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1.
The red phosphors, Na5La1−xSmx(MoO4)4 and Na5Eu1−xSmx(MoO4)4, were prepared by solid-state reaction technique at high temperature. Their structure and photo-luminescent properties were investigated. The excitation bands around 400 nm of these phosphors are broadened by Sm3+-Eu3+ co-doping. And the possible energy transfer process from Sm3+ to Eu3+ in these compounds is also discussed briefly. The phosphor Na5Eu0.90Sm0.10(MoO4)4 exhibits efficient red-emitting with broadened absorption around 400 nm and appropriate CIE chromaticity coordinates (x = 0.66, y = 0.34), bright red light can be observed from the red LED based Na5Eu0.90Sm0.10(MoO4)4.  相似文献   

2.
The (Y0.94−xyAlxGdyEu0.06)BO3 (0 ≤ x ≤ 0.04 and 0 ≤ y ≤0.4) phosphors were single-phase with a hexagonal vaterite crystal structure. The (Y0.94−x−yAlxGdyEu0.06)BO3 phosphor powders showed smooth, regular, and spherical morphology. The emission intensity of the Al- and Gd-co-doped (Y0.74−xAlxGd0.2Eu0.06)BO3 and (Y0.925−yAl0.015GdyEu0.06)BO3 phosphors was much higher than that of Al-free (Y0.74Gd0.2Eu0.06)BO3 and Gd-free (Y0.925Al0.015Eu0.06)BO3 phosphors, respectively. This means that the simultaneous addition of Gd and Al to yttrium borates was desirable for improving their photoluminescent properties.  相似文献   

3.
Eu3+- and Tb3+-activated SrGdGa3O7 phosphors were synthesized by the solid-state reaction and their luminescence properties were investigated. Sr(Gd1 − xEux)Ga3O7 and Sr(Gd1 − xTbx)Ga3O7 formed continuous solid solution in the range of x = 0-1.0. Unactivated SrGdGa3O7 exhibited a typical characteristic excitation and emission of Gd ion. The SrGdGa3O7:xEu3+ and SrGdGa3O7:xTb3+ phosphors also showed the well-known Eu3+ and Tb3+ excitation and emission. The energy transfer from Gd3+ to Eu3+ and Tb3+ were verified by photoluminescence spectra. The dependence of photoluminescence intensity on Eu3+ and Tb3+ concentration were also studied in detail and the photoluminescence (PL) intensity of SrGdGa3O7:Eu and SrGdGa3O7:Tb were compared with commercial phosphors, Y2O3:Eu and LaPO4:Ce,Tb. The luminescence decay measurements showed that the lifetimes of Eu3+ and Tb3+ were in the range of microsecond. The energy transfer from Gd3+ to Tb3+ was also observed in decay curve.  相似文献   

4.
A borate compound was adopted as a new host material of Eu3+ and Tb3+ activators to fabricate efficient luminescence materials. The phosphor compositions, Gd1−xEuxCa3(GaO)3(BO3)4 and Gd1−xTbxCa3(GaO)3(BO3)4, were synthesized by conventional solid-state reactions. The crystalline phases of the resulting powders were identified using an X-ray diffraction system. Their photoluminescence properties were investigated under long-wavelength UV excitation. The Eu3+-doped and Tb3+-doped GdCa3(GaO)3(BO3)4 phosphors efficiently emitted red and green light, respectively. The temperature dependency of emission intensity was measured in a range from room temperature to 150 °C. The emission intensities of the red and green phosphors at 150 °C are 87% and 91% of those at room temperature, respectively. In addition, the decay times of both the red and green phosphors are shorter than 3 ms.  相似文献   

