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1.
Absolute quantum yields and luminescence lifetimes were measured for Eu, Tb, Gd, formates and Y formate activated by Eu3+ as functions of temperature, deuterium substitution in ligands, and Eu3+ concentration in Y formates. Radiative and nonradiative transition probabilities in the lanthanide formates were determined using the quantum yield φ and luminescence lifetime τ. The probabilities of radiative transitions in Eu3+ were also found by employing corrected luminescence spectra. Relaxation mechanisms of electronic excitation energy in the studied crystals were discussed.  相似文献   

2.
The theory of multiphonon vibronic coupling to electronic transitions is applied in analysing fluorescence spectra of Eu2+ in BaFCI, which consist of the 4f7(6P7/2,) → 4f7(8S7/2) and 4f65d → 4f7 transitions, and the 4f7-4f65d excitation spectrum of Ce3+ in YPO4. The 4f electrons are weakly coupled to lattice vibration modes so that only weak one- and two-phonon sidebands are observable in the 4f-4f optical transitions, whereas the electron-phonon coupling is significantly stronger for a 5d electron. Accordingly, intensive multiphonon vibronic transitions overwhelmingly dominate the 4f65d → 4f7 spectrum. It is shown that the extended Judd-Ofelt theory for weak vibronic coupling in the framework of the M-process is equivalent to the Huang-Rhys theory for the δ-process. In the analysis of experimental data, contributions from local ligand modes and lattice acoustic modes are separated, and the coupling strength is evaluated, in terms of the Huang-Rhys parameter S, for the 4f-4f and 5d-4f vibronic transitions.  相似文献   

3.
Fluorinated Eu‐doped SnO2 nanostructures with tunable morphology (shuttle‐like and ring‐like) are prepared by a hydrothermal method, using NaF as the morphology controlling agent. X‐ray diffraction, field‐emission scanning electron microscopy, high‐resolution transmission electron microscopy, X‐ray photoelectron spectroscopy, and energy dispersive spectroscopy are used to characterize their phase, shape, lattice structure, composition, and element distribution. The data suggest that Eu3+ ions are uniformly embedded into SnO2 nanocrystallites either through substitution of Sn4+ ions or through formation of Eu‐F bonds, allowing for high‐level Eu3+ doping. Photoluminescence features such as transition intensity ratios and Stark splitting indicate diverse localization of Eu3+ ions in the SnO2 nanoparticles, either in the crystalline lattice or in the grain boundaries. Due to formation of Eu‐F and Sn‐F bonds, the fluorinated surface of SnO2 nanocrystallites efficiently inhibits the hydroxyl quenching effect, which accounts for their improved photoluminescence intensity.  相似文献   

4.
We have prepared polycrystalline Ca3−xEuxCo4O9+δ (x=0, 0.15, 0.3 and 0.45) samples using a sol-gel process followed by SPS sintering and investigated the Eu substitution effects on their high-temperature thermoelectric properties. With the Eu substitution, both the electrical resistivity and thermopower increase monotonously. This could be attributed to the decrease of hole concentrations by substitution of trivalent Eu3+ for divalent Ca2+. The Eu substituted samples (x=0.15, x=0.3) have lower thermal conductivity than Ca3Co4O9+δ due to their lower electronic and lattice thermal conductivity. The dimensionless figure of merit ZT reaches 0.3 at 1000 K for the sample of Ca2.7Eu0.3Co4O9+δ.  相似文献   

5.
The VUV-Vis spectroscopic properties of barium borophosphate BaBPO5 doped with lanthanide ions are investigated. The host absorption band is found to be around 150-160 nm, the charge transfer band of Eu3+ is observed at about 264 nm, the f-d transitions of Ce3+, Eu2+, and Tb3+ in the host lattice are depicted. The partial reduction of Eu3+ in air atmosphere is reported.  相似文献   

6.
A series of yellow-green (Sr, Ca)3B2O6:Eu phosphors have been synthesized using precursors prepared via a facile sol-gel route. The solid-solution phases crystallized to materials with the formula of Sr3−xyCaxEuyB2O6 with varied Ca2+ and Eu2+ contents. The emission peak centered at 540 nm under near-UV excitation exhibited a broad-band distribution in the range of 450-650 nm. The dependences of the luminescence intensity on the contents of Ca2+ substitution and Eu2+ dopant were also investigated. The composition in the host lattice sensitively affected the chromaticity index. Sr1.21Ca1.7Eu0.09B2O6 (SCB:0.09Eu) was shown to possess the highest intensity and broadest emission band. Calcining temperature was shown to greatly influence the luminescent properties of SCB:0.09Eu. It is concluded that SCB:0.09Eu can be used as an efficient yellow-green phosphor for white light-emitting diodes (white LEDs) applications.  相似文献   

