Eu3+掺杂SiO2-Al2O3-B2O3玻璃制备及光谱性能研究

高温溶制了Eu^3＋掺杂SiO2-Al2O3-B2O3-MxOy（M=Li^＋,Na^＋,K^＋,Mg^2＋,Ca^2＋,Sr^2＋,RE^3＋）硼硅酸盐玻璃,测试了玻璃样品的发射光谱、激发光谱和透射光谱,研究了不同碱金属离子、碱土金属离子对该系统荧光性能的影响。利用发射光谱计算了Ω2,Ω4以及^5D0到^7F2,^7F4的自发辐射几率和振子强度f（^5D0→^7F2）,f（^5D0→^7F4）。结果表明,材料的发射能级为^5D0→^7F1（590nm）,^5D0→^7F2（617nm）,^5D0→^7F4（698nm）,而且材料的结构对称性越差,跃迁戒律打破地越彻底,荧光发射越强。     

三种方法制备CaGdAlO4:Eu3+荧光粉及其发光性质研究

分别采用柠檬酸溶胶-凝胶法、半干半湿法和高温固相法制备了CaGdAlO4：Eu^3＋荧光粉，并用X线衍射（XRD）分析、场发射扫描电镜（FE—SEM）观察和荧光光谱分析研究了不同制备方法和制备条件对CaGdAlO4：Eu^3＋形貌、粒径和发光性质的影响。XRD结果表明，柠檬酸溶胶-胶法、半干半湿法和固相法制备CaGdAlO4：Eu^3＋生成纯相的温度分别为900，1200和1400℃。FE—SEM照片显示CCaGdAlO4：Eu^3＋颗粒粒径随温度的升高而增大，在同一烧结温度下，粒径大小为柠檬酸溶胶-凝胶法最小，半干半湿法居中，高温固相法最大而且团聚现象严重。以280nm近紫外光激发，CaGdAlO4：Eu^3＋发出明亮的橙红色荧光，以Eu^3＋的^5D0→^7F2跃迁为主，发光强度随烧结温度的升高而增加，在1400℃烧结温度下，以半干半湿法得到的样品发光最强。室温和低温发射谱中Eu^3＋的^5D0→^7Fj，发射峰的数目都表明：Eu^3＋在CaGdAlO4中只占据偏离反演中心的一种格位。     

SrZnO2:Eu3+, Li+长波紫外激发红光荧光体的合成及发光性能研究

采用高温固相法合成了一种长波紫外激发的SrZnO2：Eu^3＋, Li^＋发光材料, 用X射线衍射谱、荧光光谱对样品进行了表征. 结果表明, Eu^3＋离子在SrZnO2基质中主要占据Sr^2＋离子不对称性格位, 发射来源于5D0→7F2 612 nm为主的红光. 加入电荷补偿剂Li^＋离子能显著提高发光强度, 350～400 nm内的激发峰也有明显提高, 同时观察到来自Eu^3＋离子高能级5D1→7FJ（J=0～2）的跃迁发射, 并对其产生机制进行了初步探讨. 实验结果表明, SrZnO2：Eu^3＋, Li^＋是一种有发展前途的长波紫外激发红光荧光体.     

Sr5SiO4Cl6:Eu2+蓝白色荧光粉的发光特性研究

采用高温固相法合成了Sr5SiO4Cl6∶Eu^2＋荧光粉。该荧光粉在近紫外360 nm激发下,出现了峰值位于454 nm稍不对称的发射峰,对其进行Gaussian曲线拟合,分解得到了451和470 nm两个明显的发射峰。利用Van Uitert公式讨论了晶格环境对Eu^2＋发光中心能量状态的影响,得出451和470 nm发射峰为Eu^2＋分别占据九配位和八配位的Sr^2＋格位跃迁产生的。研究了烧结温度以及Eu^2＋含量对荧光粉发光强度的影响。     

