掺Eu3+离子Y2SiO5晶体格位选择光谱研究

分别利用白光灯、４５７－９ ｎｍ 氩离子激光、二倍频ＹＡＧ∶Ｎｄ 激光泵浦的诺丹明６Ｇ 可调谐窄线宽（０－５ ｃｍ －１） 染料激光作为光源， 以单色仪锁相放大器光电倍增管计算机数据采集系统记录光谱， 测量并研究了Ｙ２ＳｉＯ５∶Ｅｕ３ ＋ 晶体的透射光谱、荧光光谱、激发光谱和格位选择荧光光谱。５Ｄ０ →７Ｆ０，１ ，２ ，３，４ 跃迁，３０ 多根谱线（总数为５０ 根） 被观察到。在该晶体中Ｅｕ３＋ 替换Ｙ３＋ 离子， 占据两个较低对称性的光学格位， 这两个格位的５Ｄ０ ７Ｆ０ 能级跃迁谱线相隔大约只有０－２ ｎｍ ， 在室温下有一定的光谱关联。并用Ｘ射线谱对晶体的晶格常数ａ ， ｂ，ｃ 和晶面角度β进行测量， 测量结果显示掺杂后的晶格常数和未掺杂的Ｙ２ＳｉＯ５ 晶格常数基本一致。     

Li+掺杂对Y2SiO5:Pr3+上转换发光性能影响

采用溶胶-凝胶法制备Li+掺杂改性的Y2SiO5:Pr3+上转换发光材料,考察了Li+掺杂对样品晶型及发光性能的影响。采用XRD,DSC-TGA,FS对所制备的材料进行表征,结果表明Li+掺入浓度在7%～8%(摩尔分数)之间会引起Y2SiO5晶体类型由X1型转变为X2型,且Li+掺入后样品转晶型温度由950℃降至800℃;样品经800℃煅烧处理后以X1型Y2SiO5为主相,850℃煅烧处理后以X2型Y2SiO5为主相;Li+掺入同时会提高Y2SiO5:Pr3+材料的上转换发光强度,Li+最佳掺杂浓度为10%,对于双掺杂Pr3+,Li+:Y2SiO5体系中Pr3+最佳掺杂浓度为1.2%。     

Sr3SiO5∶Eu2+荧光粉的微波合成及性能研究

Silicate orange yellow phosphor used in white-light LED was prepared by microwave method. The structure and optical properties of phosphor were studied. Sr₃SiO₅∶Eu²⁺ phosphor synthesized by microwave method is tetragonal structure of Sr₃SiO₅ with uniform particle distribution. Luminescence spectrum is a broad band spectrum peaking at 575 nm. The peak of excitation is at 532 nm and phosphor can be excited by blue LED. The warm white light was obtained combined phosphor and blue LED. The CIE chromaticity coordinates and correlated color temperature of white light is (x=0.394, y=0.341) and 3 239 K respectively.     

Y2O3:Eu3+纳米线阵列的制备与表征

Y2O3:Eu3+红色荧光粉由于色纯度高、化学性质稳定和量子效率接近100%而广泛用于荧光灯和投影电视等方面.近年来,Y2O3:Eu3+的大量研究工作主要集中于纳米粉末的制备方法及其与体相材料不同的发光特性[1～3].最近,有关Y2O3:Eu3+及其稀土化合物的纳米管、纳米线和纳米带一维材料的制备成为研究热点.Wu Changfeng等[4,5]利用表面活性剂合成了Y2O3 : Eu3+纳米管.激光格位选择激发测试结果表明,Eu3+在纳米管中占据3个不同的格位,其611 nm处的红色发光峰出现了宽化.He Yu等[6]采用水热法及退火处理制备出了Y2O3:Eu3+纳米带,发现Eu3+的发射峰不仅宽化,而且出现了625 nm的新峰.Li Yadong等[7～9]采用水热法制备了稀土氧化物、硫氧化物和氢氧化物等的纳米线和纳米管,并探索了其形成机理,同时发现Y2O3S : yb3+,Er3+具有上转换的性质.     

