KZnF3：Eu的水热合成及其光谱性质

采用中温水热法合马了立方钙钛矿单相ＫＺｎＦ３及ＫＺｎＦ３：Ｅｕ，通过ＳＥＭ观察了产物形态．ＸＰＳ测定结果表明，产物含氧量不高。荧光光谱及ＥＳＲ谱表明，ＫＺｎＦ３：Ｅｕ体系中Ｅｕ＾２＋与Ｅｕ＾３＋共存，进一步讨论了不等价取代中的电荷补偿途径。     

Bi3+敏化的SrSiO3:Eu3+,Bi3+发光体的合成与发光

本文采用高温固相扩散法合成出一种新的发光体ＳｒＳｉＯ３：ｅＵ＾３＾＋，Ｂｉ＾３＾＋。研究了激活剂Ｅｕ＾３＾＋与敏化剂Ｂｉ＾３＾＋浓度变化与发光强度的关系。实验发现，组成为Ｓｒ０．８１７Ｌｉ０．０９１５ＳｉＯ３：Ｅｕ＾３＾＋０．０７５，Ｂｉ＾３＾＋的发光体其发光强度最大。给出了发光体ＳｒＳｉＯ３：Ｅｕ＾３＾＋，ＳｒＳｉＯ３：Ｅｕ＾３＾＋，Ｂｉ＾３＾＋的激发光谱与发光光谱；测定了发光体的Ｘ射线粉...     

Li_2O－Ln_2O_3－SiO_2：Eu~（3＋），Bi~（3＋）体系的结构

采用ｓｏｌ－ｇｅｌ法合成了系列发光体Ｌｉ２Ｏ－Ｌｎ２Ｏ３－ＳｉＯ２：Ｅｕ３＋，Ｂｉ３＋，并确定了发光体的物相结构．当Ｌｎ３＋＝Ｙ３＋和Ｌｎ３＋＝Ｌａ３＋时，紫外光激发下Ｅｕ３＋的发射分别以红光和橙光为主，只存在一种Ｅｕ３＋发光中心；Ｌｎ３＋＝Ｇｄ３＋时，至少存在两种Ｅｕ３＋发光中心和两种Ｂｉ３＋发光中心（共掺杂Ｅｕ３＋，Ｂｉ３＋），Ｂｉ３＋的吸收和发射所处的能量位置最低，４ｆ格位的Ｂｉ３＋发生了向Ｅｕ３＋的有效能量传递．     

（Sr，Ba）_（1－x）Eu_xTiO_3的高温高压合成及XPS研究

用高温高压法合成了Ｓｒ１－ｘＥｕｘＴｉＯ３（ｘ＝０．０，０．１，０．２，０．３，０．４，０．５）及Ｂａ０．３Ｅｕ０．７ＴｉＯ３化合物．结果表明，所有样品均为立方结构，样品中存在Ｅｕ（Ⅱ）和Ｅｕ（Ⅲ）的混合价．Ｅｕ３＋的掺入直接影响了Ｓｒ离子与氧离子的结合，使Ｓｒ３ｐ３／２的结合能随ｘ的增加而增加．     

（Sr,Ba）1—xEuxTiO3的高温高压合成及XPS研究

用高温高压法合成了Ｓｒ１－ｘＥｕｘＴｉＯ３（ｘ＝０．０，０．１，０．２，０．３，０．４，０．５）及Ｂａ０３。Ｅ０。７ＴＯ３化合物。结果表明，所有样品均为立方结构，样品中存在Ｅｕ（Ⅱ）和Ｅｕ（Ⅲ）混合价。Ｅｕ＾３＋的掺入直接影响了Ｓｒ离子与氧离子的结合。使Ｓｒ３ｐ３／２的结合能随Ｘ的增加而增加。     

化学气相色传输法分离稀土混合氧化物Sm2O3—Eu2O3—Gd2O3

以ＡｌＣｌ３为络合物配体,研究Ｓｍ２Ｏ３－Ｅｕ２Ｏ３－Ｇｄ２Ｏ３的分离特性。结果表明,其传输能力为：Ｓｍ≈Ｇｄ〉Ｅｕ,氯化物主要在９８０￣１１００Ｋ沉积。没温区的最大分离系数分别为：βＥｕ／Ｓｍ：１２００Ｋ＝１．７０,βＥｕ／Ｇｄ;１３００Ｋ＝１．８８,βＳｍ／Ｇｄ;１３００Ｋ＝１．２４,βＳｍ／Ｅｕ;８５０￣８８０Ｋ＝２．７６,βＧｄ／Ｅｕ;８８０￣９００Ｋ＝２．８３,βＧｄ／Ｓｍ;８００Ｋ＝１     

