CaMoO4：Eu3+,Bi3+,Li+红色荧光粉的共沉淀制备与表征

采用共沉淀法合成了红色荧光粉Ca_0.75MoO₄：Eu_0.25³⁺、Ca_0.75MoO₄：Eu_0.25-x³⁺,Bi_x³⁺及Ca_0.5MoO₄：Eu_0.25-2x³⁺, Bi_x³⁺,Li_0.25+x⁺,并采用X射线衍射(XRD)、拉曼光谱,扫描电镜(SEM)和荧光光谱(PL)测定分析了其结构形貌特征及发光性能。结果表明：制备的CaMoO₄：Eu³⁺,Bi³⁺,Li⁺红色荧光粉为白钨矿结构,颗粒尺寸约为0.5~1 μm。掺杂Bi³⁺的Ca_0.75MoO₄：Eu_0.25-x³⁺,Bi_x³⁺的相对发光强度明显高于未掺Bi³⁺的Ca_0.75MoO₄：Eu_0.25³⁺荧光粉。Bi³⁺离子的掺杂将吸收来的能量传递给激活离子Eu³⁺,起到了能量传递的作用。当Bi³⁺掺杂量为x=0.005时,在395 nm激发下,主发射峰在616 nm处的相对发光强度最大,但掺杂浓度过高时会出现浓度猝灭现象。另外,电荷补偿剂的掺入能够解决材料中因同晶取代引起的电荷不平衡的问题,以Li⁺作电荷补偿剂、Eu³⁺和 Bi³⁺共掺合成的Ca_0.5MoO₄：Eu³⁺_0.23,Bi_0.01³⁺,Li⁺_0.26红色荧光粉的发光性能强于Ca_0.75MoO₄：Eu_0.25³⁺、Ca_0.5MoO₄：Eu_0.25³⁺, Li_0.25⁺及Ca_0.75MoO₄：Eu_0.24³⁺,Bi_0.01³⁺。     

一种LED用红色荧光粉BaZn2(BO3)2：Eu3+的合成与发光性能研究

通过高温固相法制得双峰可调节本征半导体发光BaZn₂（BO₃）₂：Eu³⁺荧光粉,此类荧光粉在300~400 nm的紫外波段有很强的吸收。在375 nm的紫外光激发下,该荧光粉产生了两个宽带的发射峰,分别位于550 nm和615 nm处。并且,在395 nm的紫光激发下,荧光粉会由于Eu³⁺离子的⁵D₀→⁷F₂电偶极跃迁产生一个位于615 nm的强宽发射峰,这表明Eu³⁺离子占据了反演对称中心的位置,取代了BaZn₂（BO₃）₂中部分的Ba²⁺离子。当Eu³⁺的摩尔分数达到10%时,发生浓度猝灭。在不同浓度的Eu³⁺离子的掺杂下,BaZn₂（BO₃）₂：Eu³⁺荧光粉的发光从黄色延伸到红色,实现了荧光粉的色度可调。     

MgO对Sr2SiO4:Eu2+荧光粉发光性质的影响

通过在Sr₂SiO₄:Eu²⁺荧光粉中加入MgO,提高了Sr₂SiO₄:Eu²⁺荧光粉的蓝光和黄光发射带的发射强度,研究了MgO浓度对Sr₂SiO₄:Eu²⁺荧光粉发光强度的影响。当Mg与Si的量比在1.0附近时,荧光粉的亮度较高,且发光颜色为白色。通过调节Sr₂SiO₄:yEu²⁺ ,MgO荧光粉中Eu²⁺的掺杂浓度,可以调节荧光粉的发光颜色。用Sr₂SiO₄:Eu²⁺ ,MgO和400 nm的InGaN管芯制备的白光LED,色坐标优于α'-Sr₂SiO₄:Eu²⁺和β-Sr₂SiO₄:Eu²⁺荧光粉制成的白光LED,显色指数和流明效率高于β-Sr₂SiO₄:Eu²⁺和α'-Sr₂SiO₄:Eu²⁺制成的白光LED。     

