纳米晶Y_2O_2S∶Eu~(3+),Mg~(2+),Ti~(4+)长余辉发光材料的制备

采用溶剂热-高温固相法,合成了纳米晶Y2O2S∶Eu3+,Mg2+,Ti4+红色长余辉发光材料。通过XRD、TEM、荧光光谱对其进行表征。X射线衍射测试表明所制备的Y2O2S∶Eu3+,Mg2+,Ti4+纳米材料为单相,六方晶。透射电子显微镜(TEM)测试表明所制备的Y2O2S∶Eu3+,Mg2+,Ti4+纳米材料粒径小,分布集中。激发和发射光谱测试表明Eu3+离子能有效地掺入硫氧化钇基质中,并具有良好的发光性能。余辉测试表明其余辉颜色为红色,具有良好的余辉效果。     

Eu3+掺杂β-NaYF4∶20%Yb3+, 0.5%Tm3+的合成与双频光转换性能

采用高温溶剂热法合成了Eu3+掺杂的双频转换发光材料β-NaYF4∶20%Yb3+,0.5%Tm3+,并使用X射线衍射仪(XRD)、场发射扫描电镜(FESEM)和光致发光谱(PL)仪对所制备样品的物相结构、形貌特征和发光性质进行了表征,通过分析发光原理,解释了上、下转换发光的竞争机制,并探讨了稀土离子Tm3+与Eu3+之间的能量转移。结果表明:所合成的β-NaYF4∶20%Yb3+,0.5%Tm3+,xEu3+为纯六方相晶体,结晶良好,颗粒尺寸在200nm左右。改变Eu3+的掺杂浓度后晶格结构没有发生明显变化,样品可在394nm和980nm光的激发下,分别发生下转换和上转换发光。     

Eu2+、Dy3+、Li+共掺杂CaSi2O2N2荧光粉的发光性能

采用高温固相反应法制备了一系列白光LED用CaSi2O2N2:0.05Eu2+,xDy3+,xLi+(0≤x≤0.03)荧光粉.利用X射线衍射仪对样品的物相结构进行了分析,结果表明:Dy3+和Li+离子的掺入没有改变CaSi2O2N2:Eu2+荧光粉的主晶相.利用荧光光谱仪对样品的发光性能进行了测试,发现所有样品的激发光谱均覆盖了从近紫外到蓝光的较宽范围,400 nm激发下得到的发射光谱为宽波段的单峰,峰值位于545 nm左右,是Eu2+离子5d-4f电子跃迁引起的.Dy3+离子掺杂可以提高CaSi2O2N2:Eu2+荧光粉的发光强度,Dy3+与Li+共掺杂可进一步提高荧光粉的发光强度,当Dy3+和Li+的掺杂量为1mol%时,荧光粉的发光强度达到最大值,是单掺杂Eu2+的荧光粉发光强度的157%.     

SrAl2O4:Eu2+,Dy3+荧光粉复合硫磷酸盐玻璃制备及其发光性能

用二次熔融法制备了SrAl2O4∶Eu2+,Dy3+荧光粉掺杂低熔点硫磷酸盐的发光玻璃复合材料。采用DSC、透射光谱、XRD、发射光谱、SEM等测试手段对样品进行了表征。研究了熔制温度、熔制时间等因素对复合材料光学性能的影响。结果表明:熔制温度为700℃、熔制时间为30min的发光玻璃复合材料在365nm紫外光激发下,发射出峰值波长为514nm的黄绿光,保留了荧光粉的发光性能。     

Eu3+掺杂Bi4Si3O12材料的制备和发光特性（英文）

采用传统的固相合成法制备了Eu3+掺杂的Bi4Si3O12发光材料.使用X射线粉末衍射技术对制备的发光粉体进行了表征.Eu3+掺杂的Bi4Si3O12材料的激发谱表明,在265 nm处强而宽的谱带对应于Eu3+→O2-之间的电荷转移跃迁带.在用紫外光激发的荧光光谱中,Eu3+掺杂的Bi4Si3O12材料在614 nm处有强的红光发射.材料的激发和发射光谱结果表明,Eu3+掺杂的Bi4Si3O12有望做为红色固体发光的候选材料.     

