(Y,Gd)BO_3∶Eu~(3+)的结构和发光性质

采用高温固相反应合成了(Y,Gd)BO3∶Eu3+红色发光材料,确定了材料的最佳合成条件。该材料是以六面体晶体结构存在,空间群为P63/mm c(194)。红外光谱产生866 cm-1和912 cm-1的吸收峰,是由两种BO4的伸缩振动产生的,571 cm-1、621 cm-1、698 cm-1、711 cm-1峰是由BO4的弯曲振动引起的。发现了随Y/Gd比例的变化,Eu3+周围的局部对称性发生变化。Eu3+发光的红(5D0→7F2跃迁)橙(5D0→7F1跃迁)比随Y3+含量的增加而降低。     

Tb~(3+)掺杂ZnWO_4基绿色荧光粉的发光性能

以柠檬酸为螯合剂,采用沉淀法制备了稀土Tb3+掺杂的ZnWO4绿色荧光粉前驱体。通过差热分析(DTA)、热重分析(TG)、X射线衍射(XRD)等手段对产物进行了表征。结果表明,当退火温度低于700℃时,得到的样品为非晶态,而高于850℃退火处理后为单斜结构。使用荧光分光光度计研究了Tb3+在ZnWO4基质中的发光性质。结果显示,ZnWO4:Tb3+样品在544nm波长光的监测下于200~300nm处出现由W→O及Tb→O跃迁共同作用产生的重叠激发峰和系列Tb3+的f-f跃迁锐峰,其中位于488nm处的激发峰非常显著,对应于Tb3+的7F6→5D4跃迁。说明该法制备的荧光粉ZnWO4:Tb3+能够被蓝光有效激发,可以与广泛使用的蓝光LED芯片的输出波长相匹配。在488nm波长光的激发下观察到ZnWO4粉末中Tb3+的544nm(5D4→7F5)强的特征发射,说明ZnWO4:Tb3+粉末可作为白光LED的绿色补偿荧光粉。当以267nm激发ZnWO4:Tb3+时,有宽的WO2-4特征发射峰和Tb3+的5D4→7F6及5D4→7F5跃迁产生的发射峰,随着Tb3+掺杂浓度的增加,WO2-4的特征发射强度逐渐降低,而Tb3+的5D4→7F5跃迁强度增大,表明Tb3+与WO2-4之间有能量转移。     

用溶胶-凝胶法制备Y_2O_3-SiO_2:Tb~(3+)发光材料

采用溶胶-凝胶法制备了Y2O3-SiO2∶Tb3+发光材料。研究了Tb3+浓度、Y2O3和SiO2配比、烧结温度、烧结时间对发光强度的影响及其发光行为。     

Luminescence Properties of (Y, Gd)Al_3(BO_3)_4∶Eu ~(3 ) under VUV excitation

Thephosphorsasanimportantpartofplasmadis playpanel (PDP)deviceemitvisiblelightundervac uumultraviolet (VUV)excitationof 14 7nmand/or172nmfromXe/Hegasplasma[1] .Untilrecently ,Y2 O3∶Eu3 and (Y ,Gd)BO3∶Eu3 havebeenusedascommercialred emittingphosphorsforPDP[2 - 3] .Butthesematerialsstillhaveshortcomingstobeim proved :lowlightoutputofY2 O3∶Eu3 uponVUVex citationandbadcolorpurityof (Y ,Gd )BO3∶Eu3 [4～ 5] .AluminoborateshavestrongabsorptionintheVUVregion ,andexhibitexcellentma…     