Preparation and Luminescence Behavior of CaSiO3：Eu^3＋（Bi^3＋）

CaSiO3：Eu0.08^3＋Bi0.002^3＋ with a monoclinic perovskite structure was synthesized by using sol-gel method, and its luminescence characteristics were investigated. From the excitation spectrum, it can be seen that the main peaks located at 238,396,415,437 and 359 nm correspond to the charge-transfer band of Eu^3＋-O^2- , the absorption transitions of ^7F0.1→^3L6, ^7F0→^5D3, ^7F1→^5D3 of Eu^3＋ ions, and ^3P1→^1S0 of Bi^3＋ ions, respectively. When the samples were excited with a light of wavelength 359 or 395 nm, it can be seen from the emission spectrum that the electronic dipole transition located at 609 nm corresponding to ^5D0→^7F2 of Eu^3＋ ions was stronger than the magnetic dipole transition located at 587 nm corresponding to ^5D0→^7F1 of Eu^3＋ ions, which shows that more Eu^3＋ ions were located in nonreversion center lattices. The energy transfer from Bi^3＋ ions to Eu^3＋ ions in the phosphor was also discussed. The results show that Eu^3＋ ions could be well sensitized by ^3＋ions, and the energy-transfer pattern between Bi^3＋ ions and Eu^3＋ ions was resonance energy transfer.     

RbLn2F7的水热合成及RbLn2F7:Eu3+(Ln=Gd,Y)的VUV光谱

利用水热方法合成出RbLn2F7（Ln=Gd，Y，Er，Yb和Lu），均为六方RbEr2F7型结构。掺杂Eu^3＋离子样品的光谱表明水热产物中氧杂质含量极低。在RbGd2F7：Eu^3＋（0．5mol％）的激发光谱中只观测到Gd^3＋离子f-f跃迁，Eu^3＋离子的激发跃迁很弱。激发Gd^3＋离子到^6IJ能级后，观测到Eu^3＋离子的特征发射，Gd^3＋离子与Eu^3＋离子之间存在能量传递过程。Eu^3＋离子的^5D0→^7F1和^5D0→F2跃迁发射较强，表明稀土离子在六方HbLn2F7中处于非中心对称的格位。     

白光LED用荧光材料Ba3Gd（BO3）3∶Eu^（3＋）的发光性能研究

用高温固相反应法制备了稀土离子Eu^3＋掺杂的三元稀土硼酸盐Ba3Gd（BO3）3发光材料,通过X射线衍射（XRD）、荧光光谱和扫描电镜（SEM）等测试手段对Ba3Gd（BO3）3∶Eu^3＋荧光粉的制备条件、发光性能以及形貌进行了研究。XRD结果表明,在1000℃时可得到Ba3Gd（BO3）3纯相。扫描电镜照片显示颗粒基本为球形,粒径约为200-400 nm。发光光谱测试表明,Ba3Gd（BO3）3∶Eu^3＋荧光粉在近紫外区（UV）（396 nm）和蓝光区（466 nm）可以被有效地激发,分别用255和396 nm的紫外光激发样品时,以Eu3＋的5D0-7F2（611和616 nm）超灵敏跃迁为主要发射峰。当Eu3＋的掺杂浓度为10%（摩尔分数）时,Ba3Gd（BO3）3∶Eu3＋在611和616 nm处的发光强度最大。因此,这种荧光粉是一种可能应用在白光LED上的红色荧光材料。     

Eu:GGG纳米荧光粉体制备及其光学特性

采用液相共沉淀方法并在不同烧结温度下制得了Eu：GGG荧光粉体。用X射线衍射分析了样品的结构，计算了其晶格常数，为1．2371nm。室温下，测量了Eu：GGG的光致发射光谱、激发光谱和荧光衰减曲线。激发光谱在波长240～287nm的谱带内和393。。处有强的激发，分别来自于Eu^3＋O2^-间的电荷迁移态吸收和Eu“的^7F0→^5L6的跃迁吸收，同时在274nm处也出现了Gd^3＋的^8S7/2→^6I1的特征吸收。393nm激发下，591nm处的发射峰最强，对应Eu^3＋的^5D0→^7F1的磁偶极跃迁，可能由于部分Eu^3＋处于反演中心对称格位所致。随着烧结温度升高，Eu：GGG的发光强度增强，这可能由于随着烧结温度升高，样品晶粒尺寸变大，单位体积内被激发的Eu^3＋离子数增加引起，而591nm发光的荧光寿命变短，可能是由Eu^3＋离子的能量共振传递过程中发光被陷阱捕获所致。     

