高温高压合成的硅酸锶有铕铋的发光特性

用高温高压方法合成了Ｓｒ２ＳｉＯ４Ｅ＾３＋ｕ，Ｂｉ＾３＋和ＳｒＳｉＯ３Ｅｕ＾３＋＿，Ｂｉ＾３＋，研究了合成压力对其发光性能的影响，与用溶胶－凝胶共沉淀法和常压高温法合成的产品作比较，常压制备的ＳｒＳｉＯ３Ｅｕ＾３＋，Ｂｉ＾３＋为六角结构，而在２．３４－４．１０ＧＰａ的合成压力范围内，它转变为赝正交结构；常压下Ｓｒ２ＳｉＯ４；Ｅｕ＾３＋，Ｂｉ＾３＋，为单斜结构，在４．２ＧＰａ的合成压力下，未发现其结     

（Y，Zn，Sr）_3（P，VO_4）_2：Eu~（3＋），Bi~（3＋）发光性

合成了组成为（Ｙ，Ｚｎ，Ｓｒ）３（Ｐ，ＶＯ４）２：Ｅｕ３＋，Ｂｉ３＋的荧光材料，经射线结构分析确定为Ｚｎ３（ＰＯ４）２结构，属于单斜晶系，空间群为Ｐ２１／ｎ讨论了基质组成对Ｅｕ３＋离子发光性质的影响，用Ｙ３＋取代了一部分Ｚｎ２＋，用ＶＯ取代了一部分ＰＯ．由于基质的４３６ｎｍ发射与Ｅｕ３＋的激发态能级的能量重叠，Ｅｕ３＋产生较强的５９８ｎｍ和６１８ｎｍ发射．另外，掺入少量Ｂｉ３＋能增强Ｅｕ３＋发射．     

（Y,Zn,Sr）3（P,VO4）：Eu^3＋,Bi^3＋发光性质的研究

合成了组成为（Ｙ，Ｚｎ，Ｓｒ）３（Ｐ，ＶＯ４）：Ｅｕ＾３＋，Ｂｉ＾３＋的荧光材料，经Ｘ射线结构分析确定为Ｚｎ３（ＰＯ４）２结构，属于单斜晶系，空间群为Ｐ２１／ｎ。讨论了基质组成对Ｅｕ＾３＋离子发光性质的影响，用Ｙ＾３＋取代了一部分Ｚｎ＾２＋；用ＶＯ４取代了一部分ＰＯ４由于基质的４３６ｎｍ发射与Ｅｕ＾３＋的激发态能级的能量重叠，Ｅｕ＾３＋产生较强的５９８ｎｍ和６１８ｎｍ发射。另外，掺入少量Ｂｉ＾３＋     

用溶胶—凝胶法制备的Y2SiO5：Gd,Eu荧光粉的发光性能

用溶胶－凝胶法合成了Ｙ２ＳｉＯ５：Ｇｄ,Ｅｕ红色荧光粉。探讨了烧结工艺对粉体的结构及发光性能的影响。首次报道了搀杂Ｇｄ的Ｙ２ＳｉＯ５：Ｅｕ红色荧光粉的发光性能。研究结果表明,搀杂适当浓度的Ｇｄ,可以显著提高ＹｓＳｉＯ５：Ｅｕ红色荧光粉的发光强度,在Ｙ２ＳｉＯ５基质中,Ｇｄ＾３＋是Ｅｕ＾３＋的优良敏化剂。     

PbO－Bi_2O_3－B_2O_3－SiO_2系重金属氧化物玻璃的结构与光学性

通过密度、可见光光谱、红外吸收光谱、Ｃｏ－６０辐照损伤试验及荧光光谱的测试，研究了ＰｂＯ－Ｂｉ２Ｏ３－Ｂ２Ｏ３－ＳｉＯ２玻璃系的光学性能与结构．密度最高可达８．４６４ｇ／ｃｍ３其紫外吸收达截止波长随Ｐｂ２＋及Ｂｉ３＋含量升高而红移．玻璃熔化温度低达８５０℃．在ＰｂＯ－Ｂｉ２Ｏ３－Ｂ２Ｏ３系玻璃中加人ＳｉＯ２可使玻璃结构更致密．室温下该系统玻璃在３６０ｎｍ有一个宽的激发峰，能产生４１８ｕｍ及４３８ｕｍ两个弱的发射峰．该系统玻璃的结构是由［ＳｉＯ４］４－、［ＢＯ３］３－、［ＢＯ４］５－、［ＰｂＯ４］６－及［ＢｉＯ６］９－构成．其中部分Ｐｂ２＋及Ｂｉ３＋以网络外体进入玻璃．     

