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1.
Luminescence and energy transfer properties of EuWO4Cl and Gd0.99Eu0.01WO4Cl are reported. Emission due to a small amount of second phase has been observed for both samples. Energy migration among the Eu3+ ions has been observed for EuWO4Cl. The temperature dependence of the migration rate can be explained assuming phonon-assisted energy transfer. The interaction between the Eu3+ ions is probably multipole-multipole in character.  相似文献   

2.
The luminescence properties of La3WO6Cl3 are reported and discussed. The tungstate group occurs as a trigonal prismatic WO6?6 complex. The blue luminescence is, for the greater part, quenched at room temperature. No energy migration occurs in this lattice. The decay times are discussed in terms of a simple molecular-orbital (MO) scheme. The luminescence of the following activating ions was studied: Mo6+, Bi3+, Eu3+, Sm3+, Ce3+, and Tb3+. The molybdate group produces a red emission with low efficiency. The Bi3+ ion induces a narrow band emission with small Stokes shift. This is interpreted using a Bi3+O2?W6+ charge-transfer state. Except for Ce3+, the rare earth activators show luminescence, but the total transfer efficiency from tungstate to the rare-earth ions is low. This is not due to the one-step tungstate-rare-earth transfer (which is efficient), but to the localized nature of the tungstate excitation. The Eu3+ charge-transfer band is at very low energies.  相似文献   

3.
By using a hydrothermal method, a series of Eu3+ concentration dependent GdF3 nanocrystals have been synthesized. The crystalline structures of samples are characterized by XRD patterns, the morphology and size of the samples are illustrated by FE-SEM images, and the optical properties of the samples are presented by PL excitation and emission spectra. The energy transfer from host Gd3+ to Eu3+ is observed in the Eu3+ doped GdF3 nanocrystals. The optical properties of Eu3+ and the energy transfer efficiency from host Gd3+ to Eu3+ are discussed on the basis of the Eu3+ concentration dependent integrated PL excitation and emission spectra of Gd3+ and Eu3+. The discussion on optical properties of Eu3+ and the energy transfer from Gd3+ to Eu3+ is meaningful to design and synthesize Gd3+ based compounds.  相似文献   

4.
Red phosphors gadolinium tungstate and molybdate with the formula Gd(2−x)MO6:Eux3+ (M=Mo, W) were successfully synthesized by the solid-state reaction at 900 and 1300 °C for 4 h, respectively. The products were characterized by an X-ray powder diffractometer (XRD), TG-DSC, FT-IR, PL, UV-vis and SEM. Room-temperature photoluminescence indicated that the as-prepared Gd(2−x)MO6:Eux3+ (M=Mo, W) had a strong red emission, which is due to the characteristic transitions of Eu3+ (5D07FJ, J=0, 1, 2, 3, 4) for these phosphors. Meanwhile, the 5D07F2 is in the dominant position. The emission quantum efficiency of Eu3+ in the Gd(2−x)MO6:Eux3+ (M=Mo, W) system has been investigated. The XRD results indicate that both Gd2WO6 and Gd2MoO6 belong to the monoclinic system with space group C2/c [A. Bril, G. Blasse, J. Chem. Phys. 45 (1966) 2350-2356] and I2/a [A. Bril, G. Blasse, J. Chem. Phys. 45 (1966) 2350-2356], respectively. SEM images indicate that the shape of Gd1.96WO6:Eu0.043+ is aggregated small particles with a mean diameter of about 300 nm, and the shape of Gd1.96MoO6:Eu0.043+ is block-like structures.  相似文献   