Eu2+掺杂KCaCl3晶体的生长及发光性能

通过坩埚下降法生长出不同物质的量分数Eu²⁺掺杂的KCa_1-xEu_xCl₃(x=0.005、0.01、0.02、0.03、0.05)单晶,并对晶体进行了X射线粉末衍射、热重、透过率、光致发光光谱、衰减时间、X射线激发发射光谱等测定。通过相图及结构分析,判断出该晶体为一致熔融化合物,并得出其为正交结构,晶胞参数为a=0.75604 nm,b=1.04823 nm,c=0.72657 nm,空间群为Pnma(62)。在紫外光的激发下,晶体在434 nm左右有一个宽的发射峰,对应于Eu²⁺的4f⁶5d¹→4f⁷跃迁;光致衰减时间1.473μs,晶体在X射线激发下的发光强度随Eu²⁺离子浓度增加而增强。     

Eu2+掺杂KCaCl3晶体的生长及发光性能

通过坩埚下降法生长出不同物质的量分数Eu²⁺掺杂的KCa_1-xEu_xCl₃（x=0.005、0.01、0.02、0.03、0.05）单晶,并对晶体进行了X射线粉末衍射、热重、透过率、光致发光光谱、衰减时间、X射线激发发射光谱等测定。通过相图及结构分析,判断出该晶体为一致熔融化合物,并得出其为正交结构,晶胞参数为a=0.756 04 nm,b=1.048 23 nm,c=0.726 57 nm,空间群为Pnma（62）。在紫外光的激发下,晶体在434 nm左右有一个宽的发射峰,对应于Eu²⁺的4f⁶5d¹→4f⁷跃迁;光致衰减时间1.473 μs,晶体在X射线激发下的发光强度随Eu²⁺离子浓度增加而增强。     

一维Y2O3∶Eu3+纳米发光材料的制备与表征

One-dimensional Y₂O₃∶Eu³⁺ luminescence nanomaterials were prepared by hydrothermal method without template, and their properties were characterized. XRD patterns show that the precursors are hexagonal phase Y(OH)₃ crystals, and the samples are cubic Y₂O₃ after heat-treatment. SEM images indicate that the one-dimensional material with a diameter of 100 nm and length of micrometer scale can be obtained by this hydrothermal method. Photoluminescence properties show that the position and intensity of the precursors are different with that of the heat-treated samples resulted from the different hosts.     

KMgF3∶Ce3+，Eu2+的溶剂热合成与光谱性质

采用溶剂热法合成了Eu2 ,Ce3 单掺和双掺KMgF3.分析了样品的结构与形貌.结果表明,所合成的样品均为单相,颗粒粒度分布集中.测定了它们的激发和发射光谱,结果显示:在单掺Eu2 的KMgF3中,没有观察到位于420nm附近由微量氧色心引起的宽带发射,只发现峰值位于360 nm附近的锐峰线发射,说明溶剂热合成的KMgF3:Eu中氧含量极低;在KMgF3双掺体系中由于Eu2 和Ce3 争吸收激发能,Eu2 把能量传递给Ce3 ,存在Eu2 -Ce3 能量传递过程.观察到Ce3 的较强的发射带和Eu2 的较弱的线发射,并讨论了能量传递机理.     

静电纺丝技术制备Y2O3∶Eu3+纳米带及其发光性质

采用静电纺丝技术制备了PVP/[Y(NO₃)₃+Eu(NO₃)₃]复合纳米带,将其进行热处理,获得了Y₂O₃∶Eu³⁺纳米带。采用XRD、FTIR、SEM、TEM、荧光光谱等技术对焙烧后的样品进行了表征。结果表明：600 ℃焙烧即可获得Y₂O₃∶Eu³⁺纳米带,800 ℃时结晶更为良好,产物属于立方晶系。纳米带表面光滑,由平均直径为30 nm的小颗粒紧密排列而成,为多晶结构。随着温度升高,纳米带宽度减小。焙烧800 ℃获得的Y₂O₃∶Eu³⁺纳米带的发光性质优于焙烧600 ℃的Y₂O₃∶Eu³⁺纳米带。与体材料相比,该纳米带的激发光谱Eu³⁺-O^2-电荷迁移态(CTB)发生红移,发射光谱发生蓝移。     

水热法制备具有光滑表面的球形Y2O3∶Eu3+发光材料

The spherical Y₂O₃∶Eu³⁺ luminescent particles with size of 0.5～3 μm and smooth surface were synthesized by hydrothermal method. The resulted Y₂O₃∶Eu³⁺ precursors and the calcined particles were characterized by differential thermal analysis (DTA) and thermogravimetric (TG) analysis, X-ray diffraction (XRD), Fourier-transform IR spectroscopy (FTIR), scanning electron microscopy (SEM) and photoluminescence spectra (PL). FTIR, TG-DTA, XRD measurements show that the precursors are crystal with hydroxyl and carbonate group, and the pure cubic yttria is obtained after annealing above 700 ℃. The SEM images indicate that the Y₂O₃∶Eu³⁺ particles are in spherical shape and with smooth surface. PL analysis shows that the particles present characteristic red emission of Eu³⁺.     