Ca2Y8（SiO4）6O2：RE（RE=Eu,Tb）发光薄膜的制备及发光性能的研究

采用溶胶－凝胶法制备了稀土离子掺杂（Eu^3 ,Tb^3 )的氧磷灰石三元稀土硅酸盐Ca2Y8(SiO4)6O2发光薄膜。通过X射线衍射（XRD）,红外光谱（IR）,扫描电镜（SEM）等方法对薄膜的组成、结构、颗粒尺寸、形貌及厚度进行了研究,通过发光光谱对薄膜的发光性质进行了分析。XRD结果表明700℃时薄膜尚处于非晶态,800℃时已开始有Ca2Y8(SiO4)6O2的物相形成,1000℃时结晶已完全。这一点和红外光谱的结果相符。发光光谱测试表明Ca2Y8(SiO4)6O2:Eu^3 薄膜显示了很强的红光发射,并以Eu^3＋的^5D0-^7F2(616nm)超灵敏跃迁为最强一组。Ca2Y8(SiO4)6O2:Tb^3 的发射光谱由蓝光发射和绿光发射两部分组成,前者对应于^5D3-^7FJ,后者对应于^5D4-^7FJ(J=6,5,4,3),且以^5D4-^7F5(544nm)绿光发射为最强。     

LaPO4:Eu3+纳米粒子的多醇法合成及其光致发光性能研究

以一缩二乙二醇为溶剂，采用多醇法（polyol method）合成LaPO4：Eu^3＋纳米发光材料，利用XRD、FE．SEM、TG-DTA、Uv-vis光谱、光致发光光谱（PL）及寿命等手段进行了表征。结果表明：所得到的材料结晶完好，具有LaPO4的独居石型结构；粒子的形貌为球形，其粒径约为25nm；在波长为258nm的紫外光激发下，其发射光谱由Eu^3＋的5D0^-7FJ（J=1，2，3，4）特征发射组成，在592nm处的磁偶极跃迁（5D0^-7F1）最强，表现为Eu^3＋的橙-红特征发射；LaP04：Eu^3＋纳米粒子中Eu^3＋的最佳掺杂浓度为5％（摩尔比）；Eu^3＋的光致发光衰减曲线符合单指数行为，其寿命（τ）为3．9ms。     

GdPO4:Eu3+和GdBO3:Eu3+中"Gd-Eu"间的能量传递

利用同步辐射光源(德国HASYLAB实验室的SUPERLUMI实验站)对高温固相法制备的GdPO4 Eu3+和GdBO3Eu3+的发射谱与激发谱进行了研究, 并从量子剪裁的角度对"Gd3+-Eu3+"之间的能量传递作了讨论. 在两种样品监测Eu3+红光发射的激发谱上, 都显著观察到了对应Gd3+离子4f-4f跃迁的谱线, 说明从基质中Gd3+离子向掺杂的Eu3+离子之间存在非常有效的能量传递, 这有利于量子剪裁的发生. 在激发谱上还观察到了对应Eu3+-O2-电荷迁移态的宽激发带(180～270 nm), 而对应Gd3+离子8S7/2→6GJ跃迁的谱线(196 nm, 203 nm)叠加在这个宽带之上, 微弱可辨, 这不利于Gd3+-Eu3+间交叉弛豫的能量传递过程, 从而不利于量子剪裁的发生. 结合Eu3+-O2-电荷迁移态位置变化的规律, 提出了如何避开其干扰以增强量子剪裁效应的材料设计方案.     