溶胶-凝胶法制备Y_2Zr_2O_7:Tm~(3+)及其发光性能研究

以柠檬酸为络合剂采用溶胶-凝胶法制备了(Y1-xTmx)2Zr2O7(x=0.005,0.01,0.03,0.05)荧光粉.采用X-射线衍射分析仪(XRD)、扫描电子显微镜(SEM)和荧光光谱仪分别检测了Y2Zr2O7∶Tm3+的晶体结构、颗粒形貌以及样品的荧光光谱.XRD图谱表明,所得到的产物Y2Zr2O7∶Tm3+为单一相的萤石结构,而且Tm3+的掺杂并没有改变其晶体结构.荧光光谱的测试表明,在359 nm波长的紫外光激发下,1000℃下烧结的(Y1-xTmx)2Zr2O7(x=0.01)样品的发光性能最好,发射峰对应于Tm3+的1D2→3F4跃迁和1G4→3H6跃迁,并对其发光机理进行了探讨.样品在454nm处的发光强度随Tm3+离子掺杂浓度的增加先升高后降低,即出现了浓度猝灭的现象,当Tm3+掺杂浓度摩尔百分比为1%时,样品的发光强度达到最大.     

溶胶-凝胶法制备Y2Zr2O7∶Tm3+及其发光性能研究

以柠檬酸为络合剂采用溶胶-凝胶法制备了（Y1-xTmx）2Zr2O7（x=0.005,0.01,0.03,0.05）荧光粉.采用X-射线衍射分析仪（XRD）、扫描电子显微镜（SEM）和荧光光谱仪分别检测了Y2Zr2O7∶Tm3+的晶体结构、颗粒形貌以及样品的荧光光谱.XRD图谱表明,所得到的产物Y2Zr2O7∶Tm3+为单一相的萤石结构,而且Tm3+的掺杂并没有改变其晶体结构.荧光光谱的测试表明,在359 nm波长的紫外光激发下,1000℃下烧结的（Y1-xTmx）2Zr2O7（x=0.01）样品的发光性能最好,发射峰对应于Tm3+的1D2→3F4跃迁和1G4→3H6跃迁,并对其发光机理进行了探讨.样品在454 nm处的发光强度随Tm3+离子掺杂浓度的增加先升高后降低,即出现了浓度猝灭的现象,当Tm3+掺杂浓度摩尔百分比为1%时,样品的发光强度达到最大.     

红色荧光粉NaBaPO_4:Eu~(3+)的制备及其性能研究

采用高温固相法制备单一六方晶系红色荧光粉NaBaPO4:Eu3+。利用XRD、SEM和荧光光谱等对NaBaPO4:Eu3+粉末的理化特性进行表征,考察了激活剂Eu3+的浓度和助熔剂NH4F用量对粉末的晶体结构和发光性能的影响。结果表明:激活剂Eu3+最大掺入量为20%,助熔剂NH4F的最大掺入量为10%,采用该配比合成得到的荧光粉NaBa0.8PO4具有最好的发光性能。在最强激发波长的近紫外光(≈393nm)激发下,样品发射强的红光(≈613nm)和橙光(≈591nm)。     

H_3BO_3添加量对CaTiO_3∶Pr~(3+)余辉性能的影响

采用高温固相法合成CaTiO3∶Pr3+,并通过掺杂H3BO3改性。研究样品的发射光谱、发光亮度及余辉时间,探讨H3BO3添加量对CaTiO3∶Pr3+发光强度及余辉性能的影响。结果表明,所添加H3BO3的摩尔分数为15%时,CaTiO3∶Pr3+粉末具有最佳的余辉性能。     

绿色荧光粉Na_(1-x)Li_xCaPO_4:0.02Eu~(2+)的制备及其性能的研究

采用高温固相反应法制备了稀土掺杂荧光粉NaCa0.98PO4:Eu2+0.02,在波长360nm激发光激发下,荧光粉发射波长在500nm左右的绿光。采用Li+为掺杂离子取代基质晶格中的Na+位,通过杂质离子掺杂量对发光性能影响的研究,获得Li+的最佳掺杂量为5mol%。在波长为360mm近紫外光激发下,Na0.95Li0.05Ca0.98PO4:0.02Eu2+的发射强度是NaCa0.98PO4:Eu0.022+的2.5倍,该荧光粉为适用于近紫外激发的白光LED的绿色荧光粉。     

