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1.
Abstract

Ce3+-activated Gd3Al5O12 garnet, effectively stabilized by Lu3+ doping, has been developed for new yellow-emitting phosphors. The powder processing of [(Gd1?xLux)1?yCey]3Al5O12 solid solutions was achieved through precursor synthesis via carbonate precipitation, followed by annealing. The resultant (Gd,Lu)AG:Ce3+ phosphor particles exhibit typical yellow emission at ~570 nm (5d–4f transition of Ce3+) upon blue-light excitation at ~457 nm (the 2F5/2–5d transition of Ce3+). The quenching concentration of Ce3+ was determined to be ~1.0 at% (y = 0.01) and the quenching mechanism was suggested to be driven by exchange interactions. The best luminescent [(Gd0.9Lu0.1)0.99Ce0.01]AG phosphor is comparative to the well-known YAG:Ce3+ in emission intensity but has a substantially red-shifted emission band that is desired for warm-white lighting. The effects of processing temperature (1000–1500 °C) on the spectroscopic properties of the phosphors, especially those of Lu3+/Ce3+, were thoroughly investigated and discussed from the centroid position and crystal field splitting of the Ce3+ 5d energy levels.  相似文献   

2.
Shaped single crystals of (Yb0.05LuxGd0.95−x)Ga5O12 (0.0x0.9) and Yb0.15Gd0.15Lu2.7(AlxGa1−x)O12 (0.0x1.0) were grown by the modified micro-pulling-down method. Continuous solid solutions with garnet structure and a linear compositional dependency of crystal lattice parameter in the system Yb:(Gd,Lu)3(Ga,Al)5O12 are formed. Measured optical absorption spectra of the samples show 4f–4f transitions related to Gd3+ ion at 275 and 310 nm, and also an onset of charge transfer transitions from oxygen ligands to Gd3+ or Yb3+ cations below 240 nm. A complete absence of Yb3+ charge transfer luminescence under X-ray excitation in any of the investigated samples was explained by the overlapping of charge transfer absorption of Yb3+ by that of Gd3+ ions. For specific composition of Lu1.5Gd1.5Ga5O12 an intense defect––host lattice-related emission, which achieve of about 40% integrated intensity compared with Bi4Ge3O12, was found.  相似文献   

3.
Synthesis of (Gd0.95−xLnxEu0.05)2O3 (Ln = Y and Lu, x = 0–0.95) powders via ammonium hydrogen carbonate (AHC) precipitation has been systematically studied. The best synthesis parameters are found to be an AHC/total cation molar ratio of 4.5 and an ageing time of 3 h. The effects of Y3+ and Lu3+ substitution for Gd3+, on the nucleation kinetics of the precursors and structural features and optical properties of the oxides, have been investigated. The results show that (i) different nucleation kinetics exist in the Gd–Y–Eu and Gd–Lu–Eu ternary systems, which lead to various morphologies and particle sizes of the precipitated precursors. The (Gd,Y)2O3:Eu precursors display spherical particle morphologies and the particle sizes increase along with more Y3+ addition. The (Gd,Lu)2O3:Eu precursors, on the other hand, are hollow spheres and the particle sizes increase with increasing Lu3+ incorporation, (ii) the resultant oxide powders are ultrafine, narrow in size distribution, well dispersed and rounded in particle shape, (iii) lattice parameters of the two kinds of oxide solid solutions linearly decrease at a higher Y3+ or Lu3+ content. Their theoretical densities linearly decrease with increasing Y3+ incorporation, but increase along with more Lu3+ addition and (iv) the two kinds of phosphors exhibit typical red emissions at ∼613 nm and their charge-transfer bands blue shift at a higher Y3+ or Lu3+ content. Photoluminescence/photoluminescence excitation intensities and external quantum efficiency are found to decrease with increasing value of x, and the fluorescence lifetime mainly depends on the specific surface areas of the powders.  相似文献   

