Concentration dependence of the Ce3+ and Tb3+ luminescence of Ce1-xTbxMgAl11O19

The quenching of the Ce³⁺ emission and the increase of the Tb³⁺ emission with increasing x of Ce_1-xTb_xMgAl₁₁O₁₉ for x ? 0.35 is ascribed to energy transfer from Ce³⁺ to Tb³⁺, which is restricted to nearest rare earth neighbours. This transfer is almost complete at x ? 0.35. The decrease of the Tb³⁺ emission at higher Tb³⁺ concentrations is not due to Tb³⁺ concentrational quenching, but due to the limited solubility of Tb³⁺ in the CeMgAl₁₁O₁₉ phase.     

Luminescent properties of Tb activated GdTaO4 with M and M′ type structure under UV-VUV excitation

The photoluminescence of Tb³⁺ doped M and M′ type gadolinium orthotantalate Gd_1−xTb_xTaO₄ (0.01≤x≤0.20) was investigated under ultraviolet and vacuum ultraviolet excitation. For the samples of Gd_1−xTb_xTaO₄ with different crystallographic structures, emission spectra were the same in addition to intensity; the optimal concentration for Tb³⁺ was about 10 mol % in M type Gd_1−xTb_xTaO₄ but 5 mol % in M′ type Gd_1−xTb_xTaO₄. These differences could be corresponding with the difference in structures. In addition, compared to commercial Zn₂SiO₄: Mn²⁺, the integrated intensity of M and M′ type GdTaO₄: Tb³⁺ could reach 67% and 85%, respectively, of that at 147 nm excitation, which indicates that GdTaO₄: Tb³⁺ would be a promising vacuum ultraviolet phosphor for application in PDP and Hg-free lamp.     

The influence of crystal field split impurities (Tb) on the superconducting properties of LaAl2

The superconducting transition temperatures of the system La_1-xTbxAl₂ have been measured. By making use of the theory of Keller and Fulde the energy splitting between the ground state and the first excited state of Tb³⁺ is found to be 5 ± 1 K. Furthermore, we have determined the upper critical field H_c2(T) of these alloys and compared the results with those found for La_1-xGd_xAl₂. In this way the influence of the crystal field splitting of Tb³⁺ on the critical field data is clearly demonstrated.     

Cathodoluminescence properties of Tb3+-doped Na3YSi2O7 phosphors

Tb³⁺-doped Na₃YSi₂O₇ phosphors were prepared by the sol–gel method and then characterized by X-ray diffraction (XRD), field-emission scanning electron microscopy, and cathodoluminescence spectroscopy. The XRD results reveal that the Tb³⁺ ions have been introduced as dopants into the Na₃YSi₂O₇ host lattice. Under low-voltage electron beam excitation, the phosphors exhibit the characteristic emissions of Tb³⁺ (⁵ D _3,4→⁷ F _J , J=3–6 transitions). The luminescence color of the phosphors can be tuned from greenish-blue to bluish-green and to green by controlling the Tb³⁺ concentration within the 0.0005–0.15 (x value). The optimum Tb³⁺ doping concentration is 10 mol%, and the “dead voltage” is approximately 1.35 kV. All results indicate that the sample is a phosphor candidate for field-emission displays.     

Photoluminescence and decay behavior of Tb3+ ions in sodium fluoro-borate glasses for display devices

We report the optical absorption, photoluminescence and fluorescence decay properties of Tb³⁺-doped sodium fluoro-borate (SFB) glasses. Different concentrations of Tb³⁺-doped SFB glasses were prepared by conventional melt quenching technique using a chemical composition (in mol%) 25Na₂O–5LaF₃–10CaF₂–10AlF₃–(50?x) B₂O₃?x TbF₃ (0.01≤x≥4). The Judd-Ofelt model has been adopted to determine the radiative parameters of the ⁵D₄→⁷F_6–3 emission transitions. The effect of Tb³⁺ ion concentration on the emission from the ⁵D_3,4 excited levels is discussed in detail. The analysis of optimization of Tb³⁺ ion concentration for efficient green color display devises is reported. The resonance energy transfer mechanism responsible for non-radiative decay rates is clearly explored.     

Neutron spectroscopy of 0.6 meV crystal field transitions in doped superconductors

Transitions between the low lying crystal field states of Tb³⁺ and Pr³⁺ substituted for La in the superconductors LaAl₂, LaAg, and LaSn₃ have been observed by inelastic neutron scattering. Level separations of less than 1 meV and linewidths could be measured for concentrations as small as 2 mole %.     

