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1.
Terbium (0, 2, and 4?at%)-doped ZnS quantum dots (QDs) were synthesized via a solvothermal method. The crystal structures of the synthesized QDs were determined to be zinc blend by X-ray powder diffraction (XRD) and Raman analyses. Transmission electron microscopy (TEM) studies revealed that particles with a mean size of 2–4?nm were formed. An X-ray photo electron spectroscopy (XPS) examination disclosed the existence of terbium with a trivalent state in the ZnS host lattice. The absorption bands of all QDs were located around 325?nm (3.81?eV) and were higher than that of the bulk ZnS band gap (3.67?eV), consistent with the quantum confinement effect. The photoluminescence spectra of the terbium-doped samples displayed five emission peaks at 467?nm (5D47F3), 491?nm (5D47F6), 460?nm (5D47F5), 484?nm (5D47F4), and 530?nm (5D47F3), respectively. The terbium-doped QDs exhibited a higher photocatalytic activity during the degradation of crystal violet dye under UV-light illumination compared to the undoped ZnS QDs. These interesting properties of terbium-doped ZnS QDs are potentially useful for both luminescent and photocatalysis applications.  相似文献   

2.
In present work, a series of Eu doped zinc borate, ZnB2O4, phosphors prepared via wet chemical synthesis and their structural, surface morphology, cathodoluminescence (CL) and thermoluminescence (TL) properties have been studied. Phase purity and crystal structure of as-prepared samples are confirmed by X-ray diffraction measurements (XRD) and they were well consistent with PDF card No. 39-1126, indicating the formation of pure phase. The thermoluminescence (TL) behaviors of Eu activated ZnB2O4 host lattice are studied for various beta doses ranging from 0.1 to 10?Gy. The high-temperature peak of Eu activated sample located at 192?°C exhibited a linear dose response in the range of 0.1–10?Gy. Initial rise (IR) and peak shape (PS) methods were used to determine the activation energies of the trapping centres. The effects of the variable heating rate on TL behaviour of Eu activated ZnB2O4 were also studied. When excited using an electron beam induced light emission (i.e cathodoluminescence, CL) at room temperature (RT), the as-prepared phosphors generate reddish-orange color due to predominant emission peaks of Eu3+ ions located at 576–710?nm assigned to the 5D07FJ (J=1,2,3, and 4) transitions. The maximum CL intensity for Eu3+ ions at 614?nm with transition 5D07F2 was reached Eu3+ concentration of 5?mol%; quenching occurred at higher concentrations. Strong emission peak for Eu3+ ions at 614?nm with transition 5D07F2 is observed. The CL experimental data indicate that ZnB2O4:Eu3+ phosphor as an orange-red emitting phosphor may be promising luminescence materials for the optoelectronic applications.  相似文献   

3.
The coordination complexes of the crystalline structure of cellulose ethers/Eu(III) with fluorescence emission, viz CMC/Eu(III), MC/Eu(III), and HEC/Eu(III), were synthesized and characterized. Results showed the emission spectra of Eu3+ ions in these coordination compounds, which originates from electric dipole transition. The main emission peak at 615 nm generated from 5D07F2 transition of Eu3+ ions. Their absorption and excitation spectra were different, because the effect of the high polarity of water and having both hydrogen bond donor and acceptor properties on the excited molecule is different from the effect on the ground state of the molecule. Our study demonstrated that the Degree of Substitute (DS) of CMC could influence the fluorescence intensity (FI) of CMC/Eu(III). The emission intensity of CMC/Eu(III) varies with the DS of CMC. For example, when the DS of CMC was 0.89, the FS (fluorescent spectra) of solid CMC/Eu(III) displayed three emission peaks Eu(III): the strongest emission peak at 615 nm (5D07F2 transition) and other two weaker peaks at 583 nm (5D07F1 transition) and at 652 nm (5D07F3 transition), respectively. The concentration of Eu(III) could also affect the FI of these coordination complexes. The FI of the coordination complexes peaked at 615 nm all reached maximum when Eu3+ concentration was at 5% (wt/wt). © 2004 Wiley Periodicals, Inc. J Appl Polym Sci 95: 743–747, 2005  相似文献   