Tb~(3+)掺杂BiPO_4基绿色荧光粉的共沉淀法合成及发光性质

以(NH4)2HPO4为沉淀剂,采用共沉淀法合成Tb3+掺杂BiPO4基绿色荧光粉。通过DTA-TG、XRD、IR等方法对荧光粉的结构、组成进行了表征。结果表明,在室温条件下得到了纯六方相BiPO4∶Tb3+,当退火温度为400℃时,开始出现单斜相,温度升高到600℃以上时晶相转变为纯单斜相BiPO4∶Tb3+。利用激发光谱和发射光谱研究了Tb3+在BiPO4基质中的发光性能,六方相和单斜相BiPO4∶Tb3+样品均可发光,在紫外光377 nm紫外光的激发下测定的六方相和单斜相BiPO4∶Tb3+发射光谱的峰位相同,主要发射峰出现在544 nm处强的5D4→7F5跃迁和490 nm、590 nm、622 nm处弱的5D4→7F6、5D4→7F4、5D4→7F3跃迁。当BiPO4∶Tb3+为单斜相时Tb3+在BiPO4基质中的发光强度明显强于六方相BiPO4∶Tb3+。     

Red Emitting Phosphor (Y,Gd)BO3:Eu3+ for PDP Prepared by Complex Method

Red phosphor (Y, Gd)BO3:Eu3+ with grain shape, small size, non-agglomerate, high crystallinity and good photoluminescence (PL) intensity was prepared by a complex method that the precursor of the phosphor was prepared by co-precipitation method and the phosphor was prepared by combustion method. The SEM photos and the photoluminescence spectrum excited under VUV show that the morphology and luminescent properties of this phosphor are satisfied when an appropriate amount of urea was adopted as the combustion agent in the preparation procedure.     

New red phosphor （Y, Gd, Lu）BO3： Eu^3＋ for PDP applications

Highly efficient phosphors under vacuum ultraviolet excitation are still demanded for the development of plasma display panels and Hg-free fluorescent lamps. The phosphors of Eu3+ doped (Y, Gd, Lu)BO3 were synthesized with solid state reaction method and the con-tents of Y3+, Gd3+, and Lu3+ for plasma display panel red phosphor were optimized under vacuum ultraviolet excitation. Two new potential candidates, which were (Y1-S-7TGdSLuT)BO3: Eu3+ (0相似文献   

Synthesis of Spherical (Y,Gd)BO3∶Eu3+ Phosphor Using W/O Emulsion System

Spherical (Y, Gd)BO3:Eu3 phosphor particles with a narrow size distribution(2～4 μm) was obtained by firing the Y-Gd-Eu-BO3 precursor prepared in a W/O style emulsion system. In the W/O emulsion system, kerosene, used as oil phase, was mixed with Span 80 and Tween 80 compounds which were employed as the emulsifier with an HLB (hydrophile-lipophile balance) value of 5.2～5.3. Both rare earths (Y, Gd and Eu) nitrate and boric acid solution or ammonia solution were used as aqueous phase. The synthesis conditions, such as emulsion composition, emulsifying style, precipitation reaction process, reaction temperature, morphology control, and so on, were investigated, and the optimum synthesis conditions for preparing spherical (Y, Gd)BO3∶Eu3 phosphor was obtained. The phosphor was characterized by XRD, SEM, laser particle size analysis, emission and excitation spectrum under vacuum ultraviolet (VUV), and so on. The phosphor synthesized using the water-in-oil emulsion method with median diameter (D50) of 2～4 μm shows agreeable photoluminescence (PL) property and sphericity. The main emission peak appears at about 593 nm, which corresponds to 5D0→7F1 transition (magnetic-dipole transition) of the Eu3 ion. The cell parameters and powder diffraction data were indexed. The structure of the phosphor belongs to the hexagonal system with space group P63/m.     