Energy transfer mechanisms in the KCaLa1−x−yCexTby(PO4)2 phases

The various mechanisms involved in the green emission of KCaLa_1?x?yCe_xTb_y(PO₄)₂ under UV excitation are analyzed for a weak terbium concentration (y = 0.05). Ce³⁺ → Tb³⁺ transfer can be described by the Dexter model, but only for a weak cerium concentration. For higher cerium contents the cerium lifetime temperature dependence can be fitted by using a model involving energy migration between Ce³⁺ ions before Ce³⁺ → Tb³⁺ transfer. The investigation of the variation of the terbium emission vs temperature involves the presence of energy-trapping defects in the material.     

Control of luminescence and conductivity of delafossite-type CuYO2 by substitution of rare earth cation (Eu, Tb) and/or Ca cation for Y cation

Delafossite-type oxides of CuTb_yY_1−yO₂, CuEu_yY_1−yO₂, CuCa_xTb_yY_1−x−yO₂ and CuCa_xEu_yY_1−x−yO₂ have been prepared by solid state reactions. The lattice-parameter dependence on the composition implies substitution of the Tb³⁺, Eu³⁺ and Ca²⁺ cations for the Y³⁺ site. Noticeable sharp emission lines due to the f-f transitions (⁵D₄→⁷F_J, J=3-6) of Tb³⁺ or due to the f-f transitions (⁵D₀→⁷F_J, J=0-4) of Eu³⁺ are observed at room temperature. Electrical conductivities of CuCa_xTb_yY_1−x−yO₂ and CuCa_xEu_yY_1−x−yO₂ are larger than those of CuTb_yY_1−yO₂ and CuEu_yY_1−yO₂, indicating the increase of the hole concentration caused by the substitution of Ca²⁺ for the Y³⁺ site. These results indicate the controllability of the luminescence and conductivity in CuCa_xTb_yY_1−x−yO₂ and CuCa_xEu_yY_1−x−yO₂ delafossite-type oxides by simultaneous substitution of the rare earth Tb³⁺ or Eu³⁺ cation and the Ca²⁺ cation for the Y³⁺ site.     

Luminescence enhancement by energy transfer from Ce ions in Ba1.6Ca0.4P2O7:Ce:Tb phosphor

The optical properties of Ba_1.6Ca_0.4P₂O₇ doped with Ce³⁺ and Tb³⁺ are investigated. Under excitation at 280 nm the emission spectrum of Ba_1.6Ca_0.4P₂O₇:Ce³⁺ consists of a peak at 370 nm and a shoulder at the longer wavelength side. The emission spectra of Ba_1.6Ca_0.4P₂O₇:Tb³⁺ shows the well-known emission lines due to ⁵D₄-⁷F_J transitions of Tb³⁺. The green emissions of Tb³⁺ ions are enhanced upon UV excitation through energy transfer from Ce³⁺ to Tb³⁺ ions. The efficiency of such an energy transfer is estimated based on spectroscopic data. The dependence of photoluminescence (PL) intensities of Ce³⁺ and Tb³⁺ emissions on Ce³⁺ or Tb³⁺ concentrations in the systems (Ba_1.6Ca_0.4P₂O₇:0.04Ce³⁺,xTb³⁺ and Ba_1.6Ca_0.4P₂O₇:xCe³⁺,0.04Tb³⁺) and the temperature dependence of PL emission spectra of Ba_1.6Ca_0.4P₂O₇:0.06Ce³⁺,0.04Tb³⁺ is also investigated.     

The effect of pressure on the crystalline electric field levels of superconducting La1−xTbxAl2

The pressure dependence of the superconducting transition temperature (dT_c/dP) is smaller for La_1?xTb_xAl₂ than for LaAl₂. The difference is attributed to an increase with pressure of the crystalline electric field energies experienced by the Tb ion.     

Photoluminescence properties and effects of dopant concentration in Bi2ZnB2O7:Tb phosphor

A novel green phosphor, Tb³⁺ doped Bi₂ZnB₂O₇ was synthesized by conventional solid state reaction method. The phase of synthesized materials was determined using the XRD, DTA/TG and FTIR. The photoluminescence characteristics were investigated using spectrofluorometer at room temperature. Bi₂ZnB₂O₇:Tb³⁺ phosphors excited by 270 nm and 485 nm wavelengths. The emission spectra were composed of three bands, in which the dominated emission of green luminescence Bi₂ZnB₂O₇:Tb³⁺ attributed to the transition ⁵D₄ → ⁷F₅ is centered at 546 nm. The dependence of the emission intensity on the Tb³⁺ concentration for the Bi_2−xTb_xZnB₂O₇ (0.01 ≤ x ≤ 0.15) was studied and observed that the optimum concentration of Tb³⁺ in phosphor was 13 mol% for the highest emission intensity at 546 nm.     