4.
Eu3+-doped NaBaPO4 was prepared by a high-temperature solid-state reaction. The phase formation was confirmed by X-ray powder diffraction measurements. The laser site-selective excitation and emission spectra have been investigated in the 5D0 → 7F0 region by using a pulsed, tunable and narrowband dye laser. The excitation spectra corresponding to the 7F0 → 5D0 transition consist of two transitions at 579.6 nm Eu(I) and 578.9 nm Eu(II), indicating the Eu3+ ions occupy two crystallographic sites of Ba2+ ions. The decay lifetimes of the two Eu3+ sites were measured. Two crystallographic sites for Eu3+ ions doped in NaBaPO4 lattice were assigned from the luminescence characteristic and structure features. Meanwhile, the charge compensation mechanism of Eu3+ doping in NaBaPO4 was discussed.  相似文献   

5.
Eu-based vanadate Ca9Eu(VO4)7 phosphor was synthesized by the solid state reaction method and was characterized by X-ray powder diffraction (XRD). The photoluminescence excitation and emission spectra, fluorescence decay curves and the dependence of luminescence intensity on temperature were investigated. The phosphor can be efficiently excited by near UV light to realize an intense red luminescence (614 nm) corresponding to the electric dipole transition 5D07F2 of Eu3+ ions. The crystallographic site-occupations of the Eu3+ ions in Ca9Eu(VO4)7 were investigated by the site-selective excitation and emission spectra, and the fluorescence decay curves in the 5D07F0 region using a pulsed, tunable, narrowband dye laser. The red luminescence together with the thermal stability was discussed on the base of the Eu3+ site-distribution in Ca9Eu(VO4)7 host.  相似文献   

6.
BaTiO3 and BaSnO3 samples doped with Eu3+ ions were prepared using glycine‐nitrate gel combustion method. Relative intensities and line shapes of magnetic dipole allowed 5D07F1 and electric dipole allowed 5D07F2 transitions of Eu3+ from the hosts, BaTiO3 and BaSnO3, are significantly different. Based on detailed structural investigations, it is confirmed that synthesizedBaTiO3 sample is tetragonal with no center of symmetry around Ba2+ ions. Unlike this BaSnO3 is cubic with centrosymmetric Ba2+ site. From X‐ray diffraction and experimentally obtained Judd–Ofelt parameters (Ω2 and Ω4 values), it is confirmed that in BaTiO3 there is a decrease in the average Ba–O and Ba–Ba distances compared with that in BaSnO3. This leads to higher Eu–O bond polarizability and adds to the distortion in its environment around Eu3+ in BaTiO3:Eu compared with BaSnO3:Eu. This is responsible for the observed difference in the luminescence properties.  相似文献   

7.
Europium-doped yttrium orthovanadate/polyethylene oxide nanofibers were fabricated by firstly, synthesizing crystalline YVO4:Eu3+ nanoparticles using an aqueous precipitation method followed by electrospinning of PEO/YVO4:Eu3+ polymer composites. X-ray diffraction patterns showed that the nanoparticles exhibited well-defined peaks that were indexed as the tetragonal phase of YVO4. No additional peaks of other phases were observed indicating that Eu3+ ions were effectively built into the YVO4 host lattice. The photoluminescence spectra for the nanofibers showed peaks at 593, 615, 650, and 698 nm which was ascribed to the 5D0? 7F1, 5D0? 7F2, 5D0? 7F3 and 5D0? 7F4 transitions of Eu3+. Due to an efficient energy transfer from vanadate groups to Eu3+, the composite nanofibers showed a strong red emission under ultraviolet excitation characteristic of the red luminescence of the europium ion. The results demonstrate that this synthetic approach could prove to be viable for the fabrication of rare earth/polymer composite nanofibers intended for luminescent device applications.  相似文献   