7.
胡元  夏海平  张丽 《光子学报》2014,40(11):1646-1651
采用新型超声喷雾共沉淀法技术,以Lu2O3、Eu2O3、Al(NO3)3·9H2O为原料,制备了不同浓度Eu3+离子掺杂的Lu3Al5O12纳米粉体.用X射线粉末衍射表征了获得纳米粉体的相,用扫描电镜观察了纳米粒子的形貌.测定了粉体的激发光谱、7F0-5D2声子边带谱与发射光谱.研究了不同高温烧结温度与Eu3+掺杂浓度对纳米粒子的发光强度与粒子形貌的影响规律.研究表明,当烧结温度高于900 ℃时,粉体发光强度明显增强,并且随着煅烧温度的增加,发光强度有所增强.Eu3+离子的最佳掺杂浓度为5~7 mol%.根据稀土离子Eu3+光学跃起矩阵元的特点,从发射光谱获得Eu3+光学跃起的J-O参量Ω2与Ω4.在Eu3+掺杂浓度均为5 mol%时,其强度参量达最小,电-声子耦合最强.然后随着掺杂浓度的进一步提高,强度参量略有增加,电-声子耦合减弱.说明Eu-O键强增加,共价性增强,Eu3+的局域环境对称性降低.Ω2值低于Eu3+在玻璃与晶体基质中的情况,这是由于纳米粒子中存在着大量的缺陷以及晶体的结构畸变导致纳米粒子的对称性下降所致.  相似文献   

8.
X-ray diffraction pattern of solvated Eu(fod)3(H2O)1,5(i-PrOH)0,5 form of Eu(fod)3 complex (fod=6,6,7,7,8,8,8-heptafluoro-2,2-dimethyl-3,5-octanedionate) is presented. The photoluminescence (PL) spectra of Eu3+ ions in polycrystalline powder Eu(fod)3 and also in Eu(fod)3-doped polymethylmethacrylate (PMMA), polypropylene (PP) and polydimethylsiloxane (PDMS) were investigated. It is revealed that the matrix influences the temperature quenching of PL intensity in the range 20-100 °C. A polycrystalline powder Eu(fod)3 and Eu(fod)3-doped PP are the most effective materials for PL quenching. It is shown that water molecules in the first coordinating sphere of Eu3+ ions increase PL intensity temperature quenching.  相似文献   

9.
Eu3+ doped ZnO nanoparticles are known to have significance extent of surface Eu3+ ions due to a large difference in ionic radii. Effect of such Eu3+ ions on the luminescence properties of ZnO:Eu nanoparticles has been understood from the luminescence studies of ZnO:Eu nanoparticles covered with Y2O3 shell. Based on the asymmetric ratio of luminescence and extent of energy transfer, it is established that when ZnO:Eu nanoparticles are covered with Y2O3 shell, a part of Eu3+ ions present with ZnO:Eu core migrate to Y2O3 shell and occupy Y3+ lattice positions.  相似文献   

10.
The paper is devoted to investigation of the processes of excitation energy transfer between the host cations (Tb3+ ions) and the activators (Ce3+ and Eu3+ ions) in single-crystalline films of Tb3Al5O12:Ce,Eu (TbAG:Ce,Eu) garnet which is considered as a promising luminescent material for the conversion of LED's radiation. The cascade process of excitation energy transfer is shown to be realized in TbAG:Ce,Eu: (i) from Tb3+ ions to Ce3+ and Eu3+ ions; (ii) from Ce3+ ions to Eu3+ ions by means of dipole-dipole interaction and through Tb3+ ion sublattice.  相似文献   