碱土金属氟化物促进Eu2O3催化剂的甲烷氧化偶联性能

考察了碱土金属氟化物促进的Ｅｕ２Ｏ３在甲烷氧化偶联反应中的催化性能。发现在Ｅｕ２Ｏ３中添加碱土金属氧化物后，碳二烃（Ｃ２）的选择性和收率都有明显提高。当Ｅｕ２Ｏ３摩尔含量相同时，催化性能按ＣａＦ２－Ｅｕ２Ｏ３＝ＢａＦ２－Ｅｕ２Ｏ３〈ＳｒＦ２－Ｅｕ２Ｏ３顺序递增，ＸＲＤ分析结果表明，在新鲜的ＢａＦ２－Ｅｕ２Ｏ３催化剂中了菱形ＥｕＯＦ新相，而在其它两类催化剂中氟氧离子交换不明显，这种差异与碱土金属氟化     

化学气相传输法分离稀土混合氧化物Sm2O3-Eu2O3-Gd2O3

以ＡｌＣｌ３ 为络合物配体, 研究Ｓｍ２Ｏ３Ｅｕ２Ｏ３Ｇｄ２Ｏ３ 的分离特性。结果表明, 其传输能力为：Ｓｍ ≈Ｇｄ＞ Ｅｕ, 氯化物主要在９８０ ～１１００ Ｋ 沉积。不同温区的最大分离系数分别为： βＥｕ／Ｓｍ;１２００ Ｋ＝ １－７０ ,βＥｕ／Ｇｄ;１３００ Ｋ＝ １－８８ , βＳｍ／Ｇｄ;１３００ Ｋ ＝ １－２４ , β′Ｓｍ／Ｅｕ;８５０ ～８８０ Ｋ＝ ２－７６ , β′Ｇｄ／Ｅｕ;８８０～９００ Ｋ ＝ ２－８３ , β′Ｇｄ／Ｓｍ;８００ Ｋ＝１－１２ , 高于传统的湿法分离系数。     

氟化镁锶中铕和铽的电荷迁移及其平衡解析

在氩气氛中，合成子ＳｒＭｇＦ４：ｘＥｕ，ｙＴｂ复合氟化物磷光体，该体系中Ｅｕ＾３＋和Ｅｕ＾２＋共存，随共掺入Ｔｂ浓度的增加，Ｅｕ＾３＋的荧光发射强度降低，Ｅｕ＾３＋的发光增强，并且Ｅｕ＾２＋的ＥＳＲ信号增强，认为Ｅｕ＾３＋和Ｔｂ３＋之间存在的电荷迁移，即Ｅｕ＾３＋Ｔｂ＾３＋→Ｅｕ＾２＋＋Ｔｂ＾４＋，通过半量手段研究了这一电荷迁移反应的平衡常数。     

Li2O-Ln2O3-SiO2:Eu3+,Bi3+体系的结构

采用ｓｏｌ－ｇｅｌ法合成了系列发光体Ｌｉ２Ｏ－Ｌｎ２Ｏ３－ＳｉＯ２：Ｅｕ＾３＾＋，Ｂｉ＾３＾＋，并确定了发光体的物相结构。当Ｌｎ＾３＾＋＝Ｙ＾３＾＋和Ｌｎ＾３＾＋＝Ｌａ＾３＾＋时，紫外光激发下Ｅｕ＾３＾＋的发射分别以红光和橙光为主，只存在一种Ｅｕ＾３＾＋发光中心；Ｌｎ＾３＾＋＝Ｇｄ＾３＾＋时，至少存在两种Ｅｕ＾３＾＋发光中心和两种Ｂｉ＾３＾＋发光中心（共掺杂Ｅｕ＾３＾＋，Ｂｉ＾３＾＋的吸收和发射所     

Role of dopant concentration and surface coating on photophysical properties of CdS: Eu3+ nanocrystals

Here, we report the role of dopant concentration and surface coating of CdS: Eu3+ nanocrystals on the modification of crystal structure and their photoluminescence properties by steady-state and time resolved fluorescence studies. It is found that photoluminescence properties are sensitive to the crystal structure which is controlled by surface coating and dopant concentration. The emission intensity of the peak at 614 nm (5D0 --> 7F2) of the Eu3+-ions is found to be sensitive to the doping and surface coating of CdS nanocrystals. It is found that the average decay times tau are 248, 353 and 499 micros for 0.25, 0.5 and 1.0 mol% Eu ions doped into CdS nanocrystals, respectively. From the decay time measurements, it is evident that the energy transfer occurs from CdS nanoparticles to Eu3+ ions and the calculated energy transfer efficiency from CdS nanoparticles to Eu3+ ions is 9.2 and 35% for Eu3+ ions coated and doped CdS nanoparticles, respectively. Our analysis suggests that site symmetry of ions plays a very important role in the modifications of radiative and nonradiative relaxation mechanisms.     