8.
Eu3+ ions-doped cubic mesoporous silica thin films with a thickness of about 205 nm were prepared on silicon and glass substrates using triblock copolymer as a structure-directing agent using sol–gel spin-coating and calcination processes. X-ray diffraction and transmission electron microscopy analysis show that the mesoporous silica thin films have a highly ordered body-centered cubic mesoporous structure. High Eu3+ ion loading and high temperature calcination do not destroy the ordered cubic mesoporous structure of the mesoporous silica thin films. Photoluminescence spectra show two characteristic emission peaks corresponding to the transitions of 5D0-7F1 and 5D0-7F2 of Eu3+ ions located in low symmetry sites in mesoporous silica thin films. With the Eu/Si molar ratio increasing to 3.41%, the luminescence intensity of the Eu3+ ions-doped mesoporous silica thin films increases linearly with increasing Eu3+ concentration.  相似文献   

9.
Using the melt-quench technique, potassium zinc borophosphate (KZnBP) glasses incorporated with Dy3+, Eu3+, and Dy3+/Eu3+ ions individually and combinedly were prepared, and their photoluminescence (PL)-related features were investigated. The KZnBP glass containing an optimized content of Dy3+ (0.5 mol%) is co-doped with Eu3+ in various contents, and the energy transfer (ET) process between them was studied at λexci = 349, 364, 387 (Dy3+), and 394 nm (Eu3+). The Dy3+/Eu3+ co-doped system, when excited with Dy3+ excitations has resulted in a significant decrease in the intensity of Dy3+ peaks observed at 480 nm (4F9/26H15/2, blue) and 574 nm (4F9/26H13/2, yellow), with simultaneous enhancement of the intensity of Eu3+ peaks at 591 nm (5D07F1, orange) and 617 nm (5D07F2, red). This trend is due to the efficient energy transfer from Dy3+ to Eu3+, indicating that Eu3+ ions were sensitized by Dy3+ ions. Dexter's theory and the Inokuti–Hirayama (I–H) model revealed that the dipole–dipole interaction is accountable for the energy transfer from Dy3+ to Eu3+ through energy-transfer channels [4F9/2(Dy3+)+7F1,2(Eu3+)→6H15/2(Dy3+)+5D2(Eu3+)] and [4F9/2(Dy3+)+7F0(Eu3+)→6H13/2(Dy3+)+5D0(Eu3+)]. The color coordinates of the Dy3+/Eu3+ co-doped glasses under various excitations fall within the white light emission spectrum, indicating their potential application in warm white LEDs.  相似文献   

10.
The rare earth (RE = Eu and Tb) ions‐doped α‐Zr(HPO4)2 (ZrP) nanosheet phosphors were synthesized by direct precipitation method, and their structures and photoluminescence properties were investigated. The results of X‐ray diffraction and scanning electron microscopy indicated that the systems of ZrP:RE3+ had similar nanosheet structure except with relatively larger interlayer spacing as compared with pure α‐ZrP. Under the excitation of UV light, the ZrP:RE3+ nanosheet phosphors showed red and green emission peaks corresponding to the 5D07F2 transition of Eu3+ and the 5D47F5 transition of Tb3+, respectively. After Eu3+ and Tb3+ were co‐doped in ZrP host, not only the red and green emission peaks were simultaneously observed, but also the luminescent intensity and fluorescence lifetimes of Tb3+ were gradually decreased with the increase in Eu3+‐doping concentration, which implied the energy transfer from Tb3+ to Eu3+ happened. It was deduced that the energy transfer from Tb3+ to Eu3+ occurred via exchange interaction. Through optimization to the samples, a nearly white‐light emission with the color coordinate (0.322, 0.263) was achieved under 377 nm excitation. The ZrP:RE3+ nanosheet phosphors may be a potential color‐tailorable candidate for fabricating optoelectronic devices such as electroluminescence panels.  相似文献   

