YTaO_4∶Nb,Eu的发光性能研究

用高温固相反应法合成了铌酸根 Nb O3- 4 和 Eu3+共掺杂的正钽酸盐化合物 Y1 - x Eux Ta1 - y Nby O4,研究了该体系在紫外光和 X射线激发下的发光性能 .研究表明 ,在紫外光激发下 ,YTa O4∶ Nb,Eu是一种比较有效的红色发光材料 .激发能可以通过 Nb O3- 4 离子传递给 Eu3+离子 .随钽酸盐中 Nb O3- 4 基团浓度的增加 ,化合物的结构从 M′型 YTa O4变成褐钇铌型 YNb O4结构 ,它的发光性质也随之改变 .     

YTaO4：Gd,Eu体系光致发光中的能量传递

用高温固相反应法合成了钆、铕离子双掺杂的正钽酸盐化合物YTaO4 :Gd ,Eu ,研究了该体系在紫外光激发下的发光性能 .对该体系激发、发射及漫反射光谱的研究表明 ,Gd3 离子在发光过程中可以作为能量传递的中介 ,该体系在发光过程中存在钽酸根到Eu3 离子 ,或者钽酸根到Gd3 离子、再到Eu3 离子的能量传递     

稀土氧化钕对铝酸盐长余辉发光材料性能的影响

制备了SrAl2O4:Eu2 ,Nd^3 和SrAl2O4:Eu^2 ,Dy^3 ,Nd^3 长余辉材料,研究了所合成的材料在不同波段紫外光激发条件下的发光光谱和激发光谱的差异和Eu^2 ,Dy^3 ,Nd^3 的摩尔掺杂浓度对材料的余辉性能的影响等。     

LaPO4:Eu3+纳米粒子的多醇法合成及其光致发光性能研究

以一缩二乙二醇为溶剂，采用多醇法（polyol method）合成LaPO4：Eu^3＋纳米发光材料，利用XRD、FE．SEM、TG-DTA、Uv-vis光谱、光致发光光谱（PL）及寿命等手段进行了表征。结果表明：所得到的材料结晶完好，具有LaPO4的独居石型结构；粒子的形貌为球形，其粒径约为25nm；在波长为258nm的紫外光激发下，其发射光谱由Eu^3＋的5D0^-7FJ（J=1，2，3，4）特征发射组成，在592nm处的磁偶极跃迁（5D0^-7F1）最强，表现为Eu^3＋的橙-红特征发射；LaP04：Eu^3＋纳米粒子中Eu^3＋的最佳掺杂浓度为5％（摩尔比）；Eu^3＋的光致发光衰减曲线符合单指数行为，其寿命（τ）为3．9ms。     

NaGdF4:Eu3+的结构和VUV荧光性质

利用水热方法合成了纯度较高的六方结构的ＮaGdF4,在氧气存在条件下950℃加热处理可以使其转变为CaF2型立方结构,在真空紫外光激发下,六方结构的NaGdF4:Eu^3 中的Gd^3 离子吸收一个光子,并将能量分两步传递给Eu^3 离子,发生双光子发射,立方结构的NaGdF4:Eu^3 中存在有一定量的氧离子取代缺陷,使Gd^3 离子4f-5d跃迁移到177nm附近,这与惰性气体放电产生的真空紫外波长一致。     

MO-RE2O3-B2O3(M=Mg,Ca,Sr,Ba;RE=La,Eu,Gd)玻璃的发光性质

在空气中采用高温固相反应方法合成的17MO－（8-x-y)-75B2O3-xGd2O3(MLBEG,M-Mg,Ca,Sr,Ba)玻璃，在紫外光（λex=350nm)激发下发射蓝光和红光，在绿色光（λex=532nm)激发下发射红光，电子自旋共振谱研究表明玻璃体系中有Eu^2 离子存在，蓝色区的宽带发射是Eu^2 离子的5d-4f跃迁发射：红色区的窄带发射是Eu^3 离子的5Do-7FJ(J=1,2,3,4)跃迁发射，发现玻璃中的碱土金属离子对Eu^3 /Eu^2 离子的比例有很大影响，选择不同的碱土金属离子可以调节玻璃蓝色光和红色光的相对发射强度，MLBEG玻璃的发光性质可用于转换太阳能，增强植物的光合作用。     