白光LED用MSrAl3O7:Eu2+(M=Y,La,Gd)绿色发光材料合成及其光学性能

采用传统的高温固相合成技术制备出一系列组成为MSrAl3O7:Eu2+(M=Y,La,Gd)的新型绿色发射荧光体.通过X射线衍射(XRD)研究其晶体结构发现:MSrAl3O7:Eu2+系列荧光体属于M2O3-SrO-Al2O3赝三元体系的稳定结晶相.荧光光谱测试表明:MSrAl3O7:Eu3+(M=Y、La、Gd)材料均是优良的白光LED用绿色荧光体,可被近紫外(300～450nm)有效激发,产生较强的绿色发射光,发射主峰位于517nm左右,样品的紫外-可见(UV-vis)光谱进一步证实了其有效吸收近紫外光的特征.研究还发现,在MSrAl3O7:Eu2+(M=Y、La、Gd)系列荧光体中,LaSrAl3O7:Eu2+具有最强的绿色发射光,进一步地比较不同温度下LaSrAl3O7:Eu2+材料的结构与光谱特性表明,1400℃合成的样品具有稳定的结构和最佳的发光性能.     

SrAl2O4:Eu2+,Dy3+发光粉体的长余辉特性研究

采用高温固相合成法制得了SrAl_2O_4:Eu~（2+）,Dy~（3+）长余辉发光材料.X射线衍射分析(XRD)结果表明:该磷光体为SrAl2O4晶体结构,属单斜晶系.其晶格常数为:a=8.4424A,b=8.822A,c=5.1607A,β=93.415°.SrAl2O4:Eu2+,Dy3+发光材料的激发光谱和发射光谱均为宽带谱,激发谱峰位在300～450nm,发射光谱的峰值波长在518nm处.这一结果表明该材料的发光是由Eu2+的4f65d→4f7(8S7/2)宽带跃迁产生的.其余辉衰减由初始的快衰减和其后的慢衰减所组成.通过热释光谱对材料中的陷阱能级进行了分析,该材料中存在两个较深的陷阱能细。苴深度分别为0.38和1.34eV.     

红色荧光粉Ca3Y2Si3O12∶Pr3+的制备及发光特性

通过高温固相方法合成了红色荧光粉Ca3Y2Si3O12∶Pr3+,研究了Pr3+掺杂浓度及助熔剂对荧光粉发光性能的影响。结果显示,所合成的荧光粉的主晶相为Ca3Y2Si3O12。通过分析荧光光谱,发现Ca3Y2Si3O12∶Pr3+硅酸盐荧光粉的有效激发范围可以在430~490nm范围内,并发射红光。在445nm激发下,样品发射光谱中的主发射峰分别位于610nm(3P0→3 H6)和644nm(3P0→3F2),其中610nm处峰值最大。通过改变Pr3+掺杂浓度,发现荧光粉发光强度先增大后减小,最佳Pr3+掺杂量x(Pr3+)为2.0%,超过最佳掺杂浓度表现为由离子间的相互作用导致的浓度淬灭。该荧光粉色温为2261℃。通过观察助熔剂的助熔效果,发现最佳的助熔剂H3BO3添加量为2.0%。     

Ba2Gd2Si4O13∶Dy3+发光性能研究

通过高温固相反应制备Ba2Gd2Si4O13∶Dy3+发光材料,利用XRD、FTIR、SEM、XPS和激发-发射光谱表征合成样品的性能。研究表明,使用Li2CO3-NH4F复合助熔剂,形成了长柱状形貌。在349nm或274nm激发下,Ba2Gd2Si4O13∶Dy3+发出Dy3+特征峰,色坐标接近白光区域。Gd3+→Dy3+的能量传递增强了Dy3+发光强度。Dy3+最优的掺杂浓度为2%,临界传输距离为30。Ba2Gd2Si4O13∶Dy3+发光材料可作为潜在的单一掺杂单一组成的白光LED发光材料。     