Effect of Li+ ions doping on structure and luminescence of (Y,Gd)BO3:Tb3+

The (Y,Gd)BO3:Tb3+ and Li+-doped (Y,Gd)BO3:Tb3+ phosphors were prepared by high temperature solid-state method. The inductively coupled plasma atomic emission spectrometry (ICP-AES), X-ray diffraction (XRD), scanning electron microscopy (SEM), and the excitation and emission spectra were used to characterize the samples. The results of ICP-AES and XRD indicated that Li+ ions could enter the (Y,Gd)BO3:Tb3+ lattice and induce the lattice expansion. It could be seen from SEM that the particles were spherical a...     

Co-Precipitation Preparation and Luminescent Behavior of (Y,Gd)BO3∶ Eu Phosphor

(Y,Gd)BO3∶ Eu phosphors were prepared by co-precipitation precursors, and luminescent properties were investigated. The precursors were synthesized by introducing hydroxyl ion to mixed solution of rare earth nitrates and boric acid, either through adding ammonia(precursor 1)or through controlled release of hydroxyl ion of urea(precursor 2). The precursors were fired in air at 1000 ℃ for 2 h. Resulted phosphor synthesized with precursor 1 has non-uniformed particle with mean diameter of about 3 μm, while that with precursor 2 exhibits uniformed near spherical-like morphology with mean diameter of about 300 nm. Phosphors with the two methods exhibit same crystal structure as that of commercial one. Emission spectra of the samples indicate that the sample prepared with precursor 2 shows relative higher intensity(exited by 172 nm VUV)than that prepared with the other precursor.     

New Green Phosphors Ba（1-x）SrxZr（BO3）2 Doped with Tb^3＋ for PDP Applications

Thephosphorsusedinplasmadisplaypanel(PDP)deviceshouldemitvisiblelightundervacuum ultraviolet(VUV)excitationof147nmand or172nm fromXe Hegasplasma[1].Recentlylotsoftraditional lampphosphorshavebeenusedascommercialphos phorsforPDP.However,thesematerialsstill…     

Luminescence Properties of(Y,Gd)Al3(BO3)4∶Eu3+ under VUV excitation

(Y, Gd)Al3(BO3)4∶Eu3 samples were prepared by the conventional solid state reaction. The XRD results indicate that the crystal symmetry is low. The excitation spectrum is composed of two broad bands centered at about 170 and 250 nm respectively. In the emission spectra, the peak wavelength is about 616 nm under 147 nm VUV excitation. The luminescent chromaticity coordinate and the relative intensity change along with Gd3 mole concentration in the range of 0.15 to 0.85 mol(and Eu3 mole concentration, 0.02 to 0.1 mol). The correlative data show that the concentration quenching occurs when the Eu3 mole concentration ranges from 0.02 to 0.1 mol, and the Gd3 →Gd3 , Gd3 →Eu3 and host→Eu3 , Gd3 energy transfers exist, and Gd3 mole concentration influences Eu3 emission.     

Study on(Y,Gd)3(Al,Ga)5O12∶Ce3+ Phosphor

(Y1-a, Gda)3-x(Al1-b, Gab)5O12∶Ce3 x was synthesized by high-temperature solid state reaction in reducing atmosphere based on high purity raw materials. The influences of Y3 , Gd3 , Al3 , Ga3 and activator-Ce3 on the performance of the phosphor were investigated. Ce3 is the luminescent center and activates the phosphor after it replaces Y partially. When x is less than 0.12, the volume of the crystal and the emission intensity of the phosphor increase with the quantity of Ce3 . When CeO2 is added too much, the phase CeAlO3 will appear. The excitation and emission peaks of the phosphor will shift to longer wavelength when the amount of Gd3 increases. The wavelength of the emission peak can shift about 20 nm when a equals 0.45. In opposite, the excitation and emission peaks will shift to shorter wavelength, when part of Al3 is replaced by Ga3 . The wavelength of the emission peak can shift about 20 nm when b equals 0.55. Through the replacemeat of Y3 or Al3 by Gd3 or Ga3 , the emission peak of the phosphor can be adjusted from 520 to 560 nm. In this way, the phosphor is more suitable for different chips.