KZnF3中Ce3+→Eu2+的能量传递

研究了KZnF3中Ce3+和Eu2+的光谱特性,在共掺Ce3+和Eu2+的体系中,观察到了Ce3+对Eu2+的能量传递过程.计算了能量传递的量子效率,探讨了能量传递机理.研究发现,Ce3+的存在有利于Eu2+的f-f跃迁线状发射.     

Spectroscopic studies of the Eu3+ and Er3+ ions in the fluorozirconate LaZr2F11 matrix

An investigation by optical spectroscopy of the Eu3+ and Er3+ active ions in the crystallized fluorozirconate matrix LaZr2F11 is presented. The 5D1-->7F0-5 emission lines of Eu3+ are used to extract the 7F0-5 energy scheme and the observed extinctions permit the deduction of irreducible representations (IRREPS) associated with corresponding sub-levels in the D2 symmetry. The crystal field analysis was carried out on a 387 x 387 basis set, comprising the 7F, 5D(1,2,3) 5F(1,2), 5G(1,2,3) and 3P(1,2,3,4,5,6) terms of the Eu3+ 4f6 configuration. The deviation and rms are 6.8 and 7.9 cm(-1), respectively for 38 levels and ten parameters. The experimental crystal field parameters are in good agreement with the ab-initio ones. Moreover, the relative intensities of the 5D0-->7F2,3,4 emissions are well reproduced by an 'ab-initio' calculation, except for three lines. The Er3+ ions introduced in LaZr2F11, microcrystals also lie in an unique crystallographic site. A total of 31 energy levels were recorded and the crystal field analysis led to 6.6 and 7.8 cm(-1) for the deviation and rms, respectively, for nine variable parameters taken into account. The experimental CF parameters for Er3+ and Eu3+ are very similar, which seems to show that the host lattice contracts around the smaller Er3+ ion. The informations given by both Eu3+ and Er3+ optical probes in LaZr2F11 are very consistent with the structure previously determined for the isotypic PrZr2F11 fluoride.     

铕掺杂对纳米TiO2的光催化活性的影响

用溶胶-凝胶法制备了掺杂Eu3+的纳米TiO2,用XRD和TG-DTA对其进行了表征,并以正庚烷为气相有机污染物的实例研究了样品的光催化活性,发现Eu3+进入TiO2晶格中引起了TiO2晶格膨胀,导致晶格畸变增大,抑制了TiO2晶相的转变和粒径的增长.结果表明,Eu3+掺杂可提高TiO2的光催化活性,并且当掺杂摩尔分数为0.3%时,光催化活性最好.随着焙烧温度的升高,光催化活性下降,而利用较高的水解酸度则有利于得到光催化活性较高的样品.     

Optical properties and valence change of europium ions in a sol-gel Al2O3-B2O3-SiO2 glass by femtosecond laser pulses

The Al2O3-B2O3-SiO2 glass containing europium ions was prepared by a sol-gel method. Fluorescence line-narrowing spectra (FLN) indicate two different environments of the Eu 3+ ions. The calculated second crystal-field parameters exhibit the opposite behaviors of the two different environments. The FLN excitation and emission spectra before and after irradiation show that the change of the emission mainly comes from the Eu 3+ ions at site I, revealing that the concentration ratio of the Eu 3+ ions at site I to site II was decreased. The emission spectra confirmed that some Eu 3+ ions were reduced into Eu 2+ ions. The excitation spectra indicate that the Eu 3+ ions at the sites with higher covalence degree can be easily reduced, implying that the Eu 3+ ions are more easily reduced at site I than at site II. The absorption spectra before and after irradiation exhibit that the absorption of Eu 2+ ions increases and that the positive hole centers appear. These results suggest a mechanism of the formation of the Eu 2+ ions by femtosecond laser irradiation.     