三种方法制备CaGdAlO4:Eu3+荧光粉及其发光性质研究

分别采用柠檬酸溶胶-凝胶法、半干半湿法和高温固相法制备了CaGdAlO4：Eu^3＋荧光粉，并用X线衍射（XRD）分析、场发射扫描电镜（FE—SEM）观察和荧光光谱分析研究了不同制备方法和制备条件对CaGdAlO4：Eu^3＋形貌、粒径和发光性质的影响。XRD结果表明，柠檬酸溶胶-胶法、半干半湿法和固相法制备CaGdAlO4：Eu^3＋生成纯相的温度分别为900，1200和1400℃。FE—SEM照片显示CCaGdAlO4：Eu^3＋颗粒粒径随温度的升高而增大，在同一烧结温度下，粒径大小为柠檬酸溶胶-凝胶法最小，半干半湿法居中，高温固相法最大而且团聚现象严重。以280nm近紫外光激发，CaGdAlO4：Eu^3＋发出明亮的橙红色荧光，以Eu^3＋的^5D0→^7F2跃迁为主，发光强度随烧结温度的升高而增加，在1400℃烧结温度下，以半干半湿法得到的样品发光最强。室温和低温发射谱中Eu^3＋的^5D0→^7Fj，发射峰的数目都表明：Eu^3＋在CaGdAlO4中只占据偏离反演中心的一种格位。     

氧化铝柱层状类钙钛矿型铌酸盐KSr2Nb3O10的制备与表征

采用分步交换法,制备了氧化铝柱层状类钙钛矿型新铌酸盐KSr2Nb3O10。采用X射线衍射、扫描电镜对该化合物的结构与形貌进行了表征,并测定了其比表面积。结果表明,该化合物具有较高的热稳定性和较大的比表面积。     

新型双钼酸盐红色荧光粉的制备及发光性能研究

采用高温固相法合成了一种新型的白光LED用双钼酸盐红色荧光粉,利用XRD,F-4500等对其进行了研究。结果表明:该系列荧光粉可以被近紫外光(396 nm)和蓝光(466 nm)有效激发,发射峰值位于615 nm(Eu3+离子的5D0→7F2跃迁)的红光;而且在钾铕双钼酸盐荧光粉KEu(MoO4)2中引入适量的钨酸能加强其发光强度,而不改变样品的发射光谱的形状和发射峰的位置。此外,在确定WO24-/MoO42最佳比值的前提下,文章还详细探讨了碱金属离子相互置换对样品发光性能影响的机制。     

铌酸盐Ba6FeNb9O30的XRD研究

在BaO -Fe2O3-Nb2O5 三元系统中 ,新发现存在铌酸盐Ba6FeNb9O30,利用四圆单晶衍射仪进行了晶胞参数测定 ,然后采用X射线粉晶衍射法获得该化合物的粉晶衍射数据 ,并进行了指标化 ,F30 =32(0.016,58)。XRD分析结果表明 ,该化合物属于填满型四方钨青铜结构 ,晶胞参数为 :a=1.25812(4)nm ,c=0.3992(4)nm ,α=β=γ=90°。     

YTaO4：Gd,Eu体系光致发光中的能量传递

Yttrium orthotantalate co doped by Eu 3+ and Gd 3+ has been synthesized by solid state method. The emission and excitation spectra of YTaO4: Gd, Eu are studied in detail. In the excitation spectra of Eu 3+5D 0→ 7F2 transition emission in YTaO4:Gd, Eu, there appear excitations of Gd3+ and TaO43- group, which indicate energy transfer from Gd 3+ and TaO4 3- group to Eu 3+ in the process of luminescence. The excitation spectra of Gd 3+ emission(λ=312 5 nm) including strong excitation of charge transfer of group show energy transfer from host lattice to Gd 3+ . So there are two ways of energy transfer in YTaO4:Gd,Eu system. The strong evidences from excitation spectra, emission spectra and diffusive reflection spectra of this system show that Gd 3+ can play an intermediate role in the process of luminescence. There is energy transfer from TaO 3- 4 to Gd 3+ and finally to Eu 3+ via the charge transfer state and spectral overlap. The energy transfer from TaO 3- 4 to Gd 3+ is a dominating process in this system.     

Ca3La3(BO3)5中Eu3+的光致发光

本文详细地研究了紫外光激发下,Ca_3La_3(BO_3)_5中Eu~(3+)的发光光谱和激发光谱与组成、结构的关系.发现Eu~(3+)在此基质中可能不止一个发光中心;Eu~(3+)自身浓度猝灭的机理为电四极-四极相互作用.     