Eu3+ concentration dependent optical properties and energy transfer from host Gd3+ to Eu3+ in GdF3 nanocrystals

By using a hydrothermal method, a series of Eu³⁺ concentration dependent GdF₃ nanocrystals have been synthesized. The crystalline structures of samples are characterized by XRD patterns, the morphology and size of the samples are illustrated by FE-SEM images, and the optical properties of the samples are presented by PL excitation and emission spectra. The energy transfer from host Gd³⁺ to Eu³⁺ is observed in the Eu³⁺ doped GdF₃ nanocrystals. The optical properties of Eu³⁺ and the energy transfer efficiency from host Gd³⁺ to Eu³⁺ are discussed on the basis of the Eu³⁺ concentration dependent integrated PL excitation and emission spectra of Gd³⁺ and Eu³⁺. The discussion on optical properties of Eu³⁺ and the energy transfer from Gd³⁺ to Eu³⁺ is meaningful to design and synthesize Gd³⁺ based compounds.     

Tunable luminescence and energy transfer process between Tb3+ and Eu3+ in GYAG:Bi3+, Tb3+, Eu3+ phosphors

A series of Eu³⁺ ions co-doped (Gd_0.9Y_0.1)₃Al₅O₁₂:Bi³⁺, Tb³⁺ (GYAG) phosphors have been synthesized by means of solvothermal reaction method. The XRD pattern of GYAG phosphor sintered at 1500 °C confirms their garnet phase. The luminescence properties of these phosphors have been explored by analyzing their excitation and emission spectra along with their decay curves. The excitation spectra of the GYAG:Bi³⁺, Tb³⁺, Eu³⁺ phosphors consists of broad bands in the shorter wavelength region due to 4f⁸ → 4f⁷5d¹ transition of Tb³⁺ ions overlapped with 6s² → 6s¹6p¹ (¹S₀ → ³P₁) transition of Bi³⁺ ions and the charge transfer band of Eu³⁺–O^2?. The present phosphors exhibit green and red colors due to ⁵D₄ → ⁷F₅ transition of Tb³⁺ ions and ⁵D₀ → ⁷F₁ transition of Eu³⁺ ions, respectively. The emission was shifted from green to red color by co-doping with Eu³⁺ ions, which indicate that the energy transfer probability from Tb³⁺ to Eu³⁺ ions are dependent strongly on the concentration of Eu³⁺ ions.     

Eu^2＋在BaF2—xYF3体系中的光谱性质及其对Tb3＋的能量传递

研究了钡钇复合氟化物体系中Ｅｕ＾２＋的光谱性质和变化规律，讨论了影响Ｅｕ＾２＋光谱的因素，特别是氧的存在对Ｅｕ＾２＋激发和发射能量的影响，发现在ＢａＹＦ５基质中Ｅｕ＾２＋对Ｔｂ＾３＋的有效参量传递。     

Luminescence of Tb3+ and Eu3+ doped amorphous zinc benzoates

The Tb(3+) and Eu(3+) doped amorphous zinc benzoate were prepared. Their infrared absorption, emission and excitation spectra were measured. The luminescence mechanisms of Tb(3+) and Eu(3+) in the amorphous substrate were discussed. The bonding modes of OCO group to Zn(2+) ion have two of symmetric and asymmetric bridging bidentate. The energy of the S(1) pi,pi* excited state of benzene ring can be transferred to Tb(3+) and Eu(3+) ion, and results in characteristic emission from the 5D(4)-->(7)F(j) of Tb(3+) and 5D(0)-->(7)F(j) of Eu(3+), respectively.     