11.
In this work, the role of europium doping of glasses formulated in the ternary system ZnO–CdO–TeO2 is described. The Eu‐doped oxide glasses were prepared by the conventional melt‐quenching method and by using three different compositions. Structural studies reveal that there exists a good affinity between Cd and some rare earth (RE) ions to form the crystalline phase. The X‐ray diffraction (XRD) diagrams display that the structure of these glasses is amorphous and with the increase in CdO content and the compatibility of Eu3+, there is a tendency to form nanocrystals of CdTe2O5. The scanning electron microscopic (SEM) observation of their microstructure confirms the presence of phase separation. Differential thermal analysis (DTA) of these glasses showed small exothermic peaks noted around 450°C for the V2 glass and 480°C for V1 and V3 glasses, which could be attributed to the formation of these crystals. The infrared spectra showed a main absorption band around 800–600 cm?1 corresponding to the Te–O stretching mode in TeO4 and TeO3 groups. By optical absorption (OA), the band gap (Eg) for each glass was determined; these values were 3.27, 3.14, and 3.3 eV for the V1–V3 glasses, respectively. Furthermore, the presence of Eu3+ was detected in the 370–470 nm short‐range wavelengths. The photoluminescence (PL) experiments of the glasses showed light emission due to the following transitions: 5D07F1, 5D07F2, 5D07F3, and 5D07F4.  相似文献   

12.
《Ceramics International》2022,48(16):23213-23223
Red phosphors with a high quantum yield and a lower thermal quenching are needed to improve the luminescence efficiency and the stability of phosphor-converted white light-emitting diodes (pc-WLEDs). We have designed a high quantum yield NaGdSiO4 (NGSO) based phosphor with enhanced Eu3+ emissions of the 5D07F1 and 5D07F2 transitions. This design is based on the Eu3+ at both the inversion and non-inversion symmetry sites. In detail, we have studied the structure, morphology, and luminescence properties of NGSO: Eu3+ phosphors. Using a 394 nm UV excitation, a series of Eu3+ emissions of 5D07FJ (0–4) transitions has been observed. The internal quantum efficiency (IQE) is 83.42% and the red color purity is 91.4%. These values are much higher than some reported results. The higher IQE and double intense 5D07F1 and 5D07F2 emissions might originate from an unusual structure disorder around Eu3+ ions in the NGSO lattice. The lifetime of the optimal phosphor NGSO: 0.5Eu3+ is about 2 ms, suitable for solid-state lighting. The intensities of the strong emissions at 595 and 624 nm of NGSO: 0.5Eu3+ at 150 °C is about 85% of that at 30 °C, demonstrating its excellent thermal stability. Furthermore, this red NGSO: 0.5Eu3+ phosphor was packaged into a warm pc-WLED, exhibiting a lower correlated color temperature (CCT) of 4222 K and a comparable color rendering index (CRI) of 86.7. These results show that this red phosphor could act as a red component of pc-WLEDs excited by the n-UV LED chip.  相似文献   

13.
Energy conservation and environmental safety are the key requirements in the modern world. We report novel orange-emitting double perovskite Ba2LaNbO6:Eu3+ (BLN:Eu3+) nanophosphor fabricated using a citrate sol-gel method for use in general illumination and photocatalysis. After annealing at 800?℃, the particles exhibited a nanorod-like morphology with monoclinic structure. The photoluminescence emission spectra exhibited an intense 5D07F1 transition at 594?nm and a moderate 5D07F2 transition at 615?nm, demonstrating that the Eu3+ ions occupied the La3+ sites with inversion symmetry. The optimal concentration of Eu3+ ions was found to be about 5?mol% for the BLN host lattice. Energy transfer from the NbO67- octahedrons to the Eu3+ ions was clearly witnessed when the BLN:Eu3+ nanophosphors were excited with both the characteristic excitation bands of Eu3+ (7F05L6) and NbO67- octahedrons at 392 and 380?nm, respectively. The thermal quenching temperature of 5?mol% Eu3+ ions doped BLN nanophosphors was found to be 183?℃, indicating that these nanophosphors are very stable at high temperatures. In addition, the dye removal efficiency of the proposed BLN nanophosphors was verified using Rhodamine B (RhB) dye as a model pollutant under UV irradiation. Compared to a commercial nano-ZnO catalyst, our synthesized BLN nanophosphors showed superior RhB de-colorization efficiency. Therefore, the proposed BLN:Eu3+ nanophosphors are promising multifunctional materials for photocatalysis and general lighting applications.  相似文献   