发光陶瓷釉面砖的研制

文章介绍了一种新型的以ＳｒＡｌ２Ｏ４：Ｅｕ＾２＋Ｄｙ＾３＋为发光材料的发光陶瓷釉面砖及其制备工艺。产品的性能满足国家ＧＢ／Ｔ４１００－９２标准，发光釉面砖在暗的环境中８小时内能起到明显的标识作用。     

纳米Y2O3:Eu3+粉体的表面包膜处理

本文采用高分子网络凝胶法制备了粒径约为２０ｍｍ的纳米Ｙ２Ｏ３：Ｅｕ＾３＋粉体,并采用ＫＡｌ（ＳＯ４）２及Ｎａ２ＳｉＯ３溶液进行表面包膜处理。     

稀土正硼酸盐Ln_(1-x)BO_3:Eu_x(Ln=Y,Gd)的结构与发光特性

用溶胶－凝胶法和高温固相反应分别制备了纳米量级和常规尺度的稀土正硼酸盐荧光粉ＬｎＢＯ３：Ｅｕ（Ｌｎ＝Ｙ,Ｇｄ）,测量了它们的激发光谱并首次观察到了ＹＢＯ３：Ｅｕ中Ｅｕ３＋的７Ｆ０→５Ｄ０跃迁的 Ｎｅｐｈｅｌａｕｘｅｔｉｃ效应．根据低温下的激发光谱,发射光谱以及变温条件对发光光谱的影响,ＹＢＯ３中Ｌｎ３＋所占据的两种格位的对称性被修正为Ｃ３和Ｄ３在不同方法制备的样品中观察到了不同的发光强度和猝灭浓度,缺陷的影响是产生这种不同的原因,退火样品的发光和拉曼散射谱的变化反映出掺杂的杂质Ｅｕ３＋的团聚化是可能的缺陷来源．     

微波快速合成硫化锶铜铋磷光体及Bi3+对Cu+的敏化发光

本文首次采用微波辐射法快速合成了以ＳｒＳ为基质,Ｃｕ、Ｂｉ＾３＋为共激活剂的箍余辉蓝绿色光致发光磷不体,其激发和发射主峰波长分别为２６７和５２１ｎｍ,工余辉时间约为０．５ｈ。系统考察了在单掺杂和双掺杂情况下的发光规律,发现Ｂｉ＾３＋与Ｃｕ＋之间存在着能量传递作用,且Ｂｉ＾３＋对Ｃｕ＾＋具有很强的敏化和猝灭效应。     

P2O3—B2O3—Al2O3—SrO—BaO玻璃中的Yb^3＋非辐射能量转移下E …

本文研究了共掺Ｅｒ＾３＋／Ｙｂ＾３Ｐ２Ｏ３－Ｂ２Ｏ３－Ａｌ２Ｏ３－ＳｒＯ－ＢａＯ玻璃的能量转移过程。实验中制备了高掺杂Ｂｂ＾３＋离子的双掺Ｅｒ＾＃＋／Ｙｂ＆＾３＋的磷酸盐玻璃样品。在Ｅｒ＾３＋／Ｙｂ＾３＋掺杂比率〉１：１８（ｍｏｌ％）时,观测到了基于Ｙｂ＾３＋离子至Ｅｒ＾３＋离子能量转移下Ｅｒ＾３＋（＾３Ｉ１３／２→＾４Ｉ１５／２）的增强发射和ｂ＾３＋（＾２Ｆ７１／→＾２Ｆ５／２）发射的减弱,当Ｂ     

近紫外白光LED用红色荧光粉In2（MoO4）3:Eu3+,Bi3+的合成及发光性能

通过固相反应法在1000℃空气气氛中合成了In2(MoO4)3:Eu3+、Bi 3+红色荧光粉。粉体分别用X射线衍射(XRD)、荧光分度计测试。结果表明制备的荧光粉具有单相立方晶体结构,该荧光粉能够被近紫外光(395nm)有效激发,发射高强度的612nm红光。Eu3+浓度为40%(摩尔分数)时,In2(MoO4)3:Eu3+发光强度较高。In2(MoO4)3:0.4Eu3+、Bi 3+荧光粉,Bi 3+浓度为3%(摩尔分数)时,发光强度最大,高于没有掺Bi 3+的In2(MoO4)3:0.4Eu3+荧光粉。和CaMoO4:Eu3+相比,In2(MoO4)3:0.4Eu3+、0.03Bi 3+有较高的发光强度。因此,In2(MoO4)3:0.4Eu3+、0.03Bi 3+是一种可能应用于近紫外白光LED的新型红色荧光粉。     

