白光LED用LaPO4:Eu3+红色荧光粉的合成与表征

利用水热法制备了性能稳定的红色荧光粉LaPO4:Eu3+,同时研究了不同的Eu3+浓度、煅烧温度对荧光粉发光性能的影响.通过X射线粉末衍射(XRD)和扫描电子显微镜(SEM)来表征荧光粉的晶体结构和颗粒大小及形貌;用激发光谱和发射光谱以及荧光衰减曲线来表征荧光粉的荧光性能.结果表明:未煅烧时前躯体主要是六方晶相LaPO4·0.5H2O,煅烧温度在900℃时,所制备样品为单斜相LaPO4:Eu3+;SEM图像显示5 at.%Eu3+掺杂LaPO4呈椭球形,颗粒长约为500 nm,宽约为300 nm.最大发射波长和激发波长分别为592 nm和393 nm,发射光谱中592 nm和612 nm的发射峰对应的是Eu3+离子的5D0→7F1和5D0→7F2跃迁.其荧光寿命为3.32 ms.     

微波辅助液相法制备CaMoO4∶Eu3+荧光粉

采用微波辅助液相沉淀法制备了Ca1-xMoO4∶ Eu3+(0.05≤x≤0.09)系列红色荧光粉.通过荧光光谱仪、SEM、XRD测试和表征了该荧光粉的荧光性能、形貌、结构.结果表明,当Eu3+掺杂量为0.07,烧结温度为900℃,保温时间为3h时,可获得性能最佳的荧光粉,在395 nm和465 nm波长激发下,在616 nm处出现了很强的发射峰,对应于Eu3+的5D0→7F2的跃迁.采用微波辅助液相沉淀法制备的荧光粉发光强度高于高温固相法所制备的荧光粉,适合白光LED用红色荧光粉.     

微波辅助均相沉淀法制备（Y1-x-y, Lay）2O3:xEu3+红色荧光粉

用微波辅助均相沉淀法制备了一系列（Y_1-x-y, La_y）₂O₃:xEu3+(x=0.01~0.05, y=0.05~0.25) 红色荧光粉.研究Eu3+、La3+的掺杂浓度和煅烧温度对荧光粉性能的影响.通过差热分析仪、红外光谱仪、XRD、SEM和荧光分光光度计,对前驱体热重曲线和FTIR曲线、样品的晶体结构、表面形貌及颗粒大小和荧光性能进行表征.结果表明:前驱体组成为 (Y, La, Eu) OHCO₃·nH₂O;所制备样品为立方晶系;SEM显示荧光粉为均匀分散的球形颗粒,粒度为200 nm左右;较为适宜的焙烧温度为900 ℃;La3+掺杂含量y=10 %, Eu3+掺杂含量x=3 %时,样品荧光粉发光性能最好,最大发射波长为614 nm,对应的是Eu3+的5D₀→7F₂跃迁;样品的色坐标为 (0.654, 0.346).所制备的（Y_1-x-y, La_y）₂O₃:xEu3+荧光粉具备较好的发光强度与色纯度.      

Eu3+激活的Li2Gd4（MoO4）7钼酸盐红色荧光体及其发光性质

由高温固相反应首次合成Li2(Gd1-xEux)4(MoO4)7(0相似文献   

助熔剂对微波合成Y2O3:Eu3+红色荧光粉的影响

采用微波法合成Y2O3:Eu3+红色荧光粉,研究了碳酸盐、氟化物、硼酸等助熔剂对其合成过程及发光性能的影响.分别采用光谱分析仪和激光粒度仪对所合成荧光粉的光电性能和粒径进行分析.结果表明,不同助熔剂的加入对样品发射主峰的位置(610 nm)没有产生影响,但可明显影响样品的发光性能和粒径.采用碳酸盐单一助熔剂时,样品的相对亮度比采用氟化物时的高;采用复合助熔剂所制备样品在相对亮度及粒径方面,整体上较采用单一助熔剂样品的更优.     

NaGd(WO4)2∶Sm3+荧光粉的制备及光致发光

采用高温固相法制备了NaG,d(WO4)2∶Sm3+红色荧光粉.通过X射线粉末衍射(XRD)、扫描电子显微镜(SEM)和光致发光光谱(PL)对样品的物相、形貌及发光性能进行了表征.结果 表明,合成的NaGd(WO4)2∶Sm3+红色荧光粉为四方晶系,白钨矿结构.激发光谱中,位于405 nm和420 nm的激发峰分别归属...     

