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1.
Ba1−ySryLa4−xTbx(WO4)7 (x = 0.02-1.2, y = 0-0.4) phosphors were prepared via a solid-state reaction and their photoluminescence properties were investigated. An analysis of the decay behavior indicates that the energy migration between Tb3+ ions is conspicuous in the 5D3 → 7F4 transition due to the cross-relaxation in BaLa4(WO4)7. A partial substitution of Ba2+ by Sr2+ can not only enhance the emission intensity but also increase the solid solubility of Tb3+ in Ba1−ySryLa4−xTbx(WO4)7. The emission intensity of the 5D4 → 7FJ (J = 4, 5, 6) transitions can be enhanced by increasing Sr2+ and Tb3+ concentrations, with the optimal conditions being x = 1.2, y = 0.4 (Ba0.6Sr0.4La2.8Tb1.2(WO4)7). Under near-UV excitation at 379 nm, the CIE color coordinates of Ba1−ySryLa4−xTbx(WO4)7 vary from blue (0.212, 0.181) at x = 0.04, y = 0, to green (0.245, 0.607) at x = 1.2, y = 0.4.  相似文献   

2.
Oxyfluoride glasses were developed with composition 30SiO2·15AlO1.5·28PbF2·22CdF2·(4.9−x)GdF3·0.1HoF3·xYbF3 (x=0, 0.1, 0.2, 0.5, 1, 2, 3, and 4) in mol%. Powder X-ray diffraction analysis revealed that the heat-treatments of the oxyfluoride glasses at the first crystallization temperature cause the precipitation of Yb3+–Ho3+ co-doped fluorite-type nano-crystals of about 17.8 nm in diameter in the glass matrix. These transparent glass-ceramics exhibited very strong green up-conversion luminescence due to the Ho3+: (5F4, 5S2)→5I8 transition under 980 nm excitation. The intensity of the green up-conversion luminescence in the glass-ceramics was much stronger than that in the precursor oxyfluoride glass. The reasons for the highly efficient Ho3+ up-conversion luminescence in the oxyfluoride glass-ceramics are discussed.  相似文献   

3.
SrLa1−xRExGa3O7 (RE = Eu3+, Tb3+) phosphor films were deposited on quartz glass substrates by a simple Pechini sol-gel method. X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), atomic force microscopy, field-emission scanning electron microscopy, photoluminescence spectra, and lifetimes were used to characterize the resulting films. The results of XRD indicated that the films began to crystallize at 700 °C and crystallized fully at 900 °C. The results of FT-IR spectra were in agreement with those of XRD. Uniform and crack-free films annealed at 900 °C were obtained with average grain size of 80 nm, root mean square roughness of 46 nm and thickness of 130 nm. The RE ions showed their characteristic emission in crystalline SrLa1−xRExGa3O7 films, i.e., Eu3+5D0-7FJ (J = 0, 1, 2, 3, 4), Tb3+5D4-7FJ (J = 6, 5, 4, 3) emissions, respectively. The optimum concentrations (x) of Eu3+ and Tb3+ were determined to be 50, and 80 mol% in SrLa1−xRExGa3O7 films, respectively.  相似文献   

4.
Eu/Tb codoped transparent oxyfluoride borosilicate glass ceramics containing Sr2GdF7 nanocrystals were fabricated under a reductive atmosphere and the conversion of Eu3+ ions to Eu2+ ions was observed. The Sr2GdF7 nanocrystals with an average size of 32 nm were homogeneously precipitated in the oxyfluoride borosilicate glass matrix, which could be evidenced by X-ray diffraction (XRD), transmission electron microscopy (TEM) and energy-dispersive X-ray (EDX) spectroscopy. The enhancement of photoluminescence emission intensity, reduction of the relative emission intensities between 5D0 → 7F2 and 5D0 → 7F1, and long fluorescence lifetimes of Eu2+, Eu3+, and Tb3+ ions revealed that more rare earth ions were partitioned into the low phonon energy environment Sr2GdF7 nanocrystals. Under ultraviolet excitation, pure and bright white light emission was obtained in the oxyfluoride borosilicate glass ceramic, which may be a potential blue, green and red-emitting phosphor for white LEDs.  相似文献   