5.
A new Zn and Eu tungstate was characterized by spectroscopic techniques. This tungstate, of the formula ZnEu4W3O16, crystallized in the orthorhombic system and was synthesized by a solid‐state reaction. It melts incongruently at 1330°. The luminescent properties, including excitation and emission processes, luminescent dynamics, and local environments of the Eu3+ ions in ZnEu4W3O16 and ZnY4W3O16 : Eu3+ diluted phases (1, 5, and 10 mol‐% of Eu3+ ion) were studied basing on the f6‐intraconfigurational transitions in the 250–720 nm spectral range. The excitation spectra of this system (λem 615 and 470 nm) show broad bands with maxima at 265 and 315 nm related to the ligand‐to‐metal charge‐transfer (LMCT) states. The emission spectra under excitation at the O→W (265 nm) and O→Eu3+ (315 nm) LMCT states present the blue‐green emission bands. The emission of tungstate groups mainly originate from the charge‐transfer state of excited 2p orbitals of O2? to the empty orbitals of the central W6+ ions. On the other hand, in the emission of the Eu3+ ions, both the charge transfer from O2? to Eu3+ and the energy transfer from W6+ ions to Eu3+ are involved. The emission spectra under excitation at the 7F05L6 transition of the Eu3+ ion (394 nm) of ZnY4W3O16 : Eu3+ diluted samples show narrow emission lines from the 5D3, 5D2, and 5D1 emitting states. The effect of the active‐ion (Eu3+) concentration on the colorimetric characteristic of the emissions of the compound under investigation are presented.  相似文献   

6.
《Chemical physics letters》1987,133(5):425-428
The luminescence of NaGdF4:Ce,Eu has been investigated. After excitation of Ce3+ ions at room temperature, energy transfer to the Gd3+ions occurs, followed by migration over this sublattice to the Eu3+ions, resulting mainly in Eu3+ emission. At liquidhelium temperatures mainly Gd3+6P trap emission is observed. The Eu3+ emission in this system is remarkable, because ultraviolet Eu3+ emission (5H3-7FJ) is observed alongside the normal 5DJ emission in the visible region.  相似文献   

7.
Searching efficient red phosphors under near‐UV or blue light excitation is practically important to improve the current white light‐emitting diodes (WLEDs). Eu2+‐ and Mn4+‐based red phosphors have been extensively studied. Here we proposed that Eu3+ is also a promising activator when it resides on a noncentrosymmetric coordination site. We proved that Cd4GdO(BO3)3 is a good host, which has a significantly distorted coordination for Eu3+. A careful crystallographic study was performed on the solid solutions of Cd4Gd1‐xEuxO(BO3)3 (0≤x≤1) by Rietveld refinements. The as‐doped Eu3+ cations locate at the Gd3+ site and are well separated by CdO8, CdO6 and BO3 groups; thus, only a slight concentration quenching was observed at ≈80 atom % Eu3+. Most importantly, the parity‐forbidden law of 4f‐4f transitions for Eu3+ are severely depressed, thus the absorptions at ≈393 and ≈465 nm are remarkable. Cd4Gd0.2Eu0.8O(BO3)3 can be pumped by a 395 nm LED chip to give a bright red emission, and when mixed with other commercial blue and green phosphors, it can emit the proper white light (0.3657, 0.3613) with a suitable Ra≈87 and correlated colour temperature ≈4326 K. In‐situ photoluminescence study indicated the low thermal quenching of these borate phosphors, especially under 465 nm excitation. Our case proves the practicability to develop near‐UV excited red phosphors in rare‐earth‐containing borates.  相似文献   

8.
采用sol-gel法合成了系列发光体Li2O-Ln2O3-SiO2:Eu^3^+,Bi^3^+,并确定了发光体的物相结构。当Ln^3^+=Y^3^+和Ln^3^+=La^3^+时,紫外光激发下Eu^3^+的发射分别以红光和橙光为主,只存在一种Eu^3^+发光中心;Ln^3^+=Gd^3^+时,至少存在两种Eu^3^+发光中心和两种Bi^3^+发光中心(共掺杂Eu^3^+,Bi^3^+的吸收和发射所  相似文献   