5.
The highly efficient red phosphors (Ca1−xSrx)(S1−ySey):Eu2+,M3+ (M = Sc and Y) were prepared, starting from CaCO3, SrCO3, Eu2O3, Sc2O3, Y2O3, S, and SeO2 with a flux, by a conventional solid-state reaction. The optimized red phosphors converted 11.8% (Sc3+) and 11.7% (Y3+) of the absorbed blue light into luminescence. These quantum values are much higher than Q = 3.0% of CaS:Eu2+. For the fabrication of light-emitting diodes (LEDs), the prepared phosphors were coated with MgO from non-aqueous solution to overcome their weakness against moisture. White LEDs were fabricated by pasting the prepared red phosphors and the yellow YAG:Ce3+ phosphor on an InGaN blue chip (λems = 446.5 nm). The incorporation of the red phosphor to the YAG:Ce3+ phosphor resulted in an improved color rendering index (Ra) from 70 to 80.  相似文献   

6.
(Gd1−x,Eux)2O2SO4 nano-phosphors were synthesized by a novel co-precipitation method from commercially available Gd2O3, Eu2O3, H2SO4 and NaOH starting materials. Composition of the precursor is greatly influenced by the molar ratio of NaOH to (Gd1−x,Eux)2(SO4)3 (the m value), and the optimal m value was found to be 4. Fourier transform infrared spectrum (FT-IR) and thermal analysis show that the precursor (m = 4) can be transformed into pure (Gd1−x,Eux)2O2SO4 nano-phosphor by calcining at 900 °C for 2 h in air. Transmission electron microscope (TEM) observation shows that the Gd2O2SO4 phosphor particles (m = 4) are quasi-spherical in shape and well dispersed, with a mean particle size of about 30-50 nm. Photoluminescence (PL) spectroscopy reveals that the strongest emission peak is located at 617 nm under 271 nm light excitation, which corresponds to the 5D0 → 7F2 transition of Eu3+ ions. The quenching concentration of Eu3+ ions is 10 mol% and the concentration quenching mechanism is exchange interaction among the Eu3+ ions. Decay study reveals that the 5D0 → 7F2 transition of Eu3+ ions has a single exponential decay behavior.  相似文献   

7.
Phosphors of La2TeO6 doped with Eu3+ ions have been synthesized by the oxidation of the corresponding rare-earths oxytellurides of formula La2−xEuxO2Te (x = 0.02, 0.06, and 0.1) at 1050 K. Powder X-ray diffraction confirms that the as prepared materials consist of the orthorhombic La2TeO6 as main phase. The photoluminescence (PL) of red-emitting La2−xEuxTeO6 powder phosphors is reported. The emission spectrum, exhibits an intense emission peak due to 5D0 → 7F2 transition at 616 nm, which indicates that the Eu3+ ion occupies a non-centrosymmetric site in the host lattice. These materials could find application for use as lamp phosphors in the red region.  相似文献   

8.
Motivated by the need for new red phosphors for solid-state lighting applications Eu3+-doped MgMoO4 was prepared by solid-state reaction and its excitation and emission spectra were measured at room temperature. In addition, the effects of firing temperature and Eu3+ doping concentration on the PL intensities were also investigated. Compared with Y2O2S:0.05Eu3+, the obtained Mg0.80MoO4:Eu3+0.20 phosphor shows a stronger excitation band near 400 nm and intensely red-emission lines at 616 nm correspond to the forced electric dipole 5D0 → 7F2 transitions on Eu3+ under 394 nm light excitation. The CIE chromaticity coordinates (x = 0.651, y = 0.348) of Mg0.80MoO4:Eu3+0.20 close to the NTSC (National Television Standard Committee) standard values, and therefore may find application on near UV InGaN chip-based white light emitting diodes.  相似文献   

9.
Novel red phosphors Na2CaSiO4:xEu3+ were synthesized using high temperature solid-state reaction and their luminescence characteristics were investigated for the first time. The excitation spectra indicate that the Na2CaSiO4:xEu3+ phosphors can be effectively excited by ultraviolet (393 nm) light. The emission spectra of Na2CaSiO4:xEu3+ phosphors invariably exhibit four peaks assigned to the 5D0-7FJ (J = 1, 2, 3 and 4) transitions of Eu3+ under 393 nm excitation. The Commission Internationale de l’Eclairage (CIE) chromaticity coordinates and quantum efficiency (QE) are (0.66, 0.34) and 58.9%, respectively. The good color saturation and high quantum efficiency indicate that Na2CaSiO4:Eu3+ phosphors are potential candidate for light-emitting diodes.  相似文献   