Fluorescence enhancement of oxide fluoride glass co-doped with TbF3 and SmF3

The fluorescence property of xTbF₃-BaF₂-AlF₃-GeO₂+ySmF₃ (x=0.01-40 mol%, y=0-5 wt%) glasses were investigated. The enhancement of Sm³⁺ fluorescence was recognized in the presence of Tb³⁺. Increasing Tb³⁺ content, the emission color changed from green to orange. When the intensity of fluorescence at 540 nm originated from Tb³⁺ is compared with that at 600 nm originated from Sm³⁺, the information about the concentration quenching of Tb³⁺ and Sm³⁺ was obtained. From these results, rare earth ions were dispersed identically in the glasses. After heating to 673 K or cooling to 77 K, the emission color of 20TbF₃-20BaF₂-10AlF₃-50GeO₂/mol%+0.05 wt% SmF₃ glass was reversibly changed from orange to green. In addition, while the emission from 10TbF₃-20BaF₂-10AlF₃-60GeO₂+0.01 wt% SmF₃ glass was green, its crystallized sample, prepared by annealing at 1073 K, exhibited an orange emission due to Sm³⁺ at room temperature.     

Middle infrared luminescence of Tb in silver halide crystals and fibers

The optical absorption and the luminescence emission were investigated in AgCl_xBr_1−x crystals (0<x<1) doped with Tb³⁺ ions and in fibers extruded from these crystals. Strong luminescence emission in the middle infrared (MIR) in the spectral range 4.2-5.6 μm was observed for the first time in such crystals and fibers.¹ Various optical parameters were calculated for the Tb³⁺-doped crystals, using the Judd-Ofelt approximation. The measured and the calculated results have indicated that these doped crystals could be used for the development of solid-state lasers or fiber lasers operating in the middle infrared.     

Spin-glass like behaviors in La<Subscript>1−<Emphasis Type="Italic">x</Emphasis></Subscript>Tb<Subscript><Emphasis Type="Italic">x</Emphasis></Subscript>MnO<Subscript>3</Subscript> perovskite

A series of samples of La_1−x Tb _x MnO₃ (0⩽x⩽0.15) are prepared. The static and dynamic magnetizations of La_1−x Tb _x MnO₃ have been investigated. The results indicate that the spins with the short-range order are frozen into random direction at low enough temperatures which leads to the samples exhibiting the spin-glass like behavior. It is considered that the spin-glass like behavior originates from the competition between ferromagnetic double exchange among Mn³⁺ and Mn²⁺ and antiferromagnetic superexchange among Mn³⁺ and Mn³⁺, as well as Tb³⁺ and Tb³⁺.     

VUV-UV luminescence of magnetoplumbite: (Sr0.96−xBa0.04)Al12−yMgyO19:Tbx

The title compounds (Sr_0.96−xBa_0.04)Al_12−yMg_yO₁₉:Tb_x (0<x<0.4; 0<y<0.18) are single-phase magnetoplumbite determined by X-ray powder diffraction analysis. The characteristic emission lines of ⁵D₃→⁷F_j (j=2, 3, 4, 5) and ⁵D₄→⁷F_j (j=4, 5, 6) of Tb³⁺ are recorded under the VUV excitation. The intensive luminescence mainly comes from ⁵D₃→⁷F_j transition when the concentration of Tb³⁺ is low. However, when the concentration of Tb³⁺ starts to increase from very low concentration, ⁵D₄→⁷F_j transition is becoming dominant. Three broad excitation bands at 165, 193 and 233 nm have been observed. The band at 165 nm originates from the overlap between the host absorption and the charge transfer of Tb³⁺-O²⁻. The other two broad bands are the first spin-allowed and the spin-forbidden of 4f-5d transition, respectively. The experimental observation of the 4f-5d transition of Tb³⁺ is consistent well with the theoretical expectations.     