白光LED用红色荧光粉Gd2Mo3O9：Eu3+的制备及表征

利用Na₂CO₃作为助熔剂,采用高温固相反应方法制备了三价铕离子激活的Gd₂Mo₃O₉红色荧光粉。利用XRD和荧光光谱,研究了助熔剂的量、制备时的温度以及激活剂Eu³⁺的浓度对荧光粉的晶体结构和发光性能的影响。测试结果表明,这种新型的荧光粉可以被紫外光280nm,近紫外光395nm和蓝光465nm有效激发,发射主峰位于613nm,并且证明Eu³⁺离子在晶体结构中占据了非反演对称中心的位置。395,465nm的吸收与目前广泛应用的紫外和蓝光LED芯片的输出波长相匹配。因此,这种荧光粉是一种可能应用在白光LED上的红色荧光粉材料。     

Eu3+掺杂的Y10W2O21纳米荧光粉的制备及其发光性质研究

用沉淀法合成了Y10W2O21:Eu纳米发光材料,利用X射线衍射谱(XRD)和场发射扫描电镜(FE-SEM),对样品的结构和形貌进行了表征.测量了各样品的激发光谱、发射光谱,绘制了Eu3+发光的浓度猝灭图,计算了各样品的部分J-O参数和EC+5 D0能级量子效率,对Eu3+掺杂的Y10W2O21纳米发光材料的光致发光性...     

Eu3+激活K2CaP2O7荧光粉的制备和发光性质

采用高温固相法制备了系列不同浓度Eu³⁺离子掺杂的K₂CaP₂O₇红色荧光粉。通过X射线衍射、扫描电子显微镜、荧光光谱和荧光寿命曲线等手段对荧光粉的物相结构、形貌以及发光性质进行了研究。结果表明所制备的荧光粉均属于单斜结构,Eu³⁺离子掺杂没有引起晶体结构明显变化,荧光粉形貌不规则,颗粒为微米量级且部分发生团聚。在393 nm紫外光激发下,荧光粉显示出红光发射,最强发射峰位于613 nm。Eu³⁺离子掺杂浓度对发光强度有显著影响,最佳掺杂摩尔分数为0.08,由此计算能量传递临界距离为1.61 nm。荧光寿命受掺杂浓度影响较小,当Eu³⁺掺杂摩尔分数为0.005~0.10时,荧光寿命在2.45~2.58 ms范围内。变温发射光谱显示,测试温度为150℃时,荧光粉的发光强度为室温的73%。研究表明,Eu³⁺离子掺杂的K₂CaP₂O₇是性能较好的红色荧光粉。     

白光LED用红色荧光粉KLa（MoO4）2:Eu3+的制备及发光性能

采用水热法制备红色荧光粉KLa(MoO4)2:Eu3+,通过X射线粉末衍射(XRD)、场发射扫描电镜(FE-SEM)和荧光光谱(PL)对样品进行了表征。实验结果表明:pH值是合成样品KLa(MoO4)2:Eu3+的关键因素,当溶液pH值接近7时,荧光粉的纯度较高,分散性良好、粒度均匀、呈规则球形。这种荧光材料可以被紫外光279 nm、近紫外光395 nm和蓝光465 nm有效激发,发射主峰位于617 nm,是一种可应用于白光LED转换用的新型红色荧光粉。     

Eu3+掺杂CaMoO4微米荧光粉发光性质的研究

运用化学沉淀的方法合成了不同Eu³⁺掺杂浓度CaMoO₄微米荧光粉样品, 详细研究了样品的光致发光性质. 研究表明: CaMoO₄: Eu可以被蓝光或近紫外光有效激发, 实现高色纯度的红光发射; 样品的黄昆因子数值数量级为10^-2, 是一种弱电声耦合材料; 样品中Eu³⁺的跃迁强度参数(Ω₂)随着掺杂浓度的提高而增大, 但量子效率却随着掺杂浓度的提高而减小; 通过对样品发光的浓度猝灭曲线的分析, 确定Eu³⁺的理想掺杂浓度为25%, 并判断出Eu³⁺在CaMoO₄基质中通过交换相互作用实现能量传递. 沉淀法制备的CaMoO₄: Eu微米荧光粉具有发光色纯度好, 制备工艺简单, 耗时较少的优点, 是一种性能优异的红色荧光粉材料.     