Preparation and photoluminescence properties of Y2SiO5:Eu3+ nanocrystals

The sol-emulsion-gel method is used for the preparation of about 5-7 nm size Eu2O3 doped and coated Y2SiO5 nanoparticles at 1300 degrees C. Here, we report the role of surface coating, dopant concentration and temperature of heating on the modification of crystal structure and the photoluminescence properties of Y2SiO5:Eu3+ nanocrystals. It is found that photoluminescence properties are sensitive to the crystal structure which is again controlled by surface coating, concentration and heating temperature. The decay times are 0.76, 1.14, 1.23 and 1.40 ms for 0.25, 0.5, 1.0 and 2.5 mol% Eu2O3 doped Y2SiO5 nanocrystals prepared at 1100 degrees C (X1-Y2SiO5). However, in X2-Y2SiO5 crystal phase (at 1300 degrees C) the average decay times are 1.05, 1.35, 1.55 and 1.60 ms for 0.25, 0.5, 1.0 and 2.5 mol% Eu2O3 doped Y2SiO5 nanocrystals, indicating the photoluminescence properties depend on both the crystal structure and the concentration of ions. The emission intensity of the peak at 612 nm (5D0-->7F2) of the Eu3+-ions is found to be sensitive to the doping and surface coating of Y2SiO5 nanocrystals. The decay times are 1.55 and 1.70 ms for 1300 degrees C heated 1.0 mol% Eu2O3 doped and coated Y2SiO5 nanocrystals, respectively. Our analysis suggests that the site symmetry of ions plays a most important role in the modification of radiative relaxation mechanisms and as a result on the overall photoluminescence properties.     

Syntheses, structures and properties of seven isomorphous 1D Ln3+complexes Ln(BTA)(HCOO)(H2O)3 (H2BTA = bis(tetrazoly)amine, Ln = Pr, Gd, Eu, Tb, Dy, Er, Yb) and two 3D Ln3+ complexes Ln(HCOO)3 (Ln = Pr, Nd)

Seven isomorphous 1D chain Ln3+ complexes Ln(BTA)(HCOO)(H2O)3 (Ln = Pr (1), Gd (2), Eu (3), Tb (4) Dy (5), Er (6) and Yb (7)), and two formate coordinating and bridging 3D Ln3+ complexes Ln(HCOO)3 (Ln = Pr (8) and Nd (9)) have been synthesized and characterized by single crystal X-ray diffraction analysis. Although the Ln3+ ions in 1-7 have different radius, the trivalent lanthanide ions in 1-7 show the same coordinated environment. The well-defined single crystal structures of 8 and 9 are first samples for formate-bridged Ln3+ metallic complexes. The luminescent properties of solid samples of 2-5 at room temperature and the magnetic property of 2 have been also reported and discussed in this paper.     

Luminescence behavior of Eu3+ doped LaF3 nanoparticles

Europium-doped LaF3 nanoparticles have been prepared by the ionic reaction in the ethanol at 60 degrees C. From the XRD pattern of nanoparticles and the emission spectra of Eu3+ ions, it has been concluded that the Eu3+ ions could easily substitute the La3+ sites and the solid solution La(1-x)Eu(x)F3 can be synthesized. Due to very low phonon energies of LaF3 matrix, the 5D1 emission of Eu3+ ions in La(1-x)Eu(x)F3 nanoparticles can be observed at room temperature when doping concentration of Eu3+ ions is lower than 30 mol%. The quenching process of 5D1 emission can be attributed to cross-relaxation. Since clusters of Eu3+ ions and resonance energy transfer only occurs within one particle due to the hindrance by the particle boundary, the concentration quenching resulted from resonance energy transfer between neighboring Eu3+ ions occurs at higher Eu3+ concentrations in the Eu3+ doped LaF3 nanoparticles.     

Role of surface coating in ZrO2/Eu3+ nanocrystals

The sol-emulsion-gel method is used for the preparation of Eu3+ ion-doped and coated ZrO2 nanocrystals. Here, we report the role of surface coating, dopant concentration, and temperature of heating in the modification of their crystal structure and photoluminescence properties. It is found that the volume fraction of the tetragonal phase increases from 28.08 to 91.56% because of surface coating. This is a significant modification of the crystal phase in ZrO2 nanocrystals due to surface coating by Eu2O3. It is found that the photoluminescence properties are sensitive to the crystal structure, which is again controlled by surface coating, concentration, and heating temperature. It is found that the decay time (tau) of Eu-doped ZrO2 nanocrystals increases with increasing the concentration of dopant and with increasing the temperature of heating because of changes in their crystal phase. The emission intensity of the peak at 611-617 nm (5D0 --> 7F2) of the Eu3+ ion-activated ZrO2 nanocrystals (doped and coated) is also found to be sensitive to the nanoenvironment. The average decay times are 770 and 488 mus for 1100 degrees C-heated 1.0 mol % Eu2O3-doped and coated ZrO2 nanocrystals, respectively. Our analysis suggests that the site symmetry of the ions plays the most important role in the modifications of the radiative and nonradiative relaxation mechanisms as a result of the overall photoluminescence properties.