9.
The multicolor Gd2O2S:xTb3+, yEu3+ hollow spheres were successfully synthesized via a template-free solvothermal route without the use of surfactant from commercially available Ln (NO3)3·6H2O (Ln = Gd, Tb and Eu), absolute ethanol, ethanediamine and sublimed sulfur as the starting materials. The phase, structure, particle morphology and photoluminescence (PL) properties of the as-obtained products were investigated by X-ray diffraction (XRD), fourier transform infrared spectroscopy (FT-IR), field emission scanning electron microscopy (FE-SEM) and photoluminescence spectra. The influence of synthetic time on phase, structure and morphology was systematically investigated and discussed. The possible formation mechanism depending on synthetic time t for the Gd2O2S phase has been presented. These results demonstrate that the Gd2O2S hollow spheres could be obtained under optimal condition, namely solvothermal temperature T = 220 °C and synthetic time t = 16 h. The as-obtained Gd2O2S sample possesses hollow sphere structure, which has a typical size of about 2.5 μm in diameter and about 0.5 μm in shell thickness. PL spectroscopy reveals that the strongest emission peak for the Gd2O2S:xTb3+ and the Gd2O2S:yEu3+ samples is located at 545 nm and 628 nm, corresponding to 5D47F5 transitions of Tb3+ ions and 5D07F2 transitions of Eu3+ ions, respectively. The quenching concentration of Tb3+ ions and Eu3+ ions is 7%. In the case of Tb3+ and Eu3+ co-doped samples, when the concentration of Tb3+ or Eu3+ ions is 7%, the optimum concentration of Eu3+ or Tb3+ ions is determined to be 1%. Under 254 nm ultraviolet (UV) light excitation, the Gd2O2S:7%Tb3+, the Gd2O2S:7%Tb3+,1%Eu3+ and the Gd2O2S:7%Eu3+ samples give green, yellow and red light emissions, respectively. And the corresponding CIE coordinates vary from (0.3513, 0.5615), (0.4120, 0.4588) to (0.5868, 0.3023), which is also well consistent with their luminous photographs.  相似文献   

10.
The luminescence of CaWO4Hg and CaMoO4Hg is reported. The presence of Hg2+ ions in the CaWO4 lattice influences the luminescence of pure CaWO4 drastically due to efficient energy transfer from host lattice groups to the emitting centre consisting of a tungstate group with a neighbouring mercuric ion. The luminescence characteristics of CaMoO4Hg do not differ strongly from those of pure CaMoO4 due to the absence of efficient energy transfer.  相似文献   

11.
Solid solutions were prepared encompassing the entire composition range between LaTiO3 and GdTiO3. An anomaly in the magnetization-temperature data associated with magnetic ordering within the Ti3+ sublattice was observed for the phases La0.5Gd0.5TiO3LaTiO3. La0.3Gd0.7TiO3GdTiO3 appear to be two sublattice ferrimagnets. Anomalies in the magnetization-temperature curves observed for the compositions La0.6Gd0.4TiO3La0.8Gd0.2TiO3 are consistent with spin glass behavior. The saturation magnetization of GdTiO3 at 4.2K was measured to be 5.8 ± 0.2 μB/formula unit. Susceptibility data analyzed using the mean field model show a dramatic decrease in the strength of the ferromagnetic Ti3+Ti3+ exchange on the dilution of the Gd3+ sublattice by even 5% La3+.  相似文献   

12.
A stable and biocompatible MOF-based thermometer utilizing back energy transfer has been developed, which exhibits ultrasensitive temperature sensing performance in the physiological temperature range.  相似文献   

13.
Eu2+-doped inorganic-organic hybrid materials, which are potentially suitable for a tunable laser in the near ultra violet and blue region, were prepared through the photoreduction of Eu3+ ions in the materials under the irradiation of the fourth harmonic wave light (266 nm) of the Nd:YAG laser. The hybrid materials doped with Eu3+ ions were prepared from Si(OCH3)4, CH3Si(OCH3)3, EuCl3 and chloropropyltrimethoxysilane (CPTM). After the prehydrolized silica sol was added to the Eu3+-containing solution, Eu3+-doped transparent inorganic-organic hybrid material was obtained by drying at 50°C. The emission peak around 450–475 nm due to the charge transfer transition (5d-4f) of Eu2+ ions increased with the laser irradiation time. Eu3+ ions were effectively photoreduced to Eu2+ ions in pore-free materials prepared at high CPTM to Eu3+ ratios. Eu2+ ions were generated by the photodecomposition of the bond between Eu3+ and Cl (Cl or Cl(CH2)3 in CPTM).  相似文献   

