics was the conductive phase LiGe2(PO4)3. Al3+ and Ga3+ ions entered the LiGe2(PO4)3 structure by replacing Ge4+ ions, but lanthanide ions did not. The glass-ceramics exhibited much higher conductivity than the glasses. With increased ionic radius of the M3+ ions, the conductivity remained almost unchanged at ∼3 × 10−12 S/cm for the glasses, but it decreased from 1.5 × 10−5 to 8 × 10−9 S/cm for the glass-ceramics at room temperature. The higher conductivity for Al3+- and Ga3+-containing glass-ceramics was suggested to result from the substitutions of Al3+ and Ga3+ ions for Ge4+ ions in the LiGe2(PO4)3 structure.  相似文献   

18.
Compositional dependence of spontaneous emission probabilities between initial 4 F 3/2 and terminal 4 I J J = 9/2, 11/2, 13/2, 15/2) levels of Nd3+ were studied for about 90 samples of silicate, borate, and phosphate glasses using the Judd–Ofelt theory. The effect of the covalency of the Nd–O bond on the magnitude of intensity parameters was estimated from the variation of spectral profiles of the 4 I 9/24 G 5/2, 2 G 7/2 and 4 F 7/2, 4 S 3/2 transitions. Intensity parameters Ω4 and Ω6 and the spontaneous emission probabilities were strongly affected by the ionic packing ratio of the glass host. The results were discussed in terms of the site selectivity of Nd3+ ions in glasses.  相似文献   

19.
A series of novel red phosphors LiEu1− x Bi x (WO4)0.5(MoO4)1.5 ( x =0, 0.05, 0.10, 0.15, 0.20, 0.30, 0.40, and 0.50) were synthesized by the conventional solid-state reaction method. The spectrum and the crystal structure of the phosphors were characterized by Fluorescence spectrophotometry and X-ray diffraction, respectively. The photoluminescent results show that all samples can be excited efficiently by UV (396 nm) and blue (467 nm) light and that they emit red light at 615 nm with line spectra, which are coupled well with the characteristic emissions from UVLED and blue light-emitting diode (LED), respectively. There is an efficient energy transfer from Bi3+ to Eu3+ ions, leading to the emission intensity of Eu3+ being enhanced by 1.5 times, and even more when Bi3+ ions are introduced into LiEu (WO4)0.5(MoO4)1.5. The introduction of Bi3+ ions broadened the excitation band of the phosphor, and the optimum doping concentration is found to be 10 mol% of Bi3+.  相似文献   

20.
Using a novel combustion method, Eu-doped Eu:yttrium aluminum garnet (YAG) and Eu:YSAG powders, and transparent Eu:YSAG ceramics were fabricated. The optical properties of these transparent ceramics have been measured, and a reduced peak splitting of Eu3+ for 5D07F1 and 5D07F2 was observed when 10 at.% Al3+ was substituted by Sc3+. The enhanced symmetry of the Eu sites in YAG lattice, which resulted from the expanded YSAG lattice by Sc3+ doping, is the main reason for the reduced peak splitting.  相似文献   

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