4.
YAG:Ce3+, Gd3+ nano-phosphors were synthesised by the glycothermal method. The X-ray diffraction measurements showed that the samples can be well-crystallised at 600°C. The transition electron microscope showed that the particles have sizes mostly in the range between 35 and 100?nm. The YAG:Ce nano-phosphor had a wide emission band ranging from blue to yellow with a peak at 532?nm, due to the transition from the lowest 5d band to 2F7/2, 2F5/2 states of the Ce3+ ion. Red-shift of emission peak wavelength from 532 to 568?nm was achieved doping Gd3+ ions into the YAG:Ce3+ to substitute some Y3+ ions. White light emitting diodes (LEDs) were obtained by combining blue LED chip (InGaN-based 460?nm emitting) with (Y2.94? x Ce0.06Gd x )Al5O12 phosphor. As x has the value of 0.8, an intense white LED with good colour rendering of 86 was obtained.  相似文献   

5.
A nanopowder of Lu2O3:Eu3+ (C Eu = 5 at.%) was obtained by coprecipitation with urea (NH2)2CO from aqueous solutions. Using this nanopowder, compact Lu2O3:Eu3+ films with thicknesses within 20–200 μm and a relative density up to 65% of the theoretical limit were deposited using the spin-coating and painting techniques. The films were characterized by scanning electron microscopy, X-ray diffraction, and X-ray luminescence (XRL) measurements. It is established that the XRL intensity depends on the phosphor/organic binder ratio and thickness of the film. The most intense XRL and most homogeneous structure are observed for 20-μm-thick Lu2O3:Eu3+ films.  相似文献   

6.
RExLu2-x O3:Eu3+ (RE = Y, Gd) nanophosphors with x = 0.4, 1.0, and 1.6 were synthesized using rare-earth salicylate coordination polymers as precursors for the luminescent species RExLu2-x O3:Eu3+ (RE = Y, Gd) composed of polyethylene glycol both as a dispersing medium and fuel. Their particle sizes were around 100 nm as determined by scanning electron microscopy and x-ray diffraction.__________From Neorganicheskie Materialy, Vol. 41, No. 6, 2005, pp. 706–710.Original English Text Copyright © 2005 by Zhou, Yan.This article was submitted by the authors in English.  相似文献   

7.
《Materials Research Bulletin》2013,48(11):4687-4692
Epitaxial films of Ce-doped Gd3(AlxGa1−x)5O12 with x = 0.00, 0.22, 0.31, 0.38 formula units were grown using liquid-phase epitaxy method, and their optical properties were studied. The emission of Ce3+ ions can be observed only when Al3+ ions are incorporated into the garnet structure, resulting in a shift of the 5d Ce3+ states from the conduction band to the bandgap. It is shown that the shift is caused by the cumulative effect of gradual low-energy shift of the lowest 5d level of Ce3+ and the raise of the garnet bandgap energy with increasing Al3+ concentration.  相似文献   

8.
Two series of Lu3Al5O12:Cr3+ and Lu3Al5O12:0.5% Ce3+,Cr3+ luminescent materials were prepared by a sol–gel combustion method. All samples were characterized by powder X-ray diffraction (XRD), infrared (IR) and photoluminescence (PL) measurements. Moreover, luminous efficacies (LE), CIE 1931 colour points, and quantum efficiencies (QE) were calculated and discussed. Luminescence measurements indicated that Ce3+ ions located at Lu3+ site transfers absorbed energy to Cr3+ ions located at Al3+ site. However, with increasing Cr3+ concentration the total light output of Lu3Al5O12:0.5% Ce3+,Cr3+ phosphors decrease.  相似文献   