14.
《Ceramics International》2017,43(11):8424-8432
Nanocrystalline β-PbF2 phase singly-doped with Eu3+ and Tb3+ ions have been successfully synthesized using sol-gel technique and subsequent heat-treatment of xerogels at 350 °C. Thermal behavior and structural properties of obtained materials were studied using thermogravimetric analysis (TG), differential scanning calorimetry (DSC) as well as FT-IR and Raman techniques. XRD results confirmed formation of β-PbF2 nanocrystals embedded in silica amorphous hosts after annealing at 350 °C. Moreover, the photoluminescence properties have been investigated based on excitation and emission spectra as well as decay analysis from the 5D0 (Eu3+) and the 5D4 (Tb3+) excited states. The sharp intraconfigurational 4f6−4f6 and 4f8−4f8 emission transitions assigned as the 5D07FJ (J=0–4) of Eu3+ and the 5D47FJ (J=6-3) of Tb3+ bands, respectively, were registered. The most prominent bands in studied xerogels and glass-ceramic materials are related to the following electronic transitions: 5D07F1 (orange) and 5D07F2 (red) (Eu3+) as well as 5D47F5 (green) and 5D47F6 (blue) (Tb3+). Thus, the R/O (Eu3+) and G/B (Tb3+) luminescence intensity ratios were calculated and analyzed. Luminescence decay kinetic clearly indicated a presence of two different surroundings around Eu3+ and Tb3+ dopants in β-PbF2-based glass-ceramic samples. In such singly-doped with Eu3+ and Tb3+ materials, the longer luminescence lifetimes (Eu3+: τ1(5D0)=0.90 ms, τ2(5D0)=5.15 ms; Tb3+: τ1(5D4)=0.48 ms, τ2(5D4)=4.01 ms) of an appropriate excited states were achieved in comparison to xerogel hosts (Eu3+: τ(5D0)=0.38 ms; Tb3+: τ(5D4)=0.49 ms). The obtained results indicate the incorporation of Eu3+ and Tb3+ ions into nanocrystalline phase during ceramization process.  相似文献   

15.
《Ceramics International》2019,45(16):20405-20413
A series of Eu3+/Eu2+ codoped Ca2Al2SiO7 were synthesized by traditional solid-state synthesis in reducing atmosphere. In this work, XRD powder diffraction proved that the obtained sample was pure. Photoluminescence properties are characterized by excitation, emission spectra and decay curves. Double center emission is achieved by adjusting excitation wavelength and concentration. Under the 394 nm excitation, the emission spectra Ca2Al2SiO7: Eu phosphors exhibit two bands situated at blue emission of 4f5d-4f transition from Eu2+ ion and red emission of 4f-4f transition coming from Eu3+ ion. The red and yellow light can be obtained when the concentration of doped europium ions is at 0.5% and 1%, respectively. When the excitation wavelength was 394, 280 and 584 nm, the emission color change from yellow to blue, respectively. The bond energy theory explains Eu2+ and Eu3+ ion occupy Ca1 site in the Ca2Al2SiO7 lattices. In addition, the spectra show that the abnormal intensity peaks of europium ion at 701 nm can be found. Analysis of the related intensity 5D0-7F2(618 nm) transition peak is similar to that of 5D0-7F4(701 nm) transition peak in the emission spectra with the Judd-Ofelt theory.  相似文献   