11.
Borate Ba3InB9O18 (BIBO) has been adopted as a host material for phosphors for the first time. Lanthanide ions (Eu3+/Tb3+)-doped BIBO phosphors have been synthesized by solid-state reaction and luminescent properties investigated under ultravoilet (UV) excitation. For red phosphor BIBO:Eu, dominant emission peaking at 590 nm was attributed to 5D07F1 transition of Eu3+, which confirmed that the local site of Eu3+ occupied by In3+ ion in BIBO crystal lattice is at inversion symmetry center. Optimum Eu3+ concentration of BIBO:Eu under UV excitation with 227 nm wavelength is around 40%. The green phosphor BIBO:Tb showed bright green emission at 550 with 232 nm light excited and optimal of Tb3+ concentration measured in BIBO is about 8%. The corresponding luminescence mechanisms of Ln-doped BIBO (Ln=Eu3+/Tb3+) were analyzed. The luminescent intensity of Tb3+ can be significantly improved by co-doping of Bi3+ in the BIBO:Tb lattice. The likely reason was proposed in terms of the different interactions of the host lattice with these ions, and of these ions with each other.  相似文献   

12.
Nanosized luminescent (Y,Bi)VO4:Eu3+ and Y(V,P)O4:Eu3+ were synthesized at low temperatures either by a coprecipitation method or by a hydrothermal method from aqueous solutions. The effect of Bi3+ ion or P5+ ion content in the lattice, annealing temperature effects on the crystal structure and the particle size, and the luminescence property of (Y,Bi)VO4:Eu3+ and Y(V,P)O4:Eu3+ nanoparticles were examined with a field-enhanced scanning electron microscopy, XRD, and a spectrofluorometer. The pristine YVO4:Eu3+, (Y,Bi)VO4:Eu3+, or Y(V,P)O4:Eu3+ nanoparticles are 35-50 nm in size. The luminescence spectrum of the Eu3+ ion was used to probe its position in the crystal lattice. The dopant ions enter the same lattice sites in the nanocrystalline as in the corresponding bulk material, resulting similar spectral features between them. Photoluminescence intensity is weak for the pristine nanoparticles. Annealing the nanoparticles at temperatures up to 1000 °C results in the increased luminescence intensity (>80% of micrometer-sized phosphors) with the minimal particle growth and the improved particle crystallinity.  相似文献   

13.
The strong vibronic one-phonon side-bands of the 5D07F0 emission of Eu3+ in {(C4H9)4N}3 EuxY1?x(NCS)6 are used to compute the Huang-Rhys electron-phonon coupling factor (S0) of Eu3+ with the mode at 35 cm-1. Increasing concentration from 1 to 100 is found to lead to a doubling of the electron-phonon coupling strength. Generalization of such an effect is proposed as a new hypothesis for part of the self-quenching process of rare-earth ions.  相似文献   

14.
Nanosized barium aluminate materials was doped by divalent cations (Ca2+, Sr2+) and Eu2+ having nominal compositions Ba1−xMxAl12O19:Eu (M=Ca and Sr) (x=0.1-0.5), were synthesized by the combustion method. These phosphors were characterized by XRD, scanning electron microscopy-energy-dispersive spectrometry (SEM-EDS) and photoluminescence measurement. The photoluminescence characterization showed the presence of Eu ion in divalent form which gave emission bands peaking at 444 nm for the 320 nm excitation (solid-state lighting excitation), while for 254 nm it gave the same emission wavelength of low intensity (1.5 times) compared to 320 nm excitation. It was also observed that alkaline earth metal (Ca2+ and Sr2+) dopants increase the intensity of Eu2+ ion in BaAl12O19 lattice, thus this phosphor may be useful for solid-state lighting.  相似文献   

15.
A series of rare earth ternary compounds of Tb1−xEux(TTA)3Dipy (HTTA=thenoyltrifluoroacetone, Dipy=2,2′-dipyridyl) have been synthesized, and the characteristics of the compounds have been performed by DTA-TG, IR, UV and fluorescence spectroscopy. Photoluminescence measurements indicated that the complexes of Eu(III) emit strong red luminescence under UV radiation. IR spectra suggest that complexes have been successfully synthesized, and TG curves indicate that the complexes are stable up to a temperature of about 220 °C. The Eu complex was blended with poly(N-vinylcarbazole) (PVK) and spin coated into films, and electroluminescence devices with the structure of Indium Tin Oxide (ITO)/PVK:Tb1−xEux(TTA)3Dipy/BCP(2,9-dimethyl-4,7-diphenyl-1,10-phenanthroline)/aluminum quinoline (AlQ)/Al were fabricated, the luminescence of Eu3+ complexes enhances after doping with Tb3+. Therefore, it may be an effective method to improve the EL intensity of the lanthanide complex.  相似文献   

