Intermolecular energy transfer from UO2+2 to Eu3+ in solutions

The quenching constants for the UO²⁺₂ ion fluorescence by the Eu³⁺ ion in H₂O, D₂O, potassium formate and acetic acid media were determined by measuring the decrease in intensity of the 5050 Å fluorescence peak and the lifetime of the UO²⁺₂ ion fluorescence. The energy transferred to the Eu³⁺ ion was found to be a small fraction of the energy lost by the UO²⁺₂ ion by the non-radiative processes. The variations of the quenching constants of the UO²⁺₂ ion and the fluorescence lifetimes were determined for different concentrations of potassium formate and acetic acid. These results indicate that the UO²⁺₂ ion forms inner sphere complexes with the two ligands mentioned.     

Synthesis, structure and optical properties of Eu/TiO2 nanocrystals at room temperature

The nanocrystal samples of titanium dioxide doped with europium ion (Eu³⁺/TiO₂ nanocrystal) are synthesized by the sol-gel method with hydrothermal treatment. The Eu³⁺ contents (molar ratio) in the samples are 0, 0.5%, 1%, 2%, 3% and 4%. The X-ray diffraction, UV-Vis spectroscopy data and scanning electron microscope image show that crystallite size is reduced by the doping of Eu³⁺ into TiO₂. Comparing the Raman spectra of TiO₂ with Eu³⁺/TiO₂ (molar ratio Eu³⁺/TiO₂=1%, 2% and 4%) nanocrystals at different annealing temperatures indicates that the anatase-to-rutile phase transformation temperatures of Eu³⁺/TiO₂ nanocrystals are higher than that of TiO₂. This is due to the formation of Eu-O-Ti bonds on the surface of the TiO₂ crystallite, as characterized by the X-ray photoelectron spectroscopy. The photoluminescence spectra of TiO₂ in Eu³⁺/TiO₂ nanocrystals are interpreted by the surface self-trapped and defect-trapped exciton relaxation. The photoluminescence of Eu³⁺ in Eu³⁺/TiO₂ nanocrystals has the strongest emission intensity at 2% of Eu³⁺ concentration.     

Influence of phase and morphology on thermal conductivity of alumina particle/silicone rubber composites

Eu²⁺- and Eu³⁺-Zn₂GeO₄ were prepared by the high temperature solid-state reaction method. The phase purity and crystallinity of Zn₂GeO₄:Eu samples were characterized by X-ray diffraction (XRD). The excitation spectra, the emission spectra and the luminescence decay curves of the Eu²⁺- and Eu³⁺-Zn₂GeO₄ were investigated. Zn₂GeO₄:Eu²⁺ gives a bluish-green luminescence with one emission band located at 467 nm, and Zn₂GeO₄:Eu³⁺ presents an reddish-orange color due to the transition (⁵D₀→⁷F_J, J = 1 and 2) of the Eu³⁺ ions. The luminescence decay curves of Eu²⁺ and Eu³⁺ provide complementary evidence to the mixed valence of europium (Eu²⁺, Eu³⁺) in Zn₂GeO₄ host. These indicate that the mixed valence of europium (Eu²⁺, Eu³⁺) coexists in Zn₂GeO₄ host prepared in an oxidizing atmosphere. The abnormal reduction phenomenon of Eu³⁺→Eu²⁺ in Zn₂GeO₄ host prepared in an oxidizing atmosphere was reported and discussed on the basis of the charge compensation model.     

白光LED用LiBaBO3:Eu2+材料发光特性研究

采用高温固相法制备了LiBaBO₃:Eu²⁺绿色发光材料.测量了Eu²⁺浓度为1mol%时样品的激发与发射光谱,其发射光谱为双峰宽谱,主峰分别为482和507nm,与理论计算值符合很好;监测482nm发射峰时,对应激发光谱的峰值为287和365nm,监测507nm发射峰时,对应的激发峰为365和405nm.研究了Eu²⁺浓度对材料发射光谱的影响,结果显示,随Eu²⁺浓度的增大,蓝、绿发射峰均发生了     