10.
The luminescent properties of Ca2Gd8(1−x)(SiO4)6O2:xDy3+ (1% ≤ x ≤ 5%) powder crystals with oxyapatite structure were investigated under vacuum ultraviolet excitation. In the excitation spectrum, the peaks at 166 nm and 191 nm of the vacuum ultraviolet region can be assigned to the O2− → Gd3+, and O2− → Dy3+ charge transfer band respectively, which is consistent with the theoretical calculated value using Jφrgensen's empirical formula. While the peaks at 183 nm and 289 nm are attributed to the f-d spin-allowed transitions and the f-d spin-forbidden transitions of Dy3+ in the host lattice with Dorenbos's expression. According to the emission spectra, all the samples exhibited excellent white emission under 172 nm excitation and the best calculated chromaticity coordinate was 0.335, 0.338, which indicates that the Ca2Gd8(SiO4)6O2:Dy3+ phosphor could be considered as a potential candidate for Hg-free lamps application.  相似文献   

11.
The phosphors in the system Sr2−xyP2O7:xEu2+,yMn2+ were synthesized by solid-state reactions and their photoluminescence properties were investigated. These phosphors have strong absorption in the near UV region, which is suitable for excitation of ultraviolet light emitting diodes (UVLEDs). The orange-reddish emission of Mn2+ in these phosphors can be used as a red component in the tri-color system and may be enhanced by adjusting the Mn2+/Eu2+ ratio. The energy transfer from Eu2+ to Mn2+ is observed with a transfer efficiency of ∼0.45 and a critical distance of ∼10 Å. The results reveal that Sr2−xyP2O7:xEu2+,yMn2+ phosphors could be used in white light UVLEDs.  相似文献   

12.
The luminescent properties of Na3Y1−xSi3O9:xEu3+ (0.05 ≦ x ≦ 0.80) powder crystals were investigated in UV-VUV region. The Eu3+-O2− charge transfer band (CTB) was observed to be located at around 233 nm and the environmental parameter (he) was estimated to be about 0.730. The excitation spectrum monitoring the 613 nm red emission from Eu3+ ions reveals the host absorption band (HAB) to be around 145 nm. The calculated Commission Internationale de l’Eclairage (CIE) chromaticity coordinates indicate the emission by 233 nm rather than by 147 nm excitation has the better color purity and the possible mechanisms have been proposed. The Eu3+-emission showed high quenching concentration due to the isolated YO6 octahedra in the host and the small he for the Eu3+ ions and the optimum concentration was determined to be as high as x = 0.65 and 0.30 with 233 and 147 nm excitation, respectively.  相似文献   

13.
Long afterglow phosphors (Ca1−xEux)2MgSi2O7 (0.002 ≤ x ≤ 0.02) were prepared by solid-state reactions under a weak reductive atmosphere. X-ray diffraction pattern, photoluminescence spectra, decay curve, afterglow spectra and thermoluminescence curves were investigated. The phosphors showed two emission peaks when they were excited by 343 nm, due to two types of Eu2+ centers existing in the Ca2MgSi2O7 lattice. However, only one emission peak can be found in their afterglow spectra. Energy transfer between Eu2+ ions in inequivalent sites was found. A possible mechanism was presented and discussed. The afterglow decay time of Ca1.998MgSi2O7:Eu0.002 was nearly 12.5 h which means it was a good long lasting phosphor.  相似文献   

14.
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   

15.
The novel vacuum ultraviolet (VUV) excited Na3Y9O3(BO3)8:Eu3+ red phosphor was synthesized and the photoluminescence (PL) properties were investigated. The phosphor showed strong VUV PL intensity, large quenching concentration (40 mol%) and good chromaticity (0.649, 0.351). The Eu3+-O2− charge transition (CT) was observed to be at a higher energy (232 nm, 5.35 eV). The host absorption at 127-166 nm was broad and strong when monitoring the Eu3+ emission, which indicated that energy transfer from the host-lattice to the Eu3+ ions was efficient in Na3Y9O3(BO3)8:Eu3+. These excellent VUV PL properties were revealed to be correlated with the unique isolated layer-type structure of Na3Y9O3(BO3)8 host. The results showed that the Na3Y9O3(BO3)8:Eu3+ would be a good candidate for VUV-excited red phosphor.  相似文献   