High pressure luminescence and Raman studies on the phase transition of Gd2O3:Eu3+ nanorods

The cubic Gd2O3:Eu3+ nanorods were synthesized by a hydrothermal method. The SEM image indicated the nanorods with diameter of 30-35 nm and length of 200-500 nm. The structural stability of Gd2O3:Eu3+ nanorods was investigated by in situ high pressure luminescence and Raman spectra up to 18.9 GPa at room temperature. The results reveals a pressure-induced phase transition from cubic to hexagonal structure at about 11.3 GPa. After releasing pressure, the part of hexagonal structure is retained and the other transfers to monoclinic phase.     

Synthesis and luminescence properties of Sr2SiO4: Eu3+, Dy3+ phosphors by the sol-gel method

The Sr2SiO4:Eu3+, Dy3+ phosphors for white light emitting diodes (LEDs) were synthesized by the sol-gel method. The microstructure and luminescent properties of the obtained Sr2SiO4:Eu3+, Dy3+ particles were well characterized. The results demonstrate that the Sr2SiO4:Eu3+, Dy3+ particles, which have spherical morphology, emitted an intensive white light emission under excitation at 386 nm. The phosphors show three emission peaks: the blue emission at 486 nm corresponding to the 4F(9/2)-6H(15/2) transition of Dy3+, the yellow emission at 575 nm corresponding to the 4F(9/2)-6H(13/2) transition of Dy3+, and the red emission at 615 nm corresponding to the 5D0-7F2 transition of Eu3+. At the same time, the effect of Eu3+ concentration on the emission intensities of Sr2SiO4:Eu3+, Dy3+ was investigated in detail. The phosphors used for white LEDs were obtained by combining near ultraviolet (NUV) light (386 nm) with Sr2SiO4:0.04Dy3+, 0.01Eu3+ phosphors with the characteristic of Commission Internationale de l'Eclairage (CIE) chromaticity coordinate (x, y) of (0.33, 0.34), and color temperature Tc of 5,603 K. In addition, the effect of the charge compensators (Li+, Na+, and K+ ions) on the photoluminescence (PL) emission intensities were studied.     

Pressure effect on optical properties and structure stability of LaPO4:Eu(3+) microspheres

Uniform monoclinic core-shell and hexagonal urchin-like LaPO4:Eu(3+) spheres are synthesized via an attractive hydrothermal method owing to the higher yield and simplicity. Photoluminescence and Raman spectra of two samples have been investigated under high pressure up to 28 GPa using diamond anvil cells. At ambient pressure, both samples exhibit same luminescent properties with that of bulk monazite LaPO4:Eu(3+). With the increase of pressure, the emission intensity of Eu(3+) decreases and the half-widths of transition lines increase for both samples, while emission peaks show a red shift toward longer wavelengths due to increase in both the crystal-field strength and the covalency. Monoclinic core-shell LaPO4:Eu(3+) becomes amorphous finally while hexagonal urchin-like one transforms to monoclinic structure at lower pressure of 3.2 GPa and turns into amorphous structure at higher pressures, which are presented based on the analysis of high pressure Raman spectra.     

Structural transition in nanostructured Eu2O3 under high pressures

We report here studies on the effect of high pressure on the structural properties of nano-sized Europium sesquioxide (Eu2O3) up to a pressure of about 16.4 GPa. At ambient conditions, the starting sample was found to be predominantly cubic type Eu2O3 or in Eu3+ state with a trace of Eu2+. The presence of Eu2+ state is assumed to be arising due to the non-stoichiometric Eu(1-x)O phase which is obtained from XPS studies by the deconvolution of the Eu 3d-core levels. The Raman studies at ambient show a strong peak at about 333 cm(-1), which is known to occur due to the Fg mode of cubic Eu2O3 and in a similar way, the XRD data shows major peaks corresponding to the cubic phase of Eu2O3. A Mao-Bell type diamond anvil cell (DAC) was used to generate high pressures for XRD and Raman spectroscopy studies. It was observed that the material undergoes a structural change from cubic to monoclinic structure with an on set transition pressure at around 2 GPa and completes at around 8 GPa. This has been inferred from the fact that above about 2.0 GPa pressure, Raman studies show the emergence of a new peak corresponding to the monoclinic phase which increases in intensity and shifts further with increase in pressure, while the XRD studies show that above about 2.0 GPa, the peaks corresponding to monoclinic phase emerge, which show a slight increase in preferred orientation as the pressure is increased. A detailed discussion has been provided to explain this fact.     