Photoluminescence and afterglow behavior of Eu, Dy and Eu, Dy in Sr3Al2O6 matrix

This paper reports the photoluminescence and afterglow behavior of Eu²⁺ and Eu³⁺ in Sr₃Al₂O₆ matrix co-doped with Dy³⁺. The samples containing Eu²⁺ and Eu³⁺ were prepared via solid-state reaction. X-ray diffraction (XRD), photo luminescent spectroscope (PLS) and thermal luminescent spectroscope (TLS) were employed to characterize the phosphors. The comparison between the emission spectra revealed that Sr₃Al₂O₆ phosphors doped with Eu²⁺, Dy³⁺ and Eu³⁺, Dy³⁺ showed different photoluminescence. The phosphor doped with Eu³⁺, Dy³⁺ showed an intrinsic f-f transition generated from Eu³⁺, with two significant emissions at 591 and 610 nm. However, the phosphor doped with Eu²⁺, Dy³⁺ revealed a broad d-f emission centering around 512 nm. After the UV source was turned off, Eu²⁺, Dy³⁺ activated Sr₃Al₂O₆ phosphor showed excellent afterglow while Eu³⁺, Dy³⁺ activated phosphor almost showed no afterglow. Thermal simulated luminescence study indicated that the persistent afterglow of Sr₃Al₂O₆: Eu²⁺, Dy³⁺ phosphor was generated by suitable electron traps formed by the co-doped rare-earth ions (Dy³⁺) within the host.     

Eu<Superscript>3+</Superscript> As a Luminescent Probe for Studying the Structure of R<Subscript>2</Subscript>O<Subscript>3</Subscript> Materials (R = Y,Eu, and Gd)

Spectra of Eu³⁺ in various dielectric matrices (Gd₂O₃:Eu³⁺, Y₂O₃:Eu³⁺, Eu₂O₃, and mSiO₂/Gd₂O₃:Eu³⁺ mesoporous particles) are studied by local cathodoluminescence. The results allowed identification of the local environment of Er³⁺ ions in amorphous samples and detection of the monoclinic Eu₂O₃ phase impurity in samples with yttrium oxide. The cathodoluminescence spectra of chemically pure Y₂O₃, Eu₂O₃, and Gd₂O₃ are recorded. Conclusions about the structural features of the materials are made and confirmed by other methods (XRD and EPMA).     

Synthesis and luminescence properties of Eu3+,Bi3+-doped BaWO4 phosphors

BaWO₄:Eu³⁺,Bi³⁺ phosphors have been prepared by the conventional high-temperature solid-state reaction and chemical precipitation. The materials were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), and photoluminescence (PL) technologies. When the phosphors are prepared by the high-temperature solidstate reaction, Bi³⁺ doping into BaWO₄:Eu³⁺ can increase the emission intensity of 613 nm. However, maximum emission at about 595 nm was observed in Eu³⁺,Bi³⁺-doped BaWO₄ phosphors prepared by the chemical precipitation. The decay constants (monitored at 595 and/or 613 nm) are within 45–100 s. The color purity of the Ba_0:865WO₄: Eu_0:11,Bi_0:025 phosphor (prepared by chemical precipitation) was 100%. The emission mechanism of Eu³⁺,Bi³⁺ in the BaWO₄ phosphors is briefly discussed.     

Combined Rietveld refinement of BaMgAl10O17:Eu using X-ray and neutron powder diffraction data

The phosphor, BaMgAl₁₀O₁₇:Eu²⁺, showing a blue emission band at about 450 nm was prepared by a normal solid-state reaction using BaCO₃, Al₂O₃, MgO and Eu₂O₃ as starting materials with AlF₃ as a flux. The study of combined Rietveld refinement and photoluminescence spectra was carried out to determine the structural parameters, such as lattice constants, the valence state of Eu, the site preference of Mg and site fractions of Mg and Eu. The occupancies of Eu and Mg were 0.022 and 0.526, respectively. The valence state of Eu was the divalent state because there was only one broad line at about 450 nm in the photoluminescence spectrum. The site preference of Mg atoms was the tetrahedral site of Al atoms surrounded by oxygen atoms in the spinel block. Lattice parameters decreased due to the difference of two ionic radii, Eu²⁺(1.09 Å) and Ba²⁺(1.34 Å), compared with those of BaMgAl₁₀O₁₇.     