9.
Nd 1% doped complex garnet scintillators were prepared by Furukawa and their optical and scintillation properties were investigated on a comparison with previously reported Nd-doped YAG. Chemical compositions of newly developed complex garnets were Lu2Y1Al5O12, Lu2Y1Ga3Al2O12, Lu2Gd1Al5O12, Lu2Gd1Ga3Al2O12, Gd1Y2Al5O12, Gd1Y2Ga3Al2O12, and Gd3Ga3Al2O12. They all showed 50–80% transmittance from ultraviolet to near infrared wavelengths with several absorption bands due to Gd3+ or Nd3+ 4f–4f transition. In X-ray induced radioluminescence spectra, all samples exhibited intense lines at 310 nm due to Gd3+ or 400 nm due to Nd3+ depending on their chemical composition. Among them, the highest scintillation light yield was achieved by Lu2Y1Al5O12. Typical scintillation decay times of them resulted 1.5–3 μs. Thermally stimulated glow curve after 1 Gy exposure and X-ray induced afterglow were also investigated.  相似文献   

10.
The phosphors Y0.95−x M x Eu0.05B1−y R y O3:Eu3+ (M = Ca, Sr, Ba, Zn, Al, 0 ≤ x ≤ 0.1; R = Si, P, 0 ≤ y ≤ 0.1) are successfully synthesized by solid-state reaction. All the solid samples are identified as isomorphs. Their luminescent properties are studied under UV and VUV excitation. With the incorporation of metallic or nonmetallic cations, the chromaticity of YBO3:Eu3+ is remarkably improved as well as the luminescent intensity increased. When 10% of Al3+ is doped into YBO3 host lattice, the best ratio of the red emission at 610 nm to the orange one at 591 nm is obtained and the luminescent intensity increased simultaneously. The reason is analyzed, and can be explained by the decrease of the symmetry around Eu3+ site in YBO3 host lattice.  相似文献   

11.
The paper demonstrates our last achievement in development of the novel scintillating screens based on single crystalline films (SCF) of Ce doped multicomponent garnets using the Liquid Phase Epitaxy (LPE) method. We report in this work the optimized content and excellent scintillation properties of SCF of Lu3-xGdxAl5-yGayO12, Lu3-xTbxAl5-yGayO12 and TbxGdxAl5-yGayO12 garnet compounds grown by the LPE method from PbOB2O3 based melt-solution onto Gd3Al2.5Ga2.5O12 and YAG substrates.We also show that the Tb1.5Gd1.5Al2.5Ga2.5O12:Ce SCF possess the highest light yield (LY) in comparison with all ever grown garnet SCF scintillators. Namely, the LY of these SCF exceeds by 3.8 and 1.85 times the LY values of the best samples of YAG:Ce and LuAG:Ce SCF scintillators, respectively. The SCF samples of the mentioned compounds show low thermoluminescence in the above room temperature range and relatively fast scintillation decay time t1/e in the 180–200 ns range.  相似文献   

12.
Luminescence properties of Y2−xGdxO3:Eu3+ (x = 0 to 2.0) thin films are investigated by site-selective laser excitation spectroscopy. The films were grown by pulsed laser deposition method on SiO2 (100) substrates. Cubic phase Y2O3 and Gd2O3 and monoclinic phase Gd2O3 are identified in the excitation spectrum of the 7F0 → 5D0 transition of Eu3+. The emission spectra of the 5D0 → 7FJ (J = 1 and 2) transition from individual Eu3+ centers were obtained by tuning the laser to resonance with each excitation line. The excitation line at around 580.60 nm corresponds to the line from Eu3+ with C2 site symmetry of cubic phase. New lines at 578.65 and 582.02 nm for the CS sites of Gd2O3 with monoclinic phase are observed by the incorporation of Gd in Y2O3 lattice. Energy transfer occurs between Eu3+ ions at the CS sites and from Eu3+ ions at the CS sites to those at the C2 site in Y2−xGdxO3.  相似文献   