阳离子引入对CsPF6:Mn4+红色荧光粉发光性能的影响

采用共沉淀法在室温条件下合成了CsPF₆:Mn4+荧光粉,研究了Li+、Na+、K+阳离子的引入对CsPF₆:Mn4+荧光粉发光强度的影响。所制备的系列荧光粉样品均为立方结构纯相。在蓝光激发下,呈现最强峰位于634 nm处的一系列窄带红色发射。加入K+和Li+后,发光强度增强,加入Na+后发光强度有所减弱,其中加入K+的CsPF₆:Mn4+荧光粉发光强度最强。CsPF₆:Mn4+, K+荧光粉的发射强度随着温度的上升先增强然后由于非辐射跃迁的增加而降低,在423 K时达到最大值,发射强度相较于未引入阳离子的荧光粉发射强度亦增强。阳离子的引入可以有效提升CsPF₆:Mn4+荧光粉的发光性能。      

熔盐法合成红色荧光粉CaWO_4∶Eu~(3+)及其发光性能的研究

采用熔盐法在800℃条件下合成了红色荧光粉CaWO4:Eu3+。通过多种手段对样品进行了表征,并与固相法样品进行了对比。XRD结果表明所合成的荧光粉衍射峰位置和标准卡77-2233一致,为单一四方晶系的白钨矿结构;SEM结果表明荧光粉形貌规则,粒度分布均匀,分散性较好;光谱结果显示荧光粉的发射主峰位于614 nm处,激发主峰位于393 nm处,为近紫外激发,色坐标为(0.661,0.343),且色纯度与商品粉相当。由于CaWO4∶Eu3+用熔盐法合成具有工艺简单、能耗低、周期短等特点,合成样品粉体形貌好、粒度分布均匀、结晶度高,样品质量不低于固相法样品,因此,该方法值得研究者关注。     

溶胶-凝胶法制备Ca3Al2O6：Eu3+红色荧光粉及其发光性能

采用溶胶-凝胶法合成Ca3Al2O6：Eu3+红色荧光粉,通过XRD、SEM、荧光光谱分别对样品的结构、形貌以及发光性能进行表征,讨论煅烧温度、Eu3+掺杂浓度以及电荷补偿剂对样品发光性能的影响.结果表明：实验所得样品的结构与Ca3Al2O6相同,Eu3+掺杂并没有改变其晶体结构.合成的荧光粉在394 nm近紫外光激发下发出615 nm明亮的红光.样品的红光强度随着煅烧温度的升高先增加后减弱,最佳烧结温度为1200℃.同样红光强度也随着Eu3+掺杂浓度的增加先增加后减弱,最佳Eu3+掺杂浓度为4%（摩尔分数）.加入电荷补偿剂后样品的发光强度均增强,其中加入K+后发光增强的效果最显著.该铝酸盐红色荧光粉性质稳定,在白光LED近紫外芯片激发中具有潜在的应用.     

溶胶-凝胶法制备La2Ce2O7:Eu3+及其发光性能

采用溶胶-凝胶法（Sol-gel）合成La₂Ce₂O₇:Eu3+系列红色荧光粉,并研究煅烧温度、Eu3+掺杂浓度以及不同种类电荷补偿剂对样品发光性能的影响.通过XRD、SEM、荧光光谱对样品的晶体结构、形貌以及发光性能进行测量和表征.结果表明:实验所得样品主晶相为La₂Ce₂O₇,属于萤石结构. Eu3+及电荷补偿剂的掺杂没有改变其晶体结构.合成的样品在467 nm蓝光激发下发出612 nm的红光.样品的发光强度随煅烧温度以及Eu3+掺杂浓度的提高先增强后减弱,样品的较优的煅烧温度为1 100 ℃,Eu3+较优的掺杂浓度为10 %（摩尔百分比）.掺入电荷补偿剂可以有效增强样品的发光强度,其中掺入Li+后发光增强的效果最显著.      