Revisiting Y2Si2O7 and Y2SiO5 polymorphic structures by Y MAS-NMR spectroscopy

This paper describes the ⁸⁹Y MAS-NMR spectra for all the established polymorphs of Y₂Si₂O₇ (y, α, β, γ and δ) and Y₂SiO₅ (X1 and X2). The combination of our spectroscopic data with the structural information published up to now from diffraction data permits the revision and correction of mistakes which appear in the literature. Finally, the influence of different structural factors, such as yttrium coordination number and Y-O distances on the ⁸⁹Y NMR isotropic chemical shift is analyzed.     

不同形貌YF_3微米晶的水热合成及YF_3:Eu~(3+)荧光性质(英文)

水热条件下,Y(NO3)3·6H2O分别与K2SiF6、KPF6反应得到了不同形貌的YF3(八面体及椭球形)。以X射线光电子能谱(XPS)检测了产物的化学组成,表明产物中只含有Y和F。X射线衍射(XRD)结果表明所得的产物均为正交晶系。扫描电子显微镜(SEM)和透射电子显微镜(TEM)对产物的表征结果指明八面体形YF3棱长为200nm,而椭球形YF3是由小的纳米块自组装而成。还研究了Eu3+掺杂后YF3的荧光性质,并提出了可能的形成机理。     

Y2SiO5:Ce3+荧光体的基质多面体替换及其对发光性能的调控研究

荧光材料基质的结构调制对于调控发光材料的发光性能,探索固体结构-性能关系具有重要的研究意义。本文以Y2SiO5基质为模型,分别利用Si/Al和Si/P取代,以[AlO4]和[PO4]四面体替换[SiO4]四面体,设计合成了一系列组成为Y1.95Si1-xAlxO5-xFx∶0.05Ce3+(x=0.05,x=0.1,x=0.2,x=0.4,x=1)和Y1.95-yCaySi1-yPyO5∶0.05Ce3+(y=0,y=0.02,y=0.04,y=0.06,y=0.08,y=0.2)的荧光材料。结合X射线衍射、荧光光谱、荧光寿命等测试手段对其进行了表征分析。结果表明,在x≤0.2,y≤0.04时得到的产物能够保持Y2SiO5的结构特征,在一定的基质组成替换范围内,设计合成的样品Y1.95Si1-xAlxO5-xFx∶0.05Ce3+、Y1.95-yCaySi1-yPyO5∶0.05Ce3+能提高发光强度,发射光谱呈现蓝移现象。荧光寿命测试表明这两个系列的化合物中Ce3+所处的基质环境变化较小,Ce3+发光也未产生较大的变化。     

Low-temperature luminescence of Eu3+ in K2EuCl5

The luminescence associated with the Eu³⁺ ion in K₂EuCl₅ has been studied at cryogenic temperatures under conditions of high resolution. Emission was observed to originate from both the ⁵D₀ and ⁵D₁ excited states, and transitions to the ${}^7\text{F}{}_0\text{,}{}^7\text{F}{}_1\text{,}{}^7\text{F}{}_2\text{,}{}^7\text{F}{}_3$, and ⁷F₄ ground levels were observed. The fine structure observed within these emission bands was found to be consistent with the existence of an effective C₄ site symmetry for the emitting Eu(III) species, even though the crystal structure does not indicate the presence of a true or pseudo C₄ axis.     

YBO3：Eu中发光中心的格位与晶场拟合

通过对溶胶－凝胶法制备的YBO3：Eu的光致发射谱进行分析,证实Eu^3 可能占据两种晶场格位。并采用晶场拟合的方法定量确认这两种晶场格位的对称性分别为C3v和D3,这种指认下能级的拟合结果以及点群选择律和实验结果相当吻合。     

The Raman spectrum of tetragonal Eu3+CaF2

The Raman spectrum of a tetragonal single crystal of the compound Eu_xCa_1-(3/2)x F₂(where x = 0.002) is reported. The main features of the spectrum are the ⁷F₀ - ⁷F₁ and ⁷F₀ → ⁷F₂ electronic transitions of Eu³⁺ ions located at a site of C₂ symmetry and vibrational transitions which involve movements of the europium ion. The characteristic phonon band of cubic CaF₂ is for the rare-earth doped crystal moved to a higher frequency and the corresponding Raman tensor is that for a crystal of tetragonal symmetry.     

Eu+2 fluorescence in BaCl2

The Ba_1?xEu_xCl₂ system was studied over wide ranges of x, particularly regarding the fluorescent emission of Eu²⁺. In addition to the commonly observed 5d → 4f band emission sharp line, f → f transitions were observed. Single crystals of Eu²⁺ containing BaCl₂ were grown via the Czochralski technique and many of the optical properties, such as transmission, fluorescence, and excitation, were measured. X-ray and thermal parameters for the Ba_1?xEu_xCl₂ system are also reported.     

BaY2F8∶Ce, Eu中Ce3+→Eu2+的能量传递和Ce3+→Eu3+的电子转移

采用高温固相反应法制备了BaY