Eu3+掺杂CaWO4红色荧光粉发光性质的浓度依赖关系研究

采用共沉淀法制备了不同Eu³⁺掺杂浓度的CaWO₄荧光粉材料.通过X射线衍射和场发射扫描电镜技术对样品的结构和形貌进行了表征.测量了各样品的激发光谱、发射光谱和荧光衰减曲线, 计算了各样品的部分Judd-Oflet (J-O)参数和^5D_0 (Eu³⁺)能级量子效率,以及荧光粉的色坐标, 讨论了样品电荷迁移带相对强度、J-O参数、量子效率与掺杂浓度的依赖关系.对Eu³⁺掺杂的CaWO₄ 发光材料的光致发光性质的研究表明,在CaWO₄: Eu³⁺中⁵D₀→⁷F₂跃迁的616~nm 红色发光能被394.5~nm和465~nm的激发光有效激发,具有近紫外(或蓝光)激发效率高和猝灭浓度大的优点, 有潜力成为高效的近紫外(或蓝光)激发白光发光二极管用红色荧光粉材料.     

Gd2(WO4)3: Eu纳米发光材料中黄昆因子和能量传递速率的实验获得

采用共沉淀法制备了不同Eu³⁺掺杂浓度的Gd₂(WO₄)₃纳米发光材料. 测量了纳米材料样品的X射线衍射谱(XRD) 和场发射扫描电镜, 对样品的结构和形貌进行了表征. 测量了各样品的发射光谱和激发光谱(声子边带光谱), 绘制了浓度猝灭曲线, 确定了最佳的掺杂浓度为20 mol%. 通过声子边带光谱计算了不同掺杂浓度样品的黄昆因子. 测量了不同浓度样品的荧光寿命, 利用Auzel模型对Eu^{3+ 5}D₀能级荧光寿命数据进行了拟合, 确定了⁵D₀能级的固有寿命和猝灭过程中生成的声子数. 本文还根据荧光寿命数据计算了Eu³⁺之间的能量传递速率, 确定了能量传递速率与浓度的关系. 关键词： 钨酸盐 3+')" href="#">Eu³⁺ 黄昆因子 能量传递速率     

Luminescent properties of (Y,Gd)BO3:Bi,RE (RE=Eu, Tb) phosphor under VUV/UV excitation

Bi³⁺- and RE³⁺-co-doped (Y,Gd)BO₃ phosphors were prepared and their luminescent properties under vacuum ultraviolet (VUV)/UV excitation were investigated. Strong red emission for (Y,Gd)BO₃:Bi³⁺,Eu³⁺ and strong green emission for (Y,Gd)BO₃:Bi³⁺,Tb³⁺ are observed under VUV excitation from 147 to 200 nm with a much broader excitation region than that of single Eu³⁺-doped or Tb³⁺-doped (Y,Gd)BO₃ phosphor. Strong emissions are also observed under UV excitation around 265 nm where as nearly no luminescence is observed for single Eu³⁺-doped or Tb³⁺-doped (Y,Gd)BO₃. The luminescence enhancement of Bi³⁺- and RE³⁺-co-doped (Y,Gd)BO₃ phosphors is due to energy transfer from Bi³⁺ ion to Eu³⁺ or Tb³⁺ ion not only in the VUV region but also in the UV region. Besides, host sensitization competition between Bi³⁺ and Eu³⁺ or Tb³⁺ is also observed. The investigated phosphors may be preferable for devices with a VUV light 147-200 nm as an excitation source such as PDP or mercury-free fluorescent lamp.     

Eu3+激活的La2Mo2O9红色荧光粉的制备与性能

利用高温固相法制备了Eu³⁺掺杂的La₂Mo₂O₉红色荧光粉,并对这种荧光粉的结构及发光性质进行了研究。XRD结果表明,实验合成了单一立方相的La₂Mo₂O₉荧光粉体。该荧光粉的激发光谱由一宽带和一系列的锐峰组成;发射光谱由一系列锐峰组成,这些都与Eu³⁺的特征跃迁⁵D_J(J=0,1)和⁷F_J(J=1~4)相对应。结果表明该荧光粉可被395nm的紫外光和470nm的可见光有效激发,并发出峰值位于620nm左右的红光,亮度可达到传统红色荧光粉Y₂O₂S:Eu³⁺的1.5倍以上,这表明它可以作为蓝+黄模式白光LED的红色补光粉,也可以作为UV-LED激发三基色荧光粉体系中的红色荧光粉。研究了Eu³⁺的掺杂浓度以及不同助熔剂对样品发光性质的影响。Eu³⁺的摩尔分数为0.3时,发光强度达到最强。质量分数为3%的NH₄Cl作为助熔剂时效果最好。     

Synthesis,characterization and photoluminescence of Eu3+, Ce3+ co-doped CaLaAl3O7 phosphors