Ca2+、La3+及Eu3+对NaDC胶团的作用

在水溶液中将脱氧胆酸钠（ＮａＤＣ）分别与ＣａＣＬ２、ＥｕＣｌ３及ＬａＣｌ３反应,改变反应物浓度和配比,合成了系列脱氧胆酸络全物。利用红外光谱（ＦＴＩＲ）、元素分析、ＩＣＰ分析及Ｘ身材线粉末衍射谱,对它们的组成和结构进行了研究。结果表明：水溶液中ＣａＣｌ２与ＮａＤＣ的反应不是简单离子间的反应,改变其反应物浓度和配比,生成组成和结构不同的络合物;而ＬｎＣｌ３与ＮａＤＣ反应时,反应物浓度和配比的改变不影     

Thermal study in Eu3+-doped boehmite nanofibers and luminescence properties of the corresponding Eu3+:Al2O3

Eu³⁺-doped boehmite nanofiber materials with different Eu³⁺ concentrations were synthesized without any surfactant, and followed by a series of characterizations. It was found that the boehmite nanofibers became coarser with the increase of Eu³⁺ concentration, which resulted in a gradual decrease of their specific surface areas. Moreover, the thermal stability of the boehmite nanofibers was studied by thermogravimetry–differential scanning calorimetry. All materials showed the phase transition from γ-Al₂O₃ to other forms. Yet the transition temperature was increased with the increase of Eu³⁺ concentration. The Eu³⁺-doped boehmite nanofibers with the maximum Eu³⁺ concentrations showed the best thermal stability. Photoluminescence spectra showed that the 2 mol% of doping concentration of Eu³⁺ ions in Eu³⁺:Al₂O₃ nanofiber was optimum.     

多孔二氧化硅中Gd3+ → Eu3+的能量传递

通过水热反应法，获得了单掺和双掺Eu³⁺，Gd³⁺的多孔二氧化硅组装体，研究了掺杂体系的光谱特性，观察到Gd³⁺ → Eu³⁺的能量传递。分析了能量传递过程，探讨了在多孔二氧化硅中Gd³⁺→Eu³⁺的能量传递的机理，其机理主要为电偶极-电偶极相互作用。     

GdF3∶Eu3+/NaGdF4∶Eu3+纳米晶的水热合成及发光性质

采用水热法,以聚乙二醇(400)为分散剂,以NaOH和HNO3溶液调节初始溶液pH值,合成GdF3∶Eu3+和NaGdF4∶Eu3+纳米晶。XRD和SEM结果表明:在酸性溶液(pH=3,5)、中性溶液(pH=7)和碱性溶液(pH=9)中,分别获得具有正交结构的GdF3∶Eu3+纳米晶,GdF3∶Eu3+和NaGdF4∶Eu3+混合晶,六方结构NaGdF4∶Eu3+棒状微米晶。根据Scherrer公式估算pH=3和pH=5时制备纳米晶的一次性粒径分别为49和28 nm。样品的发射光谱结果表明:特征发射峰来自于5D2、5D1、5D0到7FJ跃迁。在主晶相为GdF3样品中,主发射峰来自于Eu3+的5D0→7F1的磁偶极跃迁;晶相为NaGdF4样品的主发射峰来自于Eu3+的5D0→7F2电偶极跃迁。5D0→7F1和5D0→7F2跃迁发射相对强度比值显示:Eu3+在NaGdF4晶体中的格位对称性下降。激发光谱显示出Gd3+和Eu3+具有较好的能量传递。     

Eu3+/Tb3+和Eu3+/Pr3+共掺杂P(MMA-co-St)的荧光性能的研究

将不同荧光性能的铽(Tb)、镨(Pr)离子分别与铕(Eu)离子混合，以三异丙氧基稀土的形式掺杂P(MMA-CO-St)共聚物，研究Eu^3 ／Tb^3 和Eu^3 ／pr^3 共掺杂P(MMA-CO-St)的荧光性能的变化情况．结果表明，Eu^3 ／Tb^3 掺杂的P(MMA-CO-St)中，Tb^3 作为能量给予体，Eu^3 作为能量接受体，能量转移的结果使Eu^3 特征荧光显增强；Eu^3 ／pr^3 掺杂的P(MMA-CO-St)中，Eu^3 的能量向pr^3 转移，致使Eu^3 的特征荧光猝灭，pr^3 的荧光略为增强．