作为白光LED用铕掺杂氟化镧红色荧光粉的制备与光谱性能研究

采用水热法制备具有单一相六方晶系的LaF₃:Eu3+纳米荧光粉.通过X射线粉末衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、光致发光光谱(PL)和荧光衰减曲线对LaF₃:Eu3+纳米荧光粉进行表征.LaF₃:Eu3+荧光粉的激发光谱主要由250 nm处的宽带(O2-→Eu3+的电荷转移跃迁)和一些尖峰(Eu3+ f-f跃迁)构成,其中位于近紫外区396 nm处有一较强的激发峰.通过发射光谱探测Eu3+在LaF₃晶体中的局部晶场环境.在298 K下激发光谱和发射光谱可知,在六方晶系的LaF₃纳米晶体中的Eu3+晶格位置从D_4h降至到C_2v,这是由于晶格变化所造成的.在396 nm激发下,观测到较优掺杂浓度为10%的LaF₃:Eu3+荧光粉在591 nm(5D₀→7F₁跃迁)处有强烈的红色发射峰.其发光性能表明,LaF₃:Eu3+红色荧光粉在近紫外发光二极管领域具有潜在的应用价值.      

Synthesis and photoluminescence properties of ZnTiO3:Eu3+ red phosphors via sol-gel method

ZnTiO3:Eu3+ phosphors were synthesized with different concentrations of Eu3+ doping through sol-gel method. The samples were calcined at different temperatures for 2 h in air. The synthesized powders were characterized by X-ray diffraction(XRD), scanning electron microscopy-energy dispersive spectroscopy(SEM-EDS), transmission electron microscopy(TEM), Raman and photoluminescence spectroscopy. The XRD results showed that the Zn Ti O3:Eu3+ phosphors doped with different concentrations of Eu3+ ions calcined at 600 oC were of single phase, which indicated that the Eu3+ ions had been successfully incorporated into the Zn Ti O3 host lattice and did not destroy the lattice structure of Zn Ti O3 host. The Raman spectrum, SEM and TEM also proved that the doping of Eu3+ did not change the lattice structure of hexagonal Zn Ti O3 host. The photoluminescence(PL) of Eu3+ ions with the main emission peak at 614 nm was observed to increase with Eu3+ concentrations from 0.5 mol.% to 2.0 mol.% and decreased when the concentration was increased to 2.5 mol.%. The decrease in the PL intensity at higher Eu3+ concentrations could be associated with concentration quenching effect. The CIE1931 chromaticity diagram(x, y) of Zn Ti O3:2.0 wt.%Eu3+ phosphors were located in the red region(x=0.652, y=0.347). The luminescence properties suggested that Zn Ti O3:Eu3+ phosphors might be regarded as a potential red phosphor candidate for light emitting diodes(LEDs).     

Y2O3-SiO2∶Eu3+,Bi3+荧光材料的结构及性能研究

用溶胶-凝胶法(Sol-gel法)低温合成了Y2O3-SiO2∶Eu3+,Bi3+红色发光粉.X射线实验研究发现,850℃时,样品晶体结构为Y2SiO5,属单斜晶系(a=9.012,b=0.979,c=6.630),空间点群为PI1/C;SEM实验显示发光体为不规则片层结构;粒度分析表明发光体粒度分布均匀,平均粒度为0.79μm;T≥600℃时,发光体出现温度猝灭现象.     

Influence of urea on microstructure and optical properties of YPO4：Eu^3＋ phosphors

YPO4:Eu 3+ phosphors were synthesized by solution coprecipitation method assisted by urea in the precursor reaction solution. X-ray diffraction spectral analysis showed that the samples synthesized with urea had smaller particle size and lower crystallinity than those samples synthesized without urea.Moreover,the calculated strain result indicated that the Eu 3+ site in the former exhibited a lower crystal field symmetry than that in the latter.Hence,the influence of crystal field symmetry dominated luminescence efficiency rather than crystallinity because the luminescence intensity observed in Eu0.05Y0.95PO4 synthesized with 1.0 g urea was six-fold higher than that of the as-synthesized sample.With increased concentration of Eu 3+ ion,the luminescence intensity initially increased,and then subsequently decreased as the concentration of Eu 3+ ion exceeded 12 mol.%due to concentration quenching.The optimal condition for YPO4:Eu 3+ phosphor was Eu0.12Y0.88PO4 with 1.0 g urea added in the precursor.The luminescence intensity of the optimal condition was again enhanced 1.6-fold relative to that of Eu0.05Y0.95PO4 synthesized with 1.0 g-urea.     