热分解法合成Y2O3∶Eu3+纳米球及红色荧光性质研究

用热分解法在油酸和油胺混合溶剂中,320℃条件下,反应3h,成功制备了Y2O3:Eu3+纳米球。透射显微镜(SEM)和X粉末衍射仪(XRD)表征结果表明,成功合成了尺寸大约为15nm的Y2O3:Eu3+纳米球,JCPDS号为82-2415。且在紫外灯照射下,溶解于环己烷中的Y2O3:Eu3+纳米晶发射出比较强的红光,从荧光发射光谱上发现,发射峰的位置为594nm、614nm、628nm和709nm,分别对应Eu3+离子的5 D0→7F1,5 D0→7F2和5 D0→7F4跃迁。     

改性沸石对电镀废水中Pb2+、Zn2+、Ni2+的吸附

将天然沸石进行处理制备出多孔质改性沸石颗粒。在静态条件下，研究了改性沸石颗粒对重金属离子Pb^2 ,Zn^2 ,Ni^2 的吸附效果及条件，含Pb^2 ,Zn^2 ,Ni^2 的电镀废水经改性沸石颗粒吸附后，废水中Pb^2 ,Zn^2 ,Ni^2 的含量低于国家排放标准。     

NpO 2 + -UO 2 2+ cation-cation interaction in NaCl-KCl-CsCl and LiCl-KCl-CsCl eutectic melts

Absorption spectra of the NpO ₂ ⁺ ion in UO ₂ ²⁺ -containing NaCl-KCl-CsCl (0.300:0.245:0.455) and LiCl-KCl-CsCl (0.575:0.165:0.260) eutectic melts in the region of the 5f-5f transitions, 700–2000 nm, were studied at 650 and 500°C, respectively. Processing of the spectra allowed the previously discovered phenomenon, cation-cation interaction of actinides in melts, to be interpreted for the first time in terms of the mass action law. It was shown that, at the concentrations of the interacting components studied (C _Np = 0.2 M and C _U = 0.1–2 M), a 1: 1 NpO ₂ ⁺ ·UO ₂ ²⁺ cation-cation complex is formed. Its concentration stability constant was estimated at 0.06(6) and 0.11 1 mol^?1 for the NaCl-KCl-CsCl and LiCl-KCl-CsCl systems, respectively.     

胶团强化超滤中SDS胶团对Cd^2＋，Zn^2＋和Pb^2＋的竞争吸附

胶团强化超滤法是一种将表面活性剂技术和超滤技术结合的新型、高效的重金属废水治理方法.以十二烷基硫酸钠(SDS)为表面活性剂,对含单一镉、锌、铅溶质以及混合溶质体系进行了胶团强化超滤研究,考察了胶团对Cd2 ,Zn2 ,Pb2 的竞争吸附性能.研究发现,当溶液中多种二价重金属离子存在时,各离子之间存在与SDS胶团的竞争吸附,竞争能力为Pb2 ＞Zn2 ＞Cd2 ;Cd-Zn有明显的协同吸附效应,而Cd-Pb,Zn-Pb则表现为拮抗吸附.     

On the Eu2+-Mn2+ energy transfer in BaMgF4

Energy transfer from Eu²⁺ to Mn²⁺ ions is shown to occur in BaMgF₄ : Eu, Mn crystals. The efficiency of this transfer is moderate. This is attributed to the fact that Eu²⁺ and Mn²⁺ ions are distributed randomly in the host lattice. Quantitative evaluation leads to the suggestion that the transfer is restricted to only seven neighbors at 4.0 Å and is thus exchange mediated.     

Observable effects of Ca2+ buffers on local Ca2+ signals

Calcium signals participate in a large variety of physiological processes. In many instances, they involve calcium entry through inositol 1,4,5-trisphosphate (IP(3)) receptors (IP(3)Rs), which are usually organized in clusters. Recent high-resolution optical experiments by Smith & Parker have provided new information on Ca(2+) release from clustered IP(3)Rs. In the present paper, we use the model recently introduced by Solovey & Ponce Dawson to determine how the distribution of the number of IP(3)Rs that become open during a localized release event may change by the presence of Ca(2+) buffers, substances that react with Ca(2+), altering its concentration and transport properties. We then discuss how buffer properties could be extracted from the observation of local signals.     