16.
Phosphor particles of spherical shape and uniform size are desired for high-definition displays to improve the resolution and the overall luminescent performance. However, the synthesis of RE3BO6 spherical particles is a considerable challenge in materials science. Here, uniform spheres of RE3BO6 (RE = Eu–Yb, Y) have been converted from their colloidal precursor spheres synthesized via homogeneous precipitation. The amorphous precursor spheres are solid particles with decreased boron going from the surfaces to the cores. Smaller particles were observed at decreased ionic radius from Eu3+ to Ho3+ (including Y3+), but particles with nearly unvaried sizes were observed by further decreasing the ionic radius from Ho3+ to Yb3+. They crystallized in monoclinic RE3BO6 at 900°C, with maintaining the spherical shape of precursors. However, the crystal growth and the densification toward the particle surfaces resulted in the formation of hollow spheres for smaller particles and core-shell structured spheres for larger particles. The parameters, a, b, and c, increase nearly monotonically with increasing the radius of rare earth ions. The uniform spheres of Y3BO6:Eu3+ exhibited a typical red emission at ~613 nm (5D0 → 7F2 electric dipole transition of Eu3+), with an intensity ratio I(5D0 → 7F2)/I(5D0 → 7F1) of ~3.5. The luminescence behavior of Y3BO6:Eu3+ phosphor is dependent on the excitation wavelength, which is closely related to the Eu3+ ions at different coordination sites. Driven by a 460-nm blue-LED chip, the Y3BO6:Eu3+ spheres exhibited a red emission with the CIE coordinates of (~0.65, ~0.35), indicating that they are an excellent red-emitting phosphor candidate for application in white-LEDs.  相似文献   

17.
Enhanced red luminescence in LnVO4: Bi3+, Eu3+ @ SiO2 phosphors has been improved mainly in three stages by investigating the effects of: (i) host composition (Gd, Y and Gd/Y), (ii) co-doping Bi3+ as a sensitizer and finally (iii) SiO2 shell coating. XRD data revealed that the produced phosphors possess crystalline, pure phase with tetragonal structure. Silica coating on phosphor particles have been characterized by SEM/EDAX, TEM, PL and with the presence Si–O–Si, Si–O vibrational modes from the FT-IR spectra. Absorption band edges due to VO43?, shifted to higher wavelength with Bi-concentration, owing to the presence of Bi–O bond in addition to V–O. The emission intensities of 5D07F2 transition are stronger than 5D07F1; indicating the lower inversion symmetry near Eu3+, ions. Red emission intensity due to the efficient energy transfer from VO43? to Eu3+ via Bi3+ ions in Y0.949VO4: Bi3+0.001, Eu3+0.05 phosphor was improved significantly, i.e. 1.6 times compared to Y0.95VO4: Eu3+0.05. This was further enhanced 2.25 times by SiO2 shell coating. Thus, Y0.949VO4: Bi3+0.001, Eu3+0.05 @ SiO2 are suggested to be a promising red phosphor for application in display devices or lighting.  相似文献   

18.
Highly biocompatible and efficiently luminescent whiskers of the hydroxyapatite (Ca10(PO4)6(OH)2, HAp) doped with various concentrations (0-5 at.%) of europium were prepared by hydrothermal synthesis and the Eu-doped Hap-coating layers onto the surface of titanium substrate were fabricated by the electrophoretic deposition (EPD) process for fluorescent probe application. The maximum doping concentration of Eu accommodating into the host lattice of HAp was detected as ~1.5 at.% and all the hydrothermally synthesized Eu-doped HAp whiskers were found to have high crystallinity and orientation growth along the c-axis by X-ray diffraction (XRD) identification. The valence of the doped Eu was identified as trivalent and divalent coexistence at a concentration percentage of Eu3+: Eu2+ = 78%: 22% by X-ray photoelectron spectroscopy (XPS) spectra. The replacement site of the doped Eu ions in the crystal structure of HAp host was clarified by Rietveld refinement. The whisker morphology of the hydrothermally synthesized particle was demonstrated by field-emission scanning electron microscopy (FE-SEM) observation and their component elements were analyzed by energy dispersive X-ray (EDX) mapping. The photoluminescence (PL) emissions of the Eu-doped HAp whiskers and fabricated their coating layers were both revealed mainly at ~615 nm (5D0 → 7F2) and ~697 nm (5D0 → 7F4), which is a wavelength that easily transmitting through living system for biological imaging. The PL emission are falling in the region of reddish orange and belonging to color temperature below 1500 K. Decay time and internal and external quantum efficiencies (QEs) were also measured to reveal them depending on the doping concentration of Eu. The hydrothermally prepared Eu-doped HAp whiskers would be aimed at biomedical application, due to their promising fluorescent function of probe for in vivo imaging in medical diagnose by utilizing the superior biocompatibility of the HAp host and highly efficient luminescent property of the Eu activator.  相似文献   