Investigation on Eu doped Sr2MgSi2O7 red-emitting phosphors for white-light-emitting diodes

In this work, we report the high temperature solid-state synthesis of red phosphors Sr₂MgSi₂O₇: Eu³⁺ with various Eu³⁺ concentrations. Their luminescent properties at room temperature are investigated. The X-ray diffraction patterns indicate that the red phosphors powder conforms to the tetragonal Sr₂MgSi₂O₇. Impurity structure appears when more than 20% Eu³⁺ is doped. The samples show a strong emission line at 615 nm and the intensity increases with the increase of Eu³⁺ concentration until concentration quenching occurs. Charge compensation assists in the reduction of the impurity structure and vacancies; hence the luminescent intensity is enhanced. The decay measurement indicates that the lifetime of Eu³⁺ emission is about 2-3 ms. Some of the Eu³⁺ can be reduced to Eu²⁺; this is also discussed.     

Influence of nanoenvironment on luminescence of Euactivated SnO2 nanocrystals

The emission intensity of the peak at 612 nm (⁵D₀→⁷F₂) of the Eu³⁺ ions activated SnO₂ nanocrystals (doped and coated) is found to be sensitive to the nanoenvironment. We have compared the luminescence efficiencies of the nanocrystals of SnO₂ doped by Eu₂O₃ with those of SnO₂ coated by Eu₂O₃ and we found that the intensities are significantly higher in coated nanocrystals. Furthermore, it is clear from luminescence intensity measurements that Eu³⁺ ions occupy low symmetry sites in the Eu₂O₃ coated SnO₂ nanocrystal. The analysis suggests that the radiative relaxation rate is higher in Eu₂O₃ coated SnO₂ nanocrystals than Eu₂O₃ doped SnO₂ nanocrystals due to the asymmetric environment of Eu³⁺ ions in coated samples.     

A potential red phosphor LiGd(MoO4)2:Eu for light-emitting diode application

Eu³⁺-doped LiGd(MoO₄)₂ red phosphor was synthesized by solid-state reaction, and its photoluminescent properties were measured. The effect of Eu³⁺ doping concentration on PL intensity was investigated, and the optimum concentration of Eu³⁺ doped in LiGd(MoO₄)₂ was found to be 30 mol%. Compared with Y₂O₂S:0.05Eu³⁺, Na_0.5Gd_0.5MoO₄:Eu³⁺ and KGd(MoO₄)₂:Eu³⁺, the LiGd(MoO₄)₂:Eu³⁺ phosphor showed a stronger excitation band around 395 nm and a higher intensity red emission of Eu³⁺ under 395 nm light excitation. For the first time, intensive red light-emitting diodes (LEDs) were fabricated by combining phosphor and a 395 nm InGaN chip, confirming that the LiGd(MoO₄)₂:Eu³⁺ phosphor is a good candidate for LED applications.     

Energy transfer between Eu3+ ions in a lattice with two different crystallographic sites: Y2O3:Eu3+, Gd2O3:Eu3+ and Eu2O3

The Eu³⁺ ion occupies two different crystallographic sites in (Y_1−xEu_x)₂O₃ and (Gd_1−xEu_x)₂O₃, with site symmetry S₆ and C₂. Energy transfer over more than 7 Å occurs from Eu³⁺ (S₆) ions to Eu³⁺ (C₂) ions. This is shown to be a direct one-phonon assisted process, in combination with a one-site resonant two-phonon assisted process at higher temperatures. For x = 1 there is energy migration over the Eu³⁺ (C₂) sublattice to quenching impurities. The presence of cooperative absorption points to superexchange interaction between the Eu³⁺ ions.     