Ca₂BO₃Cl:Ce³⁺,Tb³⁺:A novel tunable emitting phosphor for white light-emitting diode

<正>Ca₂BO₃Cl:Ce³⁺,Ca₂BO₃Cl:Tb³⁺,and Ca₂BO₃Cl:Ce³⁺,Tb³⁺ phosphors are synthesized by a high temperature solid-state reaction.The emission intensity of Ce³⁺ or Tb³⁺ in Ca₂BO₃Cl is influenced by the Ce³⁺ or Tb³⁺ doping content,and the optimum concentrations of Ce³⁺ and Tb³⁺ are 0.03 mol and 0.05 mol,respectively.The concentration quenching effect of Ce³⁺ or Tb³⁺ in Ca₂BO₃Cl occurs,and the concentration quenching mechanism is d-d interaction for either Ce³⁺ or Tb³⁺.The Ca₂BO₃Cl:Ce³⁺,Tb³⁺ can produce colour emission from blue to green by properly tuning the relative ratio between Ce³⁺ and Tb³⁺,and the emission intensity of Tb³⁺ in Ca₂BO₃Cl can be enhanced by the energy transfer from Ce³⁺ to Tb³⁺.The results indicate that Ca₂BO₃Cl:Ce³⁺,Tb³⁺ may be a promising double emission phosphor for UV-based white light emitting diodes.     

Superconductivity and ferromagnetism in the orthorhombic system (TbxLu1−x)RuB2

The pseudoternary orthorhombic system Tb_xLu_1?xRuB₂) (0 ? x ? 0.1 andx = 1.0) has been investigated by static magnetization, ac susceptibility and resistivity measurements down to 1.5 K. Superconductivity occurs for 0 ? x ? 0.1, while ferromagnetic order occurs for x = 1.0. For each sample studied, the Tb ion maintains a configurationally stable trivalent state. The initial linear depression of the superconducting transition temperature yields a coupling constant value N(0)Γ² between conduction electrons and magnetic Tb³⁺ moments of 3.5 x 10^-4 ev-atom-states/spin-direction.     

A verification of the occurrence of the downconversion effect (transformation of a quantum of VUV radiation into two photons of luminescence in the visible range) in KGd2F7 and K2GdF5 crystals doped with Tb3+ ions

In order to verify whether the downconversion mechanism can occur in KGd₂F₇ and K₂GdF₅ crystals, which contain different concentrations of Tb³⁺ ions, we have investigated the emission and luminescence-excitation spectra of these crystals. Our experimental results have not shown the occurrence of the downconversion effect in the examined crystals, since the rate of nonradiative relaxation from upper 4f5d levels to lower-lying 4f5d- and 4f levels of the Tb³⁺ ion is likely to exceed the rate of possible cross relaxation from these high-lying 4f5d levels with energy transfer to neighboring Tb³⁺ ions.     

Luminescence properties of Ceand Tb ions codoped strontium borate phosphate phosphors

The Ce³⁺-activated, Tb³⁺-activated, and Ce³⁺ and Tb³⁺ co-activated phosphors 2SrO-nB₂O₃-(1−n)P₂O₅ were synthesized by the solid-state reaction. The structures, photoluminescent spectra and dynamics of them were systemically studied. The results demonstrate that the structure of the samples with n=0.10-0.50 belongs to the hexagonal phase. When n is beyond this range, the structures are the mixed phases of α-Sr₂P₂O₇ and Sr₂B₂O₅. The optimum composition is determined to be n=0.25 for the 2SrO-nB₂O₃-(1−n)P₂O₅ phosphors. As n varies from 0.01 to 0.50, the lifetime of Ce³⁺ ion increases gradually, while the lifetime of Tb³⁺ ion decreases, indicating that the energy transfer efficiency decreases with the increase of n. The ET efficiency between Ce³⁺ and Tb³⁺ in the optimum composition reaches to 70%. The present results demonstrate that the Ce³⁺ and Tb³⁺ co-activated hexagonal 2SrO-0.25B₂O₃-0.75P₂O₅ powders can possibly be applied as the newly developed green efficient phosphors in the field of lighting and display.     

Highly efficient cooperative energy transfer from Ho3+ and Tm3+ ions to Ce3+ ions in crystals

A phenomenon of highly efficient cooperative energy transfer from Ho³⁺ and Tm³⁺ ions to two-particle (2Ce³⁺) cooperative acceptors in crystals of solid solutions of La_1?x Ce _x F₃ is revealed. The rates of cooperative energy transfer in Ho³⁺→2Ce³⁺, Tm³⁺→2Ce³⁺, and Tb³⁺→ 2Yb³⁺ systems are measured, as well as their dependence on the magnitude of the matrix elements of donor transition.