ESR of Cu2+and Tl2+ in thallium borate glasses

The electron spin resonance (ESR) and optical absorption spectra of Cu²⁺ were measured in thallium borate glasses in order to investigate the effects of glass transition temperature,T _g, upon the responses of cupric ion in alkali borate glasses. The ESR of Tl²⁺ induced by-ray irradiation was also obtained. An abrupt increase in the covalency of in-plane Cu²⁺-O-bonding was observed in the Tl₂O system as well as in the Na₂O system in a similar B₂O₃ composition range althoughT _g for the Tl₂O glasses has little dependency on the composition compared with the Na₂O glasses. The trend in the variation of the S-character of the Tl²⁺ unpaired electron with composition agreed with that of the covalency of in-plane Cu²⁺-O-bonding. The structure of the anion group present in Tl₂O glasses was also examined by laser reman spectroscopy.     

酸改性膨润土吸附去除镍镉离子的研究

在静态条件下,研究了改性膨润土对重金属离子的吸附性能和吸附机理,着重探讨了改性膨润土去除模拟水样中重金属离子Ni2 ,Cd2 的适宜条件及改性膨润土的再生方法.结果表明,改性膨润土对Ni2 ,Cd2 具有较好的吸附性能;pH值是影响改性膨润土对重金属离子吸附的重要因素,不同的金属离子都有其适宜的pH值范围.吸附的最佳条件是pH值5.0～7.0,废水中Ni2 ,Cd2 含量不大于45 mg/L,搅拌时间约60 min.利用改性膨润土吸附处理Ni2 ,Cd2 含量小于45 mg/L的模拟水样,效果很好,Ni2 ,Cd2 的去除率均可分别达到98.5%以上,出水可达到国家排放标准.     

锰矿尾渣对Cu2+和Ni2+的吸附性能研究

研究了锰矿尾渣对重金属离子Cu2 和Ni2 的吸附性能,分析了锰矿尾渣的吸附动力学,就吸附时间、Cu2 和Ni2 浓度及pH值等因素对锰矿尾渣吸附性能的影响作了系统考察,并对锰矿尾渣的吸附机理进行了初步探讨.结果表明,在温度为25°℃、pH值为7.5的条件下,锰矿尾渣对Cu2 和Ni2 的吸附容量可达到1.6 mg/g以上,去除率均可达到97.5%以上,适宜于处理含低浓度Cu2 或Ni2 的废水.锰矿尾渣的吸附机理为离子交换吸附和表面配位吸附.     

Characterization of various Eu2+ sites in Ca2SiO4:Eu2+ and Ba2SiO4:Eu2+ by high-pressure spectroscopy

Photoluminescence of Ba₂SiO₄ and Ca₂SiO₄ activated with Eu²⁺ was investigated at various temperatures (from 10 K to 300 K) and pressures (from ambient to 200 kbar). At ambient pressure and room temperature, under UV excitation both phosphors yielded a green emission band with maxima at 505 nm and 510 nm for Ba₂SiO₄ and Ca₂SiO₄, respectively. The energies of these bands depended on pressure; the pressure shifts were ?12:55 cm^?1/kbar for Ba₂SiO₄:Eu²⁺; and ?5:59 cm^?1/kbar for Ca₂SiO₄:Eu²⁺. In the case of Ca₂SiO₄:Eu²⁺, we observed additional broadband emission at lower energies with a maximum at 610 nm (orange band). The orange and green emission in Ca₂SiO₄:Eu²⁺ had different excitation spectra: the green band could be excited at wavelengths shorter than 470 nm, whereas the orange band — at wavelengths shorter than 520 nm. The pressure caused a red shift of orange emission of 7.83 cm^?1/kbar. The emission peaked at 510 nm was attributed to the 4f⁶5d→4f⁷(⁸S₇₌₂) transition of Eu²⁺ in the β — Ca₂SiO₄:Eu²⁺ phase, whereas the emission peaked at 610 nm — to the γ — Ca₂SiO₄:Eu²⁺ phase. The emission of Ba₂SiO₄:Eu²⁺ peaked at 505 nm was attributed to the 4f⁶5d→ 4f⁷(⁸S_7/2) transition of Eu²⁺ in the β — Ba₂SiO₄ phase.