非硅醇盐无机溶胶凝胶法合成蓝色发光材料Sr_2MgSi_2O_7:Eu~(2+),Dy~(3+)

以水玻璃(Na2SiO3)为硅源,柠檬酸三铵为PH值调节剂,通过离子交换,采用溶胶凝胶法低温合成Sr2MgSi2O7Eu2+,Dy3+蓝色发光材料。采用DTA、XRD、荧光光谱等手段对材料进行分析和表征,结果表明:前驱体干凝胶煅烧到1010℃后开始有Sr2MgSi2O7相形成,到1100℃完全转变成高纯相Sr2MgSi2O7,其产物疏松,颗粒小,不需研磨或稍加研磨便得超细粉。它的激发光谱在250～450nm之间存在一个强度较高的激发带,发射峰位于467nm,余辉时间超8h。此外,对溶胶凝胶的形成机理等进行了讨论。     

煅烧温度对红色长余辉发光材料Sr_3Al_2O_6:Eu~(2+),Dy~(3+)性能的影响

采用溶胶凝胶法合成了Sr3Al2O6:Eu2+,Dy3+长余辉发光材料,利用X射线衍射仪(XRD)对材料的物相进行了分析,采用荧光分光光度计、照度计测定了样品的发光特性。XRD结果表明:随着煅烧温度的升高,SrCO3杂相的衍射峰越来越弱,Sr3Al2O6相的衍射峰越来越强,1200℃时发光基质为纯的Sr3Al2O6相,1250℃时出现新的SrAl2O4杂相。激发光谱和发射光谱结果表明:长余辉发光材料的激发峰位于473nm,发射峰位于612nm,归属于Eu2+的4f65d1→4f7特征发光。温度升至1250℃时,Eu2+的发射峰为612nm和520nm,后者归属于Eu2+在发光基质SrAl2O4中的发光。综合分析得制备Sr3Al2O6:Eu2+,Dy3+发光材料合适的煅烧温度为1200℃,在此温度下,材料具有较好的初始亮度和余辉时间。     

Eu3+掺杂的硼酸锶系列荧光体的合成及其发光性能

采用溶胶-凝胶法和高温固相反应法合成了Eu^3 掺杂的SrB4O7、SrB2O4、Sr2B2O5、Sr3B2O6荧光体．荧光光谱测试结果表明在不同基质中Eu^3 的荧光发射是有区别的，Sr2B2O5：Eu^3 、Sr3B2O7：Eu^3 发射峰在610nm左右的红光区，SrB2O4：Eu^3 的发射峰在593nm的橙色区，而SrB4O7：Eu^3 则表现出了Eu^2 离子的特征峰，产生这种区别主要是由Eu^3 所处的配位环境不同造成的．荧光体SrB4O7：Eu^3 、SrB2O4：Eu^3 、Sr2B2O5：Eu^3 、Sr3B2O6：Eu^3 的最佳掺杂浓度为2％左右．     

Luminescence properties of nano-crystalline Ba3MgSi2O8:Eu2+, Mn2+ phosphors

Ba3MgSi2O8:Eu2+, Mn2+ phosphors were synthesized by the sol-gel method and high temperature solid-state reaction method, respectively. XRD (X-ray diffraction), FT-IR (Fourier transform infrared spectroscopy), PL (photoluminescence spectra), and PLE (photoluminescence excitation spectra) were measured to characterize the samples. Emission and excitation spectra of our Ba3MgSi2O8:Eu2+, Mn2+ phosphors monitored at 441, 515, and 614 nm are depicted in the paper. The emission intensities of 441 and 515 nm emission bands increase with increasing Eu2+ concentration, while the peak intensity of the 614 nm band increases with increasing Mn2+ concentration. We conclude that the 515 nm emission band is attributed to the 4f(6)5d transition of Eu2+ ions substituted by Ba2+ sites in Ba2SiO4. The 441 nm emission band originates from Eu2+ ions, while the 614 nm emission band originates from Mn2+ ions of Ba3MgSi2O8:Eu2+, Mn2+. Nano-crystalline Ba3MgSi2O8:Eu2+, Mn2+ phosphors prepared by the sol-gel method show higher color rendering and better color temperature in comparison with the samples prepared by high temperature solid-state reaction method.