19.
Luminescent fine crystals of Y1.00?xEuxTiNbO6, x = 0–1.00 with high crystallinity were directly synthesized by mild hydrothermal method from weakly basic precursor solution mixtures of YCl3, EuCl3, TiOSO4, and NbCl5. Orthorhombic aeschynite‐type crystals in the range of 0.5–2.0 μm consisting of crystallites with 33–91 nm based on a complete solid solution in the YTiNbO6–EuTiNbO6 system were hydrothermally formed at 240°C for 5 h. A single phase of as‐prepared aeschynite‐type structure was maintained in all the (Y,Eu)TiNbO6 solid solution after heating at temperatures up to 1000°C for 1 h in air. In the range of composition x ≤ 0.6, the as‐prepared aeschynite‐type (Y,Eu)TiNbO6 solid solutions transformed to a single phase of euxenite structure after heat treatment at temperatures higher than 1100°C–1200°C. The as‐prepared (Y,Eu)TiNbO6 fine crystals in the range of composition x = 0.75–0.90 showed the strongest luminescence in the red spectral region: strong red (5D07F2 transition of Eu3+) and weak orange light (5D07F1) line spectra among the as‐prepared and heat‐treated samples. Another wet chemical synthesis route confirmed the advantage in directly synthesizing the (Y,Eu)TiNbO6 crystals through this hydrothermal method because heating at 1200°C for 1 h in air was necessary for obtaining crystalline (Y,Eu)TiNbO6 with sufficient luminescence intensity in a composition Y0.70Eu0.30TiNbO6 from amorphous powders that were formed via co‐precipitation method.  相似文献   

20.
《Ceramics International》2017,43(17):15107-15114
A series of eulytite-type Sr3Y1-x(PO4)3:xEu3+ (x = 0–0.13) and Sr3-yY(PO4)3:yEu2+ (y = 0–0.10) phosphors were successfully synthesized via gel-combustion and subsequent calcination in O2 and Ar/H2 atmospheres at 1250 °C, respectively. Detailed crystal structure analysis via Rietveld refinement showed that the phosphors were crystallized in the cubic system (space group I-43d, No. 220), in which the Eu3+ and Eu2+ activators reside at the Y3+ and Sr2+ sites, respectively. The trivalent Eu3+ ions (CN = 6) exhibited typical narrow-band luminescence via intra-4f6 transitions, with the red emission at ~ 615 nm being dominant (5D07F2 transition, FWHM = 15.9 ± 0.2 nm). The divalent Eu2+ ions (CN = 6 and 9) showed broad-band luminescence ranging from light-blue to blue via 4f65d1 → 4f7 transitions (FWHM = 115 ± 2 nm). The optimal Eu3+ and Eu2+ concentrations were determined to be 10 at% (x = 0.10) and 7 at% (y = 0.07), respectively, and the mechanisms of concentration quenching were discussed. The excitation/emission properties, fluorescence decay kinetics, CIE chromaticity, and particularly the rarely addressed thermal stability of the phosphors were investigated in detail.  相似文献   

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