13.
The effects of the Eu3+concentration and PO4/VO4ratio on the photoluminescence (PL) of K3R1 – y Eu y (PO4) x (VO4)2 – x (R = La, Gd) phosphate vanadates were studied over wide composition ranges. The energies of the Stark components of the 7 F j(j= 0, 1, 2) levels were determined, and the crystal-field parameters were evaluated. The concentration quenching of Eu3+luminescence was examined. The PL intensity was found to increase with Eu3+content up to y= 0.3. At higher Eu3+contents, the PL intensity decreases, without, however, complete luminescence quenching even at y= 1. K3Gd0.7Eu0.3(VO4)2and K3Gd0.7Eu0.3(PO4)0.3(VO4)1.7were found to exhibit the brightest photoluminescence.  相似文献   

14.
《Optical Materials》2014,36(12):2146-2154
(GdxLu3−x)Ga3Al2O12:0.3 at.%Pr (x = 0.025, 0.05, 0.1, 0.2, 0.4, 0.6) (GLGAG:Pr) polycrystalline powders are prepared by solid-state reaction method. To better understand the luminescence mechanism, the optical diffuse reflectance, photoluminescence emission and excitation, X-ray excited luminescence spectra and decay kinetics of GLGAG:Pr were investigated in detailed, allowing the determination of energy transfer from 5d state of Pr3+ to 4f state of Gd3+, and the non-radiative relaxation from 5d to 4f state of Pr3+. Besides, the former process plays more negative role in the emission quenching of GLGAG:Pr than later one. Pr3+ ion is regarded as an ineffective activation ion in Gd-based multicomponent aluminate garnets. In addition, the wavelength-resolved thermoluminescence spectra of GLGAG:Pr were studied after UV and X-ray irradiation. It is revealed that the localized recombination processes from electron traps to lower lying 4f levels of Pr3+ occurs without populating the higher 5d levels of Pr3+.  相似文献   

15.
Discovery of novel multifunctional fluorescent materials are of great concern to the development of disciplinary crossing and integration. In this work, we prepared a broad-band Eu3+-activated Lu2MoO6 multifunctional material for potential warm white light-emitting diodes (w-LEDs) and temperature sensor applications. Lu1.9MoO6:0.1Eu3+ phosphor was synthesized by high-temperature solid-state reaction method, and the structure characterization was investigated for the first time. The excitation spectrum of this phosphor exhibits the intense broad band ranging from 250?nm to 440?nm assigned to the O2?-Mo6+ charge transfer band (CTB) transition, and a strong red emission centered at 610?nm corresponding to the 5D0?→?7F2 transition of Eu3+ ions were detected under 365?nm excitation. Importantly, warm white light composite material was hybridized via blending commercial green, blue and the present red phosphors, which under 365?nm excitation exhibited a high color rendering index (CRI) of 78 at a correlated color temperature of 4271?K with CIE coordinates of x?=?0.351, y?=?0.308. Furthermore, a strong temperature sensitization phenomenon was found, where the results show that the emission intensities and chromaticity coordinates are sensitive to the temperature, which can provide guidance for the potential application in temperature sensing.  相似文献   

16.
Polycrystalline Cd x Cu1−x Fe2−y Gd y O4 ferrites fory=0·0 and 0·1 were prepared by ceramic technique. X-ray diffractograms of powder samples show cubic symmetry withx⩾0·2 fory=0·0 and 0·1, while compositions withx=0·0 fory = 0·0 and 0·1 are tetragonal. The thermopower measurements for Gd3+-undoped ferrites in the temperature range 300 K to 788 K shown-type conductivity forx⩾0·2. The substitution of Gd3+ changedn-type conductivity of the compositions top-type. The mobilities calculated show decreasing trend on Gd3+ substitution. The values of activation energy ΔE and drift mobilityE d suggest polaron formation in substituted samples. The conduction mechanism is explained on the basis of localized model and formation of Gd3++Fe2+ stable pairs at B site and Cu1++Fe3+ at A site.  相似文献   