GdVO_4∶Eu~(3 )的真空紫外激发光谱研究

报道了GdVO4∶Eu3 的光致发光光谱和真空紫外 紫外激发光谱。GdVO4∶Eu3 是高效率的真空紫外 紫外激发荧光材料。GdVO4∶Eu3 在6 0～ 35 0nm真空紫外 紫外波段的激发可能主要来源于基质的吸收 ,有明显的Eu3 及Gd3 的 4fn - 1 5d吸收。在GdVO4∶Eu3 中 ,存在如下能量传递过程 :VO3 - 4 →Eu3 ,Gd3 →Eu3 ,Gd3 →VO3 - 4 →Eu3 ;通过后两个过程 ,Gd3 Eu3 可实现量子剪裁。     

Gd3Ga5O12∶Eu3+发光纳米晶的燃烧合成及性质

以尿素为燃烧剂,乙二醇为分散剂采用燃烧法制备了Gd3Ga5O12∶Eu3+纳米晶。利用X射线衍射、电镜和荧光光谱对前驱体和热处理后样品的结构、形貌和发光性能进行了表征。XRD结果表明:700℃热处理2 h即可获得立方结构Gd3Ga5O12∶Eu3+纳米晶。根据Scherrer公式估算经700℃和900℃热处理2 h获得的纳米晶的一次性粒径分别为28 nm和42 nm。发射光谱和激发光谱的结果表明:特征发射峰来自于5D0-7FJ跃迁,而来自于Eu3+的5D0→7F1的磁偶极跃迁发射最强;宽激发带主要来自于Eu-O电荷迁移带和Gd3Ga5O12基质吸收。发射强度和激发强度随热处理温度的提高而增强。     

An approach to control of band gap energy and photoluminescence upon band gap excitation in Pr(3+)-doped perovskites La(1/3)MO3 (M=Nb, Ta):Pr3+

We synthesized polycrystalline pristine and Pr(3+)-doped perovskites La(1/3)MO(3) (M = Nb, Ta):Pr(3+) and investigated their crystal structure, optical absorption, and luminescence properties. The optical band gap of La(1/3)NbO(3) (3.2 eV) is smaller than that of La(1/3)TaO(3) (3.9 eV), which is primarily due to the difference in electronegativity between Nb and Ta. In La(1/3)NbO(3):Pr(3+), the red emission assigned to the f-f transition of Pr(3+) from the excited (1)D(2) level to the ground (3)H(4) state upon band gap photoexcitation (near-UV) was observed, whereas the f-f transition of Pr(3+) with blue-green emission from the excited (3)P(0) level to the ground (3)H(4) state was quenched. On the other hand, in La(1/3)TaO(3):Pr(3+), the blue-green emission upon band gap photoexcitation was observed. Their differences in emission behavior are attributed to the energy level of the ground and excited states of 4f(2) for Pr(3+), relative to the energy levels of the conduction and valence bands, and the trapped electron state, which mediates the relaxation of electron from the conduction band to the excited state of Pr(3+). La(1/3)NbO(3):Pr(3+) is a candidate red phosphor utilizing near-UV LED chips (e.g., λ = 375 nm) as an excitation source.     

Vacuum Ultraviolet Excited Photoluminescence Properties of Y202S:Eu3+,Bi3+ Phosphor

As an Hg-free lamp using phosphor,the Bi3+ and Eu3+ co-doped Y2O2S phosphors were prepared and their luminescence properties under vacuum uitraviolet(VUV) excitation were investigated.The VUV photolumineseent intensity of Y2O2S:Eu3+ was weak,however,considerably stronger red emission at 626 nm with good color purity was observed in Y2O2S:Eu3+,Bi3+ systems.Investigation on the photoluminescence reveals that the strong VUV luminescence of Y2O2S:Eu3+,Bi3+ at 147 nm is mainly because the Bi3+ acts as a medium and effectively performs the energy transfer process: Y3+-O2→Bi3+→Eu3+,while the intense emission band at 172 nm is attributed to the absorption of the characteristic 1So-1P1 transition of Bi3+ and the direct energy transfer from Bi3+ to Eu3+.The Y2O2S:Eu3+,Bi3+ shows excellent VUV optical properties compared with the commercial (Y,Gd)BO3:Eu3+.Thus,the Y2O2S:Eu3+,Bi3+ can be a potential red VUV-excited candidate applied in Hg-free lamps for backlight of liquid crystal display.     