Luminescence and time-resolved spectroscopy properties of (Gd1−xEux)(BO2)3 multicrystals

(Gd_1?xEu_x)(BO₂)₃ (0≤x≤1) phosphors are synthesized by traditional high temperature solid state reaction. The photoluminescence (PL) properties of Gd(BO₂)₃ and Gd(BO₂)₃ activated with Eu³⁺ are investigated. The PL spectra exhibit the typical characteristic emission and excitation of Gd³⁺ and Eu³⁺ ions, and support the energy transfer taking place from Gd³⁺ to Eu³⁺ ions. The relationship between Eu³⁺ doping concentration and emission intensity is also studied. Even if all of the Gd³⁺ ions are substituted by Eu³⁺ ions, the concentration quenching between Eu³⁺ happens. However, the quenching is not complete. The luminescence decay curves are measured, and the lifetimes become short with the Eu³⁺ content increasing. The decreasing Gd³⁺ lifetimes also indicates that there exists efficient energy transfer between Gd³⁺ and Eu³⁺ ions.     

Abnormally enhanced Eu emission in Y2O2SO4:Eu inherited from their precursory dodecylsulfate-templated concentric-layered nanostructure

A new nanostructure-mediated approach was demonstrated to synthesize Eu³⁺-doped yttrium oxysulfates Y₂O₂SO₄:Eu³⁺ giving rise to abnormally enhanced Eu³⁺ emission. Yttrium and europium salts, sodium dodecylsulfate (SDS), and urea at various Eu³⁺ concentrations were reacted in aqueous solution at 80, 85, and 87 °C to yield Eu³⁺-doped dodecylsulfate-templated yttrium oxide mesophases with straight-layered (S-type), concentric-layered (C-type) and layer-to-hexagonal transient-layered (T-type) structures, respectively. On calcination at 1000 °C, all of these mesophases were converted into Y₂O₂SO₄:Eu³⁺ to exhibit luminescence bands including the ⁵D₀-⁷F₂ transition with a tendency in intensity to saturate or reach a maximum at 10-12 mol% Eu doping. The Eu³⁺ emissions for Y₂O₂SO₄:Eu³⁺ mediated by the T- and C-type mesophases were enhanced in intensity by a factor of about two and three times, respectively, stronger than those for not only compositionally the same sulfate Y₂O₂SO₄:Eu³⁺ obtained from yttrium-based sulfates but also Y₂O₃:Eu³⁺ obtained in the SDS-free system. In contrast, the emission intensities for the S-type-mesophase-mediated Y₂O₂SO₄:Eu³⁺ were close to those for the latter sulfates. The abnormally enhanced emission is likely based on specific deformation of sulfate groups induced through the conversion of concentric dodecylsulfate-layers to straight sulfate-layers in the oxysulfate framework upon calcination.     

Morphology and crystalline-phase-dependent luminescence of Li-doped Gd2O3:Eu3+ thin films grown by pulsed laser deposition

Gd₂O₃:Eu³⁺ and Li-doped Gd₂O₃:Eu³⁺ luminescent thin films have been grown on Si(100) substrates using pulsed laser deposition. The films grown at different deposition conditions show different crystalline and morphology structures and luminescent characteristics. Although both cubic and monoclinic crystalline structures were observed in both Gd₂O₃:Eu³⁺ and Li-doped Gd₂O₃:Eu³⁺ films, the cubic structure becomes more dominant for Li-doped Gd₂O₃:Eu³⁺ films. The photoluminescence brightness data obtained from Li-doped Gd₂O₃:Eu³⁺ films indicate that Si(100) is a promising substrate for growth of high-quality Li-doped Gd₂O₃:Eu³⁺ thin-film red phosphor. In particular, the incorporation of Li⁺ ions into the Gd₂O₃ lattice induced a change of crystallinity and enhanced surface roughness. Two major factors to determine photoluminescence brightness for Li-doped Gd₂O₃:Eu³⁺ films were crystalline phase and surface roughness. The highest emission intensity was observed with Gd_1.84Li_0.08Eu_0.08O₃, whose brightness was a factor of 2.1 larger than that of Gd₂O₃:Eu³⁺ films. This phosphor is promising for applications in flat-panel displays. PACS 78.20.-e; 78.55.-m; 78.66.-w     

Orange emission enhancement by energy transfer in Sr3Al2O5Cl2:Ce, Eu phosphor for solid-state lighting