5.
BaSi2O2N2: Eu2+ is an efficient phosphor because of its high quantum yield and quenching temperature. Partial substitution of Ba2+ by Sr2+ is the most promising approach to tune the color of phosphors. In this study, a series of (Ba1−xySrxEuy)Si2O2N2 (x = 0.0–0.97, y = 0.00–0.10) phosphors are synthesized via high-temperature solid-state reactions. Intense green to yellow phosphors can be obtained by the partial substitution of the host lattice cation Ba2+ by either Sr2+ or Eu2+. The luminescent properties and the relationships among the lowest 5d absorption bands, Stokes shifts, centroid shifts, and the splitting of Eu2+ are studied systematically. Then, based on (Ba1−xySrxEuy)Si2O2N2 phosphors and near-ultraviolet (∼395 nm)/blue (460 nm) InGaN chips, intense green–yellow light emitting diodes (LEDs) and white LEDs are fabricated. (Ba0.37Sr0.60)Si2O2N2: 0.03Eu2+ phosphors present the highest efficiency, and the luminous efficiency of white LEDs can reach 17 lm/w. These results indicate that (Ba1−xySrxEuy)Si2O2N2 phosphors are promising candidates for solid-state lighting.  相似文献   

6.
A series of mixed fluorides with general composition Ba1−xNdxF2+x (0.00≤x≤1.00) was prepared by vacuum heat treatment of the mixture of starting fluorides, and analyzed by powder XRD. From the XRD analysis, the low temperature phase equilibria in BaF2-NdF3 system is elucidated. The initial compositions in this series, that is, up to the nominal composition Ba0.65Nd0.35F2.35 (x≤0.35) exist as cubic fluorite-type solid solution. Beyond the solid solution limit, that is, x>0.35, a rhombohedral fluorite related ordered phase is observed. Further, NdF3-rich compositions (x≥0.50) exist as a mixture of rhombohedral ordered phase and NdF3 (tysonite)-type phase. About 10 mol% of BaF2 could be retained in the NdF3 lattice, forming a tysonite-type solid solution, under the short annealed and slow cooled conditions.  相似文献   

7.
La2−xBaxMo2O9−x/2 (x ≤ 0.18) have been prepared by solid state reaction method. The lattice parameter of La2−xBaxMo2O9−x/2 (x ≤ 0.18) determined by XRD data refinement shows a linear dependence on the dopant Ba content x. For the specimen with a La/Ba molar ratio of 0.18-0.2, additional reflection of secondary phase exists in the XRD pattern, so the value of solubility limit for Ba in La2Mo2O9 is defined in range of 0.18 < x < 0.2. As the replacement degree of La3+ by Ba2+ increases, the bulk conductivity of La2−xBaxMo2O9−x/2 (x ≤ 0.18) decreases initially and then increases, a minimum value at La1.9Ba0.1Mo2O8.95 exists. Hebb-Wagner studies in argon atmosphere, which use an oxide-ion blocking electrode, show that La2−xBaxMo2O9−x/2 (x ≤ 0.18) are predominantly oxide-ion conducting in the temperature ranging from 773 to 1173 K. The average thermal expansion coefficient of La1.84Ba0.16Mo2O8.92 determined by high-temperature XRD was deduced as great as 17.5 × 10−6 K−1 between 298 and 1173 K.  相似文献   

