稀土萃取信息系统

应稀土化学发展的需要,我们组建了稀土萃取信息系统。其中包括:数据的来源和数据类型;数据的组织;检索功能;数据间的关联;最优化设计以及萃取剂结构与其物理性质和结构与萃取性能的相关分析研究。     

杂质离子对Y2O3:Eu3+发光性能的影响

研究了碱金属及碱土金属离子掺杂的荧光体Y2O3:Eu^3 0.05,A^ 0.02(A=Li,Na,K)和Y2O3:Eu^3 0.05,B^2 0.02(B=Mg,Ca,Sr,Ba)的荧光，余辉发光及热释光特性，余辉光谱数据表明：杂质离子掺杂的荧光体Y2O3:Eu^3 的余辉发射主峰与未掺杂荧光体Y23:Eu^3 的荧光发射主峰（611nm)一致，为经典Eu^3 的^5D0-^7F2电偶极跃迁，杂质离子的引入明显地延缓了Y2O3:Eu^3 的余辉衰减，其中Y2O3：Eu^3 ,A^ (A=Li,Na,K)的余辉衰减趋势几乎完全一致，而Y2O3：Eu^3 ,B^2 ,B2^ (B Mg,Ca,Sr,Ba）的余辉衰减趋势由慢到快依次为Ca,Sr,Ba,Mg。热释光谱数据显示，杂质离子的掺杂导致基质中电子陷阱能级的生成，这是导致余辉衰减减慢的直接原因。Y2O3：Eu^3 ,A^ 的热释峰都位于175℃左右，相应电子陷阱能级深度为0.966eV左右，而Y2O3：Eu^3 的热释峰由高到低分别位于192℃（Ca),164℃（Sr),135℃（Ba),118℃(Mg)，电子陷阱能级深度分别为1.003eV(Ca),0.942eV（Sr),0.880eV(Ba),0.843eV(Mg)。结合余辉衰减数据，可以看到，Y2O3:Eu^3 ，A^ 和Y2O3：Eu^3 ,B^2 的热释光谱与相应荧光体的余辉衰减趋势吻合得十分好，由此可以得出，一定相同的条件下，热释峰值温度越高，杂质陷阱能级越深，相应荧光体的余辉衰减越慢。     

用化学氧化法分析混合稀土中的Tb

根据 Tb在 K IQ_4—KOH—K_2S_2O_8体系中的氧化反应,建立了混和稀土中 Tb 的分光光度分析方法.Tb被氧化为 Tb~(4+),其颜色由无色转变为红棕色,最大吸收峰在420nm.Ce~(3+)加入 KIO_4—KOH 溶液后,立即被完全氧化为 Ce~(4+),Ce~(4+)在420nm 也有吸收,其干扰可以在本底中排除,其它三价稀土离子在此体系中不能发生氧化反应,故无干扰.在 Tb 的分析浓度范围为5×10~(-5)～5×10~(-4)M 时,符合 Beer 定律,Tb 在混合稀土中含量分析的最低限为1%。此方法可用于萃取稀土过程中 Tb 的分析和监控,方法简便快速。     

Luminescence Properties of Sm^3＋ doped Bi2ZnB2O7

The phosphors of （Bi1- x Smx ） 2ZnB2O7 （ x = 0. 01, 0. 03, 0. 05, 0. 07, and 0. 09） were synthesized by conventional solid state reaction. The purity of all samples was checked by X-ray powder diffraction （XRD）. XRD analysis shows that all these compounds are of a single phase of Bi2ZnB2O7, indicating that the Bi^3＋ in Bi2ZnB2O7 can be partly replaced by the Sm^3＋ without the change of crystal structure. The excitation and emission spectra at room temperature show the typical 4f-4f transitions of Sm^3＋ . The dominant excitation line is around 404 nm due to ^6H5/2→^4K11/2 and the emission spectrum consists of a series of lines at 563, 599, 646, and 704 nm due to ^4G5/2→^6H5/2, ^6H7/2, ^6H9/2, and ^6H11/2, respectively. The optimal concentration of Sm^3＋ in Bi2ZnB2O7 is about 3mol% （relative to lmol Bi^3＋ ） and the critical distance Rc was calculated as 2.1 nm. The temperature dependence of the emission intensity of Bi1.94Sm0.06ZnB2O7 was examined in the temperature range between 100 and 450 K. The quenching temperature where the intensity has dropped to half of the initial intensity is 280 K. The lifetime for Sm^3＋ in Bi1.94Sm0.06ZnB2O7 is fitted as a value of 0.29 and 1.03 ms.     

国家中长期科学和技术发展规划纲要中与稀土有关部分的思考——稀土发光材料部分

在纲要的重点领域及其优先主题的第（31）：基础原材料内，明确提出了要重点研究开发满足国民经济基础产业发展需求的稀土材料。     

Low Temperature Preparation of Ceria Solid Solutions Doubly Doped with Rare-Earth and Alkali-Earth and Their Properties as Solid Oxide Fuel Cells

Solidoxidefuelcells (SOFCs)haveseveraldis tinctadvantages ,e .g .,highenergyconversioneffi ciency ,wideadaptabilitytofuels ,theusageofnon preciousmaterials ,noliquids ,nocorrosions ,modularconstructionandmuchlowerproductionofNOx,SOxandnoise .Therefore ,theyreceiveincreasingatten tion[1,2 ] .AtypicalSOFCwhichutilizesyttria stabi lizedzirconia (YSZ)astheelectrolyterequireshighoperationtemperaturesuchas 10 0 0℃togainhighe noughionicconductivity .Loweringtheoperationtem peratureto 80 0℃wou…     

Study on Spectra of La_2CaB_(10)O_(19)∶Eu~(3 ) in VUV-VIS Range

Manyboratesareexcellenthostsforrareearthlu minescence ,forexample ,nowbestredphosphorinplasmadisplaypanel (PDP )is (Y1-xGdx)BO3∶Eu[1] .Boratephosphorsdopedwithrareearthionshavebeenrichlystudiedinthepastfewdecades[2 ,3] .RecentlyWuYichengetal .[4 ] synthesizedanewbo rateLa2 CaB10 O19,whichispotentialnonlinearopticalmaterials.InthisworkweselectedLa2 CaB10 O19ashostofluminescencematerialsbecauseitprobablyisabetterhostforrareearthluminescence .Duetotherequirementofplasmadisplaypenal(PDP)…     

Er~(3+)离子及ErP_5O_(14)晶体的光谱性质

根据ErP_5O_(14)的吸收和荧光光谱,用Judd—Ofelt理论计算了在此晶体中Er~(3+)的强度参数Ω_λ(或τ_λ),由此计算了激光能级辐射跃迁速率、辐射寿命、荧光分支比和积分发射截面等光谱参数。提出了在Peap与强度参数的总和之间存在直线关系的经验公式。讨论了ErP_5O_(14)作为激光材料的可能性。     

Development of Doped Lanthanum Gallate Solid Electrolytes

Development of the doped lanthanum gallate solid electrolytes in the recent years was reviewed. The structure and oxygen ion transference mechanism were discussed. Effects of alkali earths, transition metals, and impurities on electrical conductivity of the doped lanthanum gallates were also discussed. The applications of doped lanthanum gallate were described. The current problems and corresponding strategies were explored.