Structure and Magnetocaloric Effect in Tb（ Co1-xSnx）2 Alloys

Recently,researchonmagnetocaloriceffect(MCE)hasattractedagreatdealofinterestinrare earth(RE)basedcompoundsbecauseoftheirenergy efficiencyandenvironmentalsafetyformagneticrefrig eration.Afirst ordermagneticphasetransitionwas foundintheintermetalliccompoundsRECo2(RE=Er,Ho,Dy)withMgCu2typestructure[1,2],leadingtoa largemagneticentropychangeforthesecompounds,whereasasecond ordertransitionwasfoundinTbCo2andGdCo2.IntheintermetalliccompoundsRECo2,theloweringofd electronconcentrationbythesubst…     

Broadband downconversion in YVO4：Tm3＋,Yb3＋ phosphors

An efficient near-infrared (NIR) downconversion (DC) by converting broadband ultraviolet (UV) into NIR was demonstrated in YVO4:Tm3+,Yb3+ phosphors. The phosphors were extensively characterized using various methods such as X-ray diffraction, photoluminescence excitation, photoluminescence spectra and decay lifetime to provide supporting evidence for DC process. Upon UV light varying from 260 to 350 nm or blue light (473 nm) excitation, an intense NIR emission of Yb3+ corresponding to transition of 2F5/2→2F7/2 peaking at 985 nm was generated. The visible emission, the NIR mission and the decay lifetime of the phosphors of various Yb3+ concentrations were investigated. Experimental results showed that the energy transfer from vanadate group to Yb3+ via Tm3+ was very efficient. Application of the broadband DC YVO4:Tm3+,Yb3+ phosphors might greatly enhance response of siliconbased solar cells.     

Effect of gadolinium incorporation on optical characteristics of YNbO_4：Eu~（3＋） phosphors for lamp applications

Eu3+-doped (Y,Gd)NbO4 phosphor was synthesized by solid-state reaction for possible application in cold cathode fluorescent lamps. A broad absorption band with peak maximum at 272 nm was observed which was due to the charge transfer between Eu3+ ions and neighboring oxygen anions. A deep red emission at the peak wavelength of 612 nm was observed which could be attributed to the 5D0→7F2 transition in Eu3+ ions. The highest luminance for Y1-x-yGdyNbO4:Eux3+ under 254 nm excitation was achieved at Eu3+ concentration of 18 mol.% (x=0.18) and Gd3+ concentration of 8.2 mol.% (y=0.082). The luminance of Y0.738Gd0.082NbO4:Eu3+0.18 was higher than that of a typical commercial phosphor Y2O3:Eu3+ and the CIE chromaticity coordinate was (0.6490, 0.3506), which was deeper than that of Y2O3:Eu3+. The particle size of the synthesized phosphors was controlled by the NaCl flux and particle size as high as 8 μm with uniform size distribution of particles was obtained.     

Properties of red-emitting phosphors Sr2MgSi2O7:Eu3+ prepared by gel-combustion method assisted by microwave

Novel red-emitting phosphors Sr2MgSi2O7:Eu3+ were prepared by gel-combustion method assisted by microwave. The phase struc-ture and luminescent properties of as-synthesized phosphors were investigated by XRD and fluorescence spectrophotometer, respectively. The results showed that the as-synthesized sample was Sr2MgSi2O7 with tetragonal crystal structure. The excitation spectrum of Sr2MgSi2O7:Eu3+ was composed of two major parts: one was the broad band between 200 and 350 nm, which belonged to the charge transfer of Eu3+-O2-; the other consisted of a series of sharp lines between 350 and 450 nm, ascribed to the f-f transition of Eu3+. The emission spec-trum consisted of two emission peaks at 593 and 616 nm, which was attributed to 5D0→7F1 and 5D0→7F2 of Eu3+, respectively. The concen-tration of Eu3+ (x) had great effect on the emission intensity of Sr2-xMgSi2O7:Eu3+x. When x varied in the range of 0.04-0.18, the intensity of emission peaks at 593 and 616 nm increased gradually with the concentration of Eu3+ increasing. It was interesting that no concentration quenching occurred. Moreover, the luminescent intensity could be greatly enhanced with incorporation of charge compensator Li+ ions.     

A novel Tb3+ and Eu3+ co-doped dual-emitting phosphate K3SrBi(P2O7)2 phosphor for application in FIR thermometers

Rare earth co-doped phosphor for fluorescence intensity ratio(FIR) thermometer has gained increasing attention in recent years. Herein, the novel Tb³⁺and Eu³⁺co-doped K₃SrBi(P₂O₇)₂(KSBP) phosphate phosphors were reported. The crystal structure of the title phosphor was determined using Rietveld refinement and proved to have a three-dimensional structure. The time-resolved spectroscopy reveals that there is almost no energy transfe...