8.
High-quality Y1−xyAlxTbyBO3 (0 ≤ x ≤ 0.1, 0.04 ≤ y ≤ 0.16) phosphor powders with fine size, spherical and regular morphology, and non-agglomeration were successfully prepared by ultrasonic spray pyrolysis. The blue emission from the 5D37FJ (J = 4, 5, and 6) transition for the Y0.94−xAlxTb0.06BO3 phosphor was quenched. The optimal concentration of Tb3+ was reduced by doping Al3+ into the Y1−yTbyBO3 phosphor, i.e., y = 0.1 and 0.12 for Y0.975−yAl0.025TbyBO3 and Y1−yTbyBO3, respectively. The Al3+ doping was highly effective for improving the photoluminescence characteristics. The photoluminescence emission intensity of the Al3+-doped Y0.915Al0.025Tb0.06BO3 phosphor at 543 nm was about three times stronger than that of the Al3+-free Y0.94Tb0.06BO3 phosphor.  相似文献   

9.
High-quality Gd0.94(P1−xVx)O4:Eu0.06 (0 ≤ x ≤ 1.0) powders having small size, spherical morphology, smooth surface, and nonaggregation are synthesized by the ultrasonic spray pyrolysis. The complex host composition, Gd0.94(P1−xVx)O4:Eu0.06 (x ≥ 0.5), shows a single phase with the tetragonal xenotime structure. The introduction of V5+ ions in the P5+ lattice yields the deviation from the centrosymmetry of Eu3+ ions. By increasing the V5+ content, the emission intensity corresponding to the 5D0 → 7F1 transition decreases. On the other hand, the emission intensity corresponding to the 5D0 → 7F2 transition increases up to x = 0.5, and then decreases upon further increasing the V5+ content. The emission intensity, peaking at 620 nm, of complex composition Gd0.94(P0.5V0.5)O4:Eu0.06 is approximately five and two times stronger than that of the Gd0.94PO4:Eu0.06 and Gd0.94VO4:Eu0.06, respectively. It is believed that the introduction of the complex composition Gd0.94(P1−xVx)O4:Eu0.06 is highly effective for improving the emission properties.  相似文献   

10.
The effect of CaO-SiO2-B2O3 (CSB) glass addition on the sintering temperature and dielectric properties of BaxSmyTi7O20 ceramics has been investigated using X-ray diffraction, scanning electron microscopy and differential thermal analysis. The CSB glass starts to melt at about 970 °C, and a small amount of CSB glass addition to BaxSmyTi7O20 ceramics can greatly decrease the sintering temperature from about 1350 to about 1260 °C, which is attributed to the formation of liquid phase. It is found that the dielectric properties of BaxSmyTi7O20 ceramics are dependent on the amount of CSB glass and the microstructures of sintered samples. The product with 5 wt% CSB glass sintered at 1260 °C is optimal in these samples based on the microstructure and the properties of sintering product, when the major phases of this material are BaSm2Ti4O12 and BaTi4O9. The material possesses excellent dielectric properties: ?r = 61, tan δ = 1.5 × 10−4 at 10 GHz, temperature coefficient of dielectric constant is −75 × 10−6 °C−1.  相似文献   

11.
A comparative study of the microstructure and dielectric properties between Ba1−xCaxTiO3 (BCT) ceramics and films were performed in the whole Ca concentration range of x = 0-1. The ceramics were prepared by conventional solid-state reaction technique and the films by the method of pulsed-laser deposition. X-ray diffraction (XRD) study of the BCT ceramics exhibited a pure tetragonal phase for x = 0-0.25, a tetragonal-orthorhombic diphase for x = 0.25-0.85 and a pure orthorhombic phase for x = 0.90-1.00. And the dielectric phase transition temperature from tetragonal to cubic was marginally affected by the Ca doping into BaTiO3. However, BCT films deposited on Pt/Si/SiO2/Si substrates showed a different microstructure and dielectric properties. Tetragonal-orthorhombic diphase was not found in the BCT films for x = 0.25-0.85, and a large decrease of the Curie point and diffuse phase transition were observed in the BCT films. Based on the compositional analysis, such phenomena were ascribed to the occupancy of some Ca2+ to the Ti4+ sites in the BCT films.  相似文献   