Orange-emissive Ce³⁺/Eu²⁺ co-doped Sr₃Al₂O₅Cl₂ phosphors were synthesized by a solid-state reaction. The large overlap between the emission spectrum of blue Sr₃Al₂O₅Cl₂:Ce³⁺ and the excitation spectrum of orange Sr₃Al₂O₅Cl₂:Eu²⁺, and the shortening trend in lifetime of Ce³⁺ donors with increasing Eu²⁺ concentration in Sr₃Al₂O₅Cl₂:Ce³⁺, Eu²⁺ provide the strong evidence of energy transfer from Ce³⁺ to Eu²⁺ ions. It supports that the orange emission intensity of the optimal co-doped phosphor is 1.5 times stronger than that of single Eu²⁺-doped one. The Sr₃Al₂O₅Cl₂:Ce³⁺, Eu²⁺ phosphor is a promising orange-emitting phosphor for warm-white-light-emitting diode because of its effective excitation in the near ultraviolet range.     

Hydrothermal synthesis of Sb doped and (Sb, Eu) co-doped YBO3 with nearly white light luminescence

Sb³⁺-doped, Eu³⁺-doped and (Sb³⁺, Eu³⁺) co-doped YBO₃ crystals have been synthesized using Y₂O₃, B₂O₃, SbCl₃ and Eu₂O₃ as raw materials through a hydrothermal method. Phase-pure YBO₃ crystal with hexagonal flake shape has been synthesized at 473 K for 3 days. The photoluminescent property of YBO₃ with different activators were investigated using luminescent spectrometer at room temperature. The color of the (Sb³⁺, Eu³⁺) co-doped YBO₃ crystal could be controlled from blue to red by changing the Sb³⁺/Eu³⁺ ratio in the initial reactants. The nearly white emission could be obtained through changing the Sb³⁺/Eu³⁺ ratio in reaction.     

UV-induced photoluminescence and thermally stimulated luminescence of CaSO4:Eu and CaF2:Tb3+ phosphors

Ultraviolet radiation induced changes in photoluminescence (PL) and thermally stimulated luminescence (TSL) of europium activated calcium sulphate (CaSO₄:Eu³⁺, Eu²⁺) and terbium doped calcium fluoride (CaF₂:Tb³⁺) phosphors have been studied. PL measurements suggest conversion of Eu³⁺ to Eu²⁺ on 254 nm irradiation corresponding to charge transfer band of Eu³⁺ ions and reduction of Eu²⁺ ions with 365 nm illumination representing a f–d transition of Eu²⁺ ions. Similar studies carried out on CaF₂:Tb³⁺ phosphor, however, do not show any significant wavelength specific changes. The integrated TSL output appears to be rate-dependent for both phosphors. The wavelength dependent changes in TSL output observed for CaSO₄:Eu phosphor have been correlated with those obtained in PL studies. The changes in TSL and PL characteristics of CaF₂:Tb³⁺ phosphor have been explained on the basis of stabilisation of traps based on matrix specific charge similarities.     

Quadrupole interactions at europium sites in Eu3V2O7 and Eu2VO4

The electric-quadrupole interactions at the Eu sites in Eu₃V₂O₇ and Eu₂VO₄ oxides have been studied at room temperature with¹⁵¹Eu Mössbauer spectroscopy. Both divalent and trivalent Eu ions were found in the oxides. The fraction of Eu²⁺ is 17.1(8)% in Eu₃V₂O₇ and 39.0(1.6) % in Eu₂VO₄. The values of the quadrupole coupling constant, eV_zzQ_g, obtained from the fits using a full Hamiltonian method are ?6.594(50) and ?8.043(65) mm/s for Eu³⁺, and ?13.168(402) and ?18.032(134) mm/s for Eu²⁺, respectively in Eu₃V₂O₇ and Eu₂VO₄. The magnitude of eV_zzQ_g in Eu₂VO₄ is the largest ever reported for Eu²⁺ in any Eu oxide system.     

Stability of divalent/trivalent oxidation state of europium in some Sr-based inorganic compounds

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.