17.
K2Gd1?xZr(PO4)3:Eux3+ (0.02  x  0.1, x is in mol.%) were prepared by solid-state reaction method and their photoluminescence properties were investigated in ultra-violet (UV) and vacuum ultra-violet (VUV) region. The phenomenon of visible quantum cutting through downconversion was observed for the Gd3+–Eu3+ couple in this Eu3+-doped K2GdZr(PO4)3 system. Visible quantum cutting, the emission of two visible light photons per absorbed VUV photon, occurred upon the 186 nm excitation of Gd3+ at the 6GJ level via two-step energy transfer from Gd3+ to Eu3+ by cross-relaxation and sequential transfer of the remaining excitation energy. The results revealed that the efficiency of the energy transfer process from Gd3+ to Eu3+ in the Eu3+-doped K2GdZr(PO4)3 system could reach to 155% and K2GdZr(PO4)3:Eu3+ was effective quantum cutting material.  相似文献   

18.
Gd2O3:Eu3+ nanobelts were fabricated by calcination of the electrospun PVP/[Gd(NO3)3 + Eu(NO3)3] composite nanobelts. For the first time, Gd2O2S:Eu3+ nanobelts were successfully prepared via inheriting the morphology and sulfurization of the as-prepared Gd2O3:Eu3+ nanobelts precursor using sulfur powders as sulfur source by a double-crucible method we newly proposed. X-ray diffraction analysis indicated that Gd2O2S:Eu3+ nanobelts were pure hexagonal in structure with space group P \( \bar{3} \) m1. Scanning electron microscope analysis results showed that the width and thickness of the Gd2O2S:Eu3+ nanobelts were ca. 2.1 μm and 129 nm, respectively. Under the excitation of 330-nm ultraviolet light, Gd2O2S:Eu3+ nanobelts emitted red emissions of predominant peaks at 628 and 618 nm which were attributed to the 5D0 → 7F2 energy levels transitions of the Eu3+ ions. It was found that the optimum doping molar concentration of Eu3+ ions in Gd2O2S:Eu3+ nanobelts was 5 %. Possible formation and sulfurization mechanisms of Gd2O2S:Eu3+ nanobelts were also proposed. This new sulfurization technique is of great importance, not only can inherit the morphology of rare earth oxides, but also can fabricate pure-phase rare earth oxysulfides at low temperature compared with conventional sulfurization method.  相似文献   

19.
Eu3+-Y3+ co-doping Ca0.54Sr0.34?1.5x Eu0.08Y x (MoO4) y (WO4)1?y (x = 0.01, 0.02, 0.04, 0.06, 0.08, 0.10, 0.12, 0.14, 0.16, 0.18, 0.20. y = 0, 0.1, 0.2, 0.4, 0.6, 0.8, 1.0), have been prepared and their luminescent properties are investigated to seek a new red-emitting phosphor for ultraviolet-light emitting diodes chips. In absorption efficiency, luminescent intensity and chromaticity coordinates, Ca0.54Sr0.22(MoO4)0.2(WO4)0.8:0.08Eu3+, 0.08Y3+ phosphor is better than commercial Y2O2S:Eu3+ phosphor excited by 390?C405 nm light emitting diodes chip.  相似文献   

20.
We fabricated a series of Y3Al5O12:Mn4+ and Y1?yLuyAl5O12:Mn4+ phosphors by a solid state reaction. The phase and the optical properties of the synthesized phosphors were investigated. Under the excitation at 465 nm, Y3Al5O12:Mn4+ phosphors show emission bands locating at deep red regions, which is induced by the spin- and parity-forbidden 2Eg → 4A1g transitions of Mn4+. The substitution of Y3+ by Lu3+ decreases the lattice parameter and thus strengthens the crystal field strength, which gives rise to the blue shift of emission band for Y1?yLuyAl5O12:Mn4+ phosphors. Due to the compensation of red light by Y3Al5O12:Mn4+ or Y1?yLuyAl5O12:Mn4+ phosphor, the values of correlated-color-temperature for fabricated LEDs are decreased, which leads to the suitable application for them in indoor illumination.  相似文献   

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