12.
This study investigated the photoluminescent properties of Er3+/Yb3+ and Ce3+/Er3+/Yb3+ -doped oxyfluoride glass–ceramics. The transparent oxyfluoride glass–ceramics were prepared by high temperature melting method and subsequent heat treatment. Effect of heat treatment schedules on crystallization behavior and microstructure were analyzed by differential scanning caborimetry, X-ray diffraction, infrared spectrum and scanning electron microscopy. The structure of fluoride nanocrystals indicates that the main phase in the oxyfluoride glass ceramics is CaF2 nanocrystal sized at 25 nm at the optimal crystallization temperature 600 °C for 8 h. The Ce3+/Er3+/Yb3+ tri-doped oxyfluoride glass–ceramics shows wider absorption bands comparing with Er3+/Yb3+ co-doped oxyfluoride glass–ceramics. The effective energy transfer processes from Ce3+ to Yb3+, Er3+ to Yb3+ and Ce3+ to Er3+ all can take place simultaneously. The idea of using Ce3+ together with Er3+ and Yb3+ ions could enhance the ultraviolet visible light absorption and the 960–1040 nm near infrared emission. Results of this study demonstrate that the tri-activator Ce3+/Er3+/Yb3+ materials are promising for practical application to enhance the energy efficiency of crystalline Si solar cells via spectrum modification.  相似文献   

13.
Undoped and doped either by Eu3+ or Tb3+ bismuth borate Ba3BiB9O18 was structurally characterized and analyzed by fluorescence spectroscopy. Belonging to synthetic borate member of the family Ba3XB9O18, layers of planar triangular B3O6 groups connecting with deformed BaO6 hexagons are interleaved by 9-coordinate Ba atoms, and 6-coordinate Bi atoms. Its crystal structure was determined and refined from powder X-ray diffraction data by the Rietveld method and the results showed that Ba3BiB9O18 belongs to space group P63/m with unit cell dimensions of a = 7.1999(2) Å, c = 17.3567(6) Å, and z = 2. Curves of differential thermal analysis and thermogravimetric analysis showed that Ba3BiB9O18 is a congruent melting compound and chemically stable above 728 °C. Ba3Bi1−xEuxB9O18 and Ba3Bi1−xTbxB9O18 form a continuous solid solution from x = 0.01 to x = 0.9. The ultraviolet excited photoluminescence intensity increased with both Eu3+ and Tb3+ concentration in the matrix of Ba3BiB9O18. There may be an interesting correlation between spectroscopic properties and lattice structural features of doped Ba3BiB9O18.  相似文献   

14.
Transparent glass ceramics have been obtained by nucleation and growth of Y2Te6O15 or Er2Te5O13 cubic phase in a new Er3+-doped oxyfluoride tellurite glass. Effect of heat treatment on absorption spectra, luminescence and up-conversion properties in the oxyfluoride tellurite glass has been investigated. With heat treatment the ultraviolet absorption edge red shifted evidently for the oxyfluoride telluride glass. The near infrared emission that corresponds to Er3+:4I13/2 → 4I15/2 can be significantly enhanced after heat treatment. Under 980 nm LD pumping, red and green up-conversion intensity of Er3+ in the glass ceramic can be observed much stronger than that in the base glass.  相似文献   

15.
Y0.5−xDyxLi1.5VO4 phosphor particles have been synthesized by a new wet-chemical method of in situ co-precipitation via assembling inorganic/organic hybrid precursors. X-ray diffraction and scanning electronic microscope show that these materials have the micrometer dimension. All the emission spectra exhibit the characteristic transitions of Dy3+, which is due to the 4F9/2 → 6H15/2 (blue) and 4F9/2 → 6H13/2 (yellow) and the concentration quenching phenomenon occurs in the system of Y0.5−xDyxLi1.5VO4.  相似文献   