16.
Y2O2S co-doped with Bi3+,Eu3+ phosphors were prepared and their luminescence properties under vacuum ultraviolet (VUV) excitation were investigated. Much stronger red emission for Y2O2S:Eu3+,Bi3+ were observed under 147 nm excitation than that for Y2O2S:Eu3+. Investigation on photoluminescence and calculation of electronic structure of Y2O2S:Eu3+,Bi3+ revealed that the Bi3+ acts as a medium in energy transfer process and the great VUV luminescence enhancement of Y2O2S:Eu3+ by doping Bi3+ is due to effective energy transfer process: charge transfer (CT) transition of Y3+-O2− → Bi3+ → Eu3+. The Y2O2S:Eu3+,Bi3+ showed excellent optical properties when compared with the commercial (Y,Gd)BO3:Eu3+. Thus, the Y2O2S:Eu3+,Bi3+ would be a promising VUV-excited red phosphor.  相似文献   

17.
Scheelite-type Ca1−xSmxMoO4+δ electrolyte powders were prepared by the sol-gel auto-combustion process. The crystal structure of the samples was determined by employing the techniques of X-ray diffraction (XRD). According to the XRD analysis, the formed continuous series of Ca1−xSmxMoO4+δ (0 ≤ x ≤ 0.3) solid solutions had the structure of tetragonal scheelite, and the lattice parameters increased with increasing x in the Sm-substituted system. Results of sinterability and electrochemical testing revealed that the performances of Sm-doped calcium molybdate were superior to that of pure CaMoO4. Ca1−xSmxMoO4+δ ceramics show higher sinterability, and the Ca0.8Sm0.2MoO4+δ sample with 98.7% of the theoretical density were obtained after being sintered at 1250 °C for 4 h. The conductivity increased with increasing samarium content, and a total conductivity 9.54 × 10−3 S cm−1 at 800 °C could be obtained in Ca0.8Sm0.2MoO4+δ sintered at 1250 °C for 4 h.  相似文献   

18.
A series of new red phosphors, NaEu(MoO4)2−2x(SO4)2x, were prepared by the conventional solid state reaction. Their excitation spectra, emission spectra and decay curves were measured at room temperature. When the SO42− content is in excess of 20%, other phases appear. With the introduction of SO42−, the Mo-O charge transfer band of NaEu(MoO4)2−2x(SO4)2x shows red shift, and the excitation intensities of the 4f - 4f transitions of Eu3+ are strengthened, compared with that of NaEu(MoO4)2. The single red light-emitting diodes-based these phosphors were fabricated. The light-emitting diode fabricated with the phosphor NaEu(MoO4)1.80(SO4)0.20 exhibited higher red emission relative to that with NaEu(MoO4)2. Bright red light can be observed by naked eyes from the light-emitting diode-based NaEu(MoO4)1.80(SO4)0.20.  相似文献   

19.
Co-doped ceria of Ce1−xGdxyYyO2−0.5x, wherein x = 0.15 and 0.2, 0 ≤ y ≤ x, were prepared by glycine-nitrate method. Their structures and ionic conductivities were characterized by X-ray diffraction (XRD) and AC impedance spectroscopy (IS). All the electrolytes were found to be ceria-based solid solutions of fluorite type structures. Co-doping was found to effectively enhance the conductivity. In comparison to the singly doped ceria, the co-doped ceria showed much higher ionic conductivities at 673-973 K. At 773 K, the ionic conductivity of Ce0.8Gd0.05Y0.15O1.9 is 0.013 S cm−1 which is three times as high as that of Ce0.8Gd0.2O1.9. These Gd3+and Y3+ co-doped ceria are ideal electrolyte materials of intermediate temperature solid oxide fuel cells (SOFCs).  相似文献   

20.
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