Synthesis and Luminescent Properties of Nano-scale Y2Si2O7:Re3+ (Re=Eu,Tb) Phosphors via Sol-Gel Method

By using metal nitrates as starting materials and citric acid as a complexing agent, Y2Si2O7:Re3+ (Re=Eu, Tb) phosphors were prepared by a sol-gel method. X-ray diffraction was employed to characterize the resulting samples. The results of XRD indicate that the ff-Y2Si2O7 nanocrystal with size of 27 nm is obtained at 1000 oC and the doping ion content does not influence the structure. The excitation spectra in the UV and VUV ranges and the emission spectra of Re3+ doped samples were measured. The excitation spectra in the VUV range is due to absorption of host, that in the UV range is ascribed to absorption transitions from 4f to 5d state of the Tb3+ and the charge transfer in the Eu3+-O2- bond. The spectral energy distribution of the Tb3+ emission depends strongly on the Tb3+ concentration. The dependence of photoluminescence intensity on Re3+ concentration is also discussed in detail. The fluorescent decay curves at room temperature were measured and analyzed.     

立方Gd2O3∶Eu纳米晶及光谱性质

用透射电镜拍摄球形ＣＧｄ２Ｏ３∶Ｅｕ纳米晶,并研究了室温下它的激发和发射光谱。结果表明,９００℃制备的体材料和相应的纳米晶相比,其激发光谱存在明显差异。前者以基质激发带为主导,电荷转移带（ＣＴＢ）很弱,而后者以ＣＴＢ为主。在绝缘体稀土氧化物中,可以忽略纳米效应对Ｅｕ３＋离子的４ｆ４ｆ能级跃迁的激发和发射光谱峰位的影响     

CaAl12O19基质中Eu2+-Cr3+的能量传递与发光性质

在还原气氛下高温固相法合成了CaAl12O19:Eu2+,Cr3+荧光粉.样品光谱显示:Eu2+发射带与Cr3+吸收带有重叠,具备Eu2+-Cr3+之间发生能量传递必要条件.在290 nm近紫外光激发下,单掺杂Eu2+和Cr3+时样品均无691 nm发射,仅在Eu2+,Cr3+共掺时才出现691 nm发射,这证明Eu2+和Cr3+之间发生了能量传递,且监测691 nm时样品的激发光谱也证实了这一点.CaAl12O19:1%Eu2+,x%Cr3+样品组的发射光谱研究表明:增大x能提高Cr3+红光与Eu2+蓝紫光发射强度之比及Eu2+-Cr3+之间能量传递效率.CaAl12O19:2%Cr3+,x%Eu2+样品组的激发光谱分析表明:x>2时,Cr3+在415 nm处的吸收效率相对于565 nm有显著提高.还对样品CaAl12O19:1%Eu2+,1%Cr3+荧光寿命和能量传递速率进行了简单分析.     

Identification of charge transfer (CT) transition in (Gd,Y)BO3:Eu phosphor under 100-300 nm

A broad excitation band in an excitation spectrum of (Gd,Y)BO₃:Eu was observed in the VUV region. It could be considered that this band was composed of two bands at about 160 and 166 nm. The preceding band was assigned to the BO₃ group absorption. The later one at about 166 nm could be assigned to the charge transfer (CT) transition of Gd³⁺-O²⁻. Such an assignment was deduced from the result that broadbands at around 170 nm for GdAlO₃:Eu, and at 183 nm for Gd₂SiO₅:Eu are due to the CT transition of Gd³⁺-O²⁻; this was also identified by CaZr (BO₃)₂:Eu. Since there are no Gd³⁺ ions in it; a weak band in the VUV region in the excitation spectrum of Ca_0.95ZrEu_0.05(BO₃)₂ was observed. The excitation spectra were overlapped between the CT transition of Gd³⁺-O²⁻ and BO₃ group absorption, and it caused the emission of Eu³⁺ effectively in the trivalent europium-doped (Gd,Y)BO₃ host lattice under 147 nm excitation. Intense broad excitation bands were observed at about 155 nm for YBO₃:Eu and at about 153 nm for YAlO₃:Eu; it could be attributed to the CT transition between Y³⁺ and O²⁻. As a result, under the xenon discharge (147 nm) excitation, the intense emission of Eu³⁺ in GdBO₃ was found to be more convenient just because of the partial substitution of Y³⁺ for Gd³⁺.