16.
Erbium-doped BaF2 nanoparticles were prepared using the ultrasonic surge method. The particles were characterized by X-ray diffraction, transmission electron microscope, photoluminescence and absorption. The results show that when Er3+ ions were introduced into the BaF2 lattice, cubic fluorite-type Ba1−xErxF2+x solid solution, x = 0.42 was formed. Furthermore, the crystalline phase of Ba1−xErxF2+x solid solution was largely influenced by the annealing temperature.  相似文献   

17.
The aim of this article was to study the influence of GeO2 on the thermal stability and optical properties of Er3+/Yb3+ codoped (70 − x)TeO2xGeO2–PbF2–BaF2 (TGEYx) glasses prepared by using a melting method. The properties of Er3+/Yb3+ codoped glasses were investigated by using differential scanning calorimetry, upconversion luminescence, Raman and optical absorption spectra. The results indicated that TGEY35 glass with the germanate–tellurite mixed network showed the best thermal stability and poor crystallization tendency. With increasing the GeO2 content, the maximum phonon energy of oxyfluoride tellurite glass network increased, while the phonon density decreased. The upconversion emission intensities enhanced obviously based on the decreasing phonon density of glass hosts, while the increasing red emission (657 nm) with the increase of GeO2 concentration was attributed to the relative larger maximum phonon energy which matching the energy gap between the pertinent 4S3/2 and 4F9/2 levels.  相似文献   

18.
A series of mixed fluorides with general composition Ba1−xErxF2+x (0.00≤x≤1.00) were prepared by a vacuum heat treatment of the binary fluorides and analyzed by powder XRD, which revealed the phase equilibrium in BaF2-ErF3 system. The nominal compositions with x≤0.25 compositions exist as cubic fluorite type solid solution. A rhombohedral ordering is observed in the vicinity of 42 mol% of ErF3 in BaF2. A monoclinic phase with the composition Er2BaF8 dominates the ErF3-rich compositions. The compositions for x>0.67 exist as a mixture of Er2BaF8 and leftover ErF3, whereas the compositions for x<0.67 exist as a mixture of Er2BaF8 and rhombohedral fluorite derived phase. The evolution of the various phases will be discussed in reference to the powder XRD data.  相似文献   

19.
The Ho3+/Yb3+/Ce3+:YF3 nanocrystals embedded transparent oxyfluoride glass ceramics were successfully synthesized and the emission spectra have been measured. We changed the doped concentrations of ion Ce3+ in the glass ceramics and unexpectedly found that the different concentrations brought forth different luminescence wavelengths, a tunable luminescence wave band from green to red, which might be useful to the tunable visible laser or display applications. In addition, excitated with wavelength 975 nm LD, the transitions of Ho3+: 5G45I8 at 390 nm, 5G55I8 at 420 nm and 5F35I8 at wavelength 490 nm were observed in the glass ceramic GCCe0, while in samples GCCeJ(J=1,3,5,8), the three peaks disappeared.  相似文献   

20.
Oxides belonging to the families Ba3ZnTa2−xNbxO9 and Ba3MgTa2−xNbxO9 were synthesized by the solid state reaction route. Sintering temperatures of 1300°C led to oxides with disordered (cubic) perovskite structure. However, on sintering at 1425°C hexagonally ordered structures were obtained for Ba3MgTa2−xNbxO9 over the entire range (0≤x≤1) of composition, while for Ba3ZnTa2−xNbxO9 the ordered structure exists in a limited range (0≤x≤0.5). The dielectric constant is close to 30 for the Ba3ZnTa2−xNbxO9 family of oxides while the Mg analogues have lower dielectric constant of ∼18 in the range 50 Hz to 500 kHz. At microwave frequencies (5-7 GHz) dielectric constant increases with increase in niobium concentration (22-26) for Ba3ZnTa2−xNbxO9; for Ba3MgTa2−xNbxO9 it varies between 12 and 14. The “Zn” compounds have much higher quality factors and lower temperature coefficient of resonant frequency compared to the “Mg” analogues.  相似文献   

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