16.
This work investigates the stability of Eu2+ and Eu3+ in some Sr-based inorganic compounds. Generally reducing condition is adopted in order to obtain Eu2+, however, the Eu doped SrAl2O4/SrLaAlO4 case indicates that for some compounds Eu3+ is stabilized even in reducing atmosphere. Bond valence method is applied to explain this phenomenon and it reveals that crystal structure also determines the valence state of europium cations along with reducing/oxidizing condition. An analysis of other Eu doped Sr-based materials is performed which shows the relationship between Eu2+/Eu3+ stability and the Global Instability Index (GII). This research provides a guideline for synthesizing specific novel Eu2+/Eu3+ phosphors.  相似文献   

17.
Green phosphor compositions MgxSr1−xAl2O4:Eu, Nd (with x=0.05-0.25) were prepared by solid state reaction method. The effect of Mg substitution on photoluminescence characteristics was investigated. The photoluminescence show intense green emission for MgSrAl2O4:Eu2+, Nd3+ with long persistence. This green emission corresponds to transitions from 4f65d1 to 4f7 of Eu2+ ion. Comparative analysis of the excitation and emission spectra were used to evaluate the crystal field splitting of the 5d states of Eu2+ and the parameters of electron-vibrational interaction, such as Huang-Rhys factor, effective phonon energy, and zero-phonon line position.  相似文献   

18.
Rare-earth-doped polycrystalline Ca3(PO4)2:Eu, Ca3(PO4)2:Dy and Ca3(PO4)2:Eu,Dy phosphors prepared by a modified solid-state synthesis has been studied for its X-ray diffraction, thermoluminescence (TL) and photoluminescence (PL) characteristics. The PL emission spectra of the phosphor suggest the presence of Eu3+ ion in Ca3(PO4)2:Eu and Dy3+ ion in Ca3(PO4)2:Dy lattice sites. The TL glow curve of the Ca3(PO4)2:Eu compounds has a simple structure with a prominent peak at 228 °C, while Ca3(PO4)2:Dy peaking at 146 and 230 °C. TL sensitivity of phosphors are compared with CaSO4: Dy and found 1.52 and 1.20 times less in Ca3(PO4)2:Eu and Ca3(PO4)2:Dy phosphors, respectively. The Ca3(PO4)2:Eu,Dy phosphors shows switching behavior under two different excitation wavelengths and enhancement in PL intensity of Dy3+ ions were reported. The paper discusses the photoluminescence and thermoluminescence behavior of Eu3+ and Dy3+ ion in Ca3(PO4)2 hosts, it may be applicable to solid-state lighting as well as thermoluminescence dosimetry applications.  相似文献   

19.
Eu2+–Mg2+ co-doped alon phosphors were successfully prepared by carbothermal reaction at 1600 °C for 2 h and their structure and photoluminescence properties were studied. The lattice parameter increased with increasing Eu concentration, indicating the incorporation of Eu into alon crystal lattice. The pure alon phase was obtained when Eu concentration is below 0.2%. Compared with solid state reaction process, this method lead to less amounts of secondary phase, larger amounts of Eu2+ against Eu3+, smaller particle size, narrower particle size distribution and stronger luminescence intensity. The absolute emission intensity of obtained phosphor reached 82% relative to that of famous BAM: Eu2+ phosphor. The emission could be tuned widely from blue to green by varying carbon content.  相似文献   

20.
The luminescence of Li2SrSiO4: 0.01Eu, xCe (x=0.0025, 0.005, 0.0075, and 0.01) is studied as a potential ultraviolet light-emitting diode (UV-LED) phosphor that is capable of converting the ultraviolet emission of a UV-LED into white light with good luminosity. There are broad blue and yellow emissions peaked at 413 and 575 nm, respectively. The two emissions come from d-f transitions of Ce3+ and Eu2+, respectively. The emission intensity of Li2SrSiO4: 0.01Eu, xCe reaches its maximum at x=0.0075. The energy transfer from Ce3+ to Eu2+ is demonstrated to be the type of electric dipole-dipole interaction with considerable spectral overlap and nonradiative transition is calculated to dominate. The Commission International de I’Eclairage (CIE) chromaticity coordinates of Ce3+/Eu2+ substituted compounds is also discussed.  相似文献   

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