Powder phosphors of CaLa_{1? x} Eu _x Al₃O₇, CaLa_{1? x} Ce _x Al₃O₇ and CaLa_{0.99? x} Eu _x Ce_0.01Al₃O₇, where x = 0.01, 0.03, 0.05 and 0.07, were prepared by a combustion method. The powders were well characterized by X-ray diffraction (XRD), scanning electron microscope (SEM) and photoluminescence techniques. Emission spectra of Eu³⁺-doped powder phosphors showed strong red emission at 613 nm (⁵D₀ → ⁷F₂); no concentration quenching was observed. Generally, Ce³⁺ acts as an efficient sensitizer when doped with other trivalent lanthanide ions. However, interestingly, in the CaLaAl₃O₇ powder phosphors, the addition of Ce³⁺ with Eu³⁺ exhibited an adverse effect–decreased photoluminescence intensity. The reasons for this behavior are discussed.     

Synthesis, characterization and optical spectroscopy of Eu doped titanate nanotubes

The synthesis of Eu³⁺ doped titania nanotubes was carried out via a hydrothermal method. X-ray diffraction and transmission electron microscope analyses showed that the nanotubes were formed by rolling multilayered titania structure with a length of up to 100 nm. The Eu³⁺-doped nanotubes exhibited strong emission lines associated with the ⁵D₀→⁷F_J (with J from 1 to 4) transition of Eu³⁺ and the differences between the luminescence properties of the precursor powders and the nanotubes were studied at low temperature.     

Synthesis and properties of submicron range CaSO4:Eu particles

CaSO₄:Eu with particle size in submicron range was synthesized. Radiation induced Eu³⁺↔Eu²⁺ conversion as well as thermal conversion was studied. The samples showed thermal conversion above 400 °C. However, no radiation induced conversion in submicron range particles was observed. Particles heated above 400 °C coalesce and when heated at 925 °C bigger particles of 20 μm size were formed. Optical microscopy of these particles reveals red inclusion of about 5 μm inside CaSO₄ particle. It is speculated that the red inclusion is CaS:Eu²⁺.     

发光二极管用红色荧光粉SrMoO4:Eu3+的制备和发射性质

采用化学共沉淀法制备了适合于紫外、近紫外、蓝光发光二极管(LED)激发的红色荧光粉SrMoO4:Eu3+.研究了样品的晶体结构和发光性质.结果表明:化学共沉淀法合成的SrMoO4:Eu3+荧光粉为四方纯相,其激发光谱包括一个宽带峰和一系列尖峰,峰值位于280nm(宽带峰中心),395nm,465nm,可以被紫外LED和蓝光LED有效激发.在395nm的激发下,测得发射光谱的强发射峰位于613nm,对应Eu3+离子的5D0→7F2跃迁.Eu3+离子掺杂浓度的改变对基质的晶格常数、Eu3+离子在晶体中对称性及发光性能有较大影响.通过对比不同掺杂浓度Eu3+离子的发射谱,发现在SrMoO4基质中Eu3+离子掺杂存在浓度猝灭现象,其最佳掺杂浓度为15%.     

纳米YPO4:Eu3+的合成及发光性质研究

采用水热法合成了纳米Y_1-xPO₄:xEu³⁺（005≤x≤030）系列荧光粉,并对样品进行了热处理.通过X射线衍射（XRD）、扫描电镜（SEM）等手段分析了合成样品的结构及形貌,结果表明合成的样品均为四方磷钇矿结构,在酸性和碱性条件下分别为球状和细棒状,且均在纳米尺度.研究其在真空紫外（VUV）激发下的发光性质发现,样品的激发峰最大值位于142 nm左右;与固相法的样品相比,PO^3-     

Radiation effects on luminescent and structural properties of YPO4: Pr3+ nanophosphors

ABSTRACT

YPO₄ phosphors doped with trivalent ion Pr³⁺ were prepared by sol–gel method and treated with different doses of gamma radiation, from 0.25 MGy to 4 MGy. Effects of radiation on morphology, structure and luminescent properties were analyzed. Also, the influence of radiation on the change in the color of the samples was examined. The color efficiency of powders was evaluated by colorimetric analysis (CIE and L * a * b system). It has been observed that powders change color under the influence of radiation, i.e. they pass from white to pinkish red. Also, it has been determined that the radiation affects morphology change, as the particle size increases with increasing of the radiation dose. With the increase in the radiation dose, the emission intensity of samples decreases. The structure remains almost unchanged after irradiation, and the intensity constantly decreases with increasing of dose.