14.
Eu3+-doped Gd3PO7 nanospheres with an average diameter of ∼300 nm and a narrow size distribution have been prepared by a facile combustion method and structurally characterized by X-ray diffraction and field emission scanning electron microscopy. The luminescent properties were systemically studied by the measurement of excitation/emission spectra, and emission spectra under different temperatures, as well as by photostability. The strong red-emission intensity peaking at 614 nm originates the 5D07F2 transition and is observed under 254-nm irradiation, indicating that Eu3+ ions in Gd3PO7 mainly occupied non-centrosymmetry sites. The CIE1931 XY chromaticity coordinates of Gd3PO7:Eu3+ nanospheres are (x=0.654, y=0.345) in the red area, which is near the National Television Standard Committee standard chromaticity coordinates for red. Thus, Gd3PO7:Eu3+ nanospheres may be potential red-emitting phosphors for PDP and Xe-based mercury-free lamps.  相似文献   

15.
16.
The luminescence of Ce3+, Sm3+, Eu3+, Gd3+, Tb3+, and Dy3+ in NaLn(SO4)2H2O (Ln = lanthanide) is reported. Only Ce3+, Gd3+, and Tb3+ show efficient emission. This is explained in terms of an energy-gap law. Energy transfer is studied in several codoped compositions. The mutual transfer between Gd3+ ions is the only one encountered with high probability. The several transfers are discussed and where possible their rates are calculated.  相似文献   

17.
以P123为表面活性剂,异丙醇铝为铝源,用简易溶胶-凝胶法,获得了单掺和双掺Gd3+,Eu3+的介孔氧化铝组装体。用广角X-射线衍射仪(WAXD)进行了物相分析;小角X-射线衍射仪(SAXD)、比表面仪进行了孔结构分析和形貌表征;研究了组装体的发光性能并发现Gd3+对Eu3+有能量传递作用,并分析了能量传递过程。  相似文献   

18.
Luminescence and energy transfer properties of Gd2Ti2O7: Eu and Eu2Ti2O7 are reported. Transfer between unperturbed (intrinsic) Eu3+ ions and perturbed (extrinsic) Eu3+ ions has been observed. At low temperatures the emission spectra of Eu2Ti2O7 are dominated by trap emission, due to direct energy transfer from the intrinsic Eu3+ ions to the extrinsic Eu3+ ions. Above 10 K energy migration among the Eu3+ ions to quenching centers occurs. The interaction between the Eu3+ ions is probably exchange in character. The nature of the extrinsic Eu3+ ions has been elucidated.  相似文献   

19.
Europium-doped nanocrystalline GdVO4 phosphor layers were coated on the surface of preformed submicron silica spheres by sol-gel method. The resulted SiO2@Gd0.95Eu0.05VO4 core-shell particles were characterized by X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), scanning electron microscopy (FESEM), energy-dispersive X-ray spectra (EDS), transmission electron microscopy (TEM), photoluminescence (PL) spectra, low voltage cathodoluminescence (CL), time resolved PL spectra and kinetic decays. The XRD results demonstrate that the Gd0.95Eu0.05VO4 layers begin to crystallize on the SiO2 spheres after annealing at 600 °C and the crystallinity increases with raising the annealing temperature. The obtained core-shell phosphors have spherical shape, narrow size distribution (average size ca. 600 nm), non-agglomeration. The thickness of the Gd0.95Eu0.05VO4 shells on the SiO2 cores could be easily tailored by varying the number of deposition cycles (50 nm for four deposition cycles). PL and CL show that the emissions are dominated by 5D0-7F2 transition of Eu3+ (618 nm, red). The PL and CL intensities of Eu3+ increase with increasing the annealing temperature and the number of coating cycles. The optimum concentration for Eu3+ was determined to be 5 mol% of Gd3+ in GdVO4 host.  相似文献   

20.
Rare-Earth Actived Sol-Gel Films for Scintillator Applications   总被引:2,自引:0,他引:2  
Recently, there has been a growth of interest in new phosphors preparation for high resolution X-rays imaging systems. Sol-gel method has been used to synthesize europium doped gadolinium and lutetium oxide films. Structural and optical results are investigated and discussed on both Gd2O3:Eu3+ (5 mol%) and Lu2O3:Eu3+ (5 mol%). Those films are crystallized into cubic phase and present a density of 7.1 g/cm3 and 8.4 g/cm3 for Gd2O3:Eu3+ and Lu2O3:Eu3+ respectively. Room temperature emission spectra using an excitation of 468 nm was used to obtain the intense red emission 5D0 7F2 (611 nm) of Eu3+. Scintillation properties at 611 nm are finally proved using X-rays excitation.  相似文献   

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