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测量和分析了不同温度下Eu3+:ThO2的激发光谱、发射光谱和荧光 衰减曲线.Eu3+:ThO2晶体是用熔融法生长的.通过12K下格位选择激 发下的发射光谱测量,利用晶场理论,确定了Eu3+在ThO2占据Oh和C3v两种格位.列表给出了两种格位Eu3+离子的晶场能 级和室温及12K下的荧光寿命.讨论了温度对能 相似文献
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本文首次报道在3.15 GPa、1 200 ℃高温高压条件下合成出了SrSiO3:Eu3+Bi3+发光材料,并与常压合成产物相比较,研究了高温高压合成产物的结构以及合成压力、温度对发光特性的影响。结果表明,高压合成产物SrSiO3:Eu3+Bi3+的结构为膺正交(单斜)结构,而常压合成的为六角结构,高压使发光强度下降,量子发光效率下降了88%,谱线红移达756 cm-1,半值宽度也显著增加,发光性能的改变是由于压致结构的变化引起的。 相似文献
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采用共沉淀法制备了不同Eu3+掺杂浓度的CaWO4荧光粉材料.通过X射线衍射和场发射扫描电镜技术对样品的结构和形貌进行了表征.测量了各样品的激发光谱、发射光谱和荧光衰减曲线, 计算了各样品的部分Judd-Oflet (J-O)参数和5D_0 (Eu3+)能级量子效率,以及荧光粉的色坐标, 讨论了样品电荷迁移带相对强度、J-O参数、量子效率与掺杂浓度的依赖关系.对Eu3+掺杂的CaWO4 发光材料的光致发光性质的研究表明,在CaWO4: Eu3+中5D0→7F2跃迁的616~nm 红色发光能被394.5~nm和465~nm的激发光有效激发,具有近紫外(或蓝光)激发效率高和猝灭浓度大的优点, 有潜力成为高效的近紫外(或蓝光)激发白光发光二极管用红色荧光粉材料. 相似文献
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三基色荧光粉中, 红色荧光粉性能较差, 为获得性能优良的红色荧光粉, 本文采用高温固相法合成了Eu2+, Cr3+单掺杂及共掺杂的碱土金属多铝酸盐MAl12O19 (M =Ca, Sr, Ba) 发光体. 实验表明, 在以上三种基质中均存在Eu2+→Cr3+的能量传递, 利用能量传递可以有效将Eu2+的蓝光或绿光转换为红光. 三种碱土金属多铝酸盐基质的晶体结构相似,但Eu2+, Cr3+发光受晶体场影响,导致在不同的基质中Eu2+, Cr3+间能量传递效率不同.通过光谱分析及能量传递效率计算发现, 相同掺杂浓度下,CaAl12O19中Eu2+→Cr3+的能量传递效率最高,SrAl12O19次之, BaAl12O19最低.红光转换率在CaAl12O19中最高. 相似文献
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采用新型超声喷雾共沉淀法技术,以Lu2O3、Eu2O3、Al(NO3)3·9H2O为原料,制备了不同浓度Eu3+离子掺杂的Lu3Al5O12纳米粉体.用X射线粉末衍射表征了获得纳米粉体的相,用扫描电镜观察了纳米粒子的形貌.测定了粉体的激发光谱、7F0-5D2声子边带谱与发射光谱.研究了不同高温烧结温度与Eu3+掺杂浓度对纳米粒子的发光强度与粒子形貌的影响规律.研究表明,当烧结温度高于900 ℃时,粉体发光强度明显增强,并且随着煅烧温度的增加,发光强度有所增强.Eu3+离子的最佳掺杂浓度为5~7 mol%.根据稀土离子Eu3+光学跃起矩阵元的特点,从发射光谱获得Eu3+光学跃起的J-O参量Ω2与Ω4.在Eu3+掺杂浓度均为5 mol%时,其强度参量达最小,电-声子耦合最强.然后随着掺杂浓度的进一步提高,强度参量略有增加,电-声子耦合减弱.说明Eu-O键强增加,共价性增强,Eu3+的局域环境对称性降低.Ω2值低于Eu3+在玻璃与晶体基质中的情况,这是由于纳米粒子中存在着大量的缺陷以及晶体的结构畸变导致纳米粒子的对称性下降所致. 相似文献
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采用传统固相法和水热法成功地制备出棒状La2Zr2O7:Eu3+荧光粉. 利用X射线粉末衍射仪、透射电镜和荧光光谱仪等分析了产物的结构、形貌和发光特性. 结果表明红色荧光粉La2Zr2O7:Eu3+有良好的晶相,属于立方结构,空间点群为Fd3m; 其形貌主要为纳米棒, 平均直径约47 nm, 长度为50~700 nm. 并对纳米棒的生长机理进行了探讨. 在466 nm蓝光激发下,La2Zr2O7:Eu3+荧光粉能发射出Eu3+的特征红色荧光,发射主峰位于616 nm处,归属于Eu3+的5DO→7F2超灵敏电偶极跃迁.此外,在产物的发射光谱中能够观察到5D1→7FJ (J=0, 1, 2)跃迁和5D1→7FJ (J=1, 2, 4)跃迁的劈裂峰,这说明Eu3+处在低对称性的晶体场格位中. 相似文献
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A photoluminescence (PL) study of the green-emitting SrGa2S4:Eu2+ phosphor is reported. Diffuse reflectance, excitation, and emission spectra were examined with the aim to enlarge the fundamental knowledge about the emission of the Eu2+ ion in this lattice. The thermal dependence of the radiative properties was investigated. In particular, the Stokes shift, the crystal field splitting and the activation energy of the thermal quenching were determined. By combining these results with the information presented in literature, we discussed the location of the Eu2+ levels relative to the valence and conduction bands of SrGa2S4. 相似文献
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R.B. Jabbarov B.G. Tagiev N.N. Musayeva P. Benalloul 《Journal of Physics and Chemistry of Solids》2005,66(6):1049-1056
A photoluminescence study of the blue-green emitting BaGa2S4:Eu2+ phosphor is reported. Diffuse reflectance, excitation and emission spectra were examined with the aim to enlarge the fundamental knowledge about the emission of the Eu2+ rare earth ion in this lattice. The thermal dependence of the radiative properties and the influence of the Eu2+ concentration were investigated. The Stokes shift, the crystal field splitting and the activation energy of the thermal quenching were determined. By combining these results with data available in literature, we discussed the radiative properties of the BaAl2S4:Eu2+ blue phosphor in relation with those determined in this study for the isostructural BaGa2S4:Eu2+ phosphor. 相似文献
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The photoluminescent (PL) emission and excitation behaviour of green-emitting CaAl2S4:Eu2+ powder phosphor is reported in detail. CaAl2S4:Eu2+ emission provides good CIE colour coordinates (x=0.141; y=0.721) for the green component in display applications. Powder with a dopant concentration of 8.5 mol% shows the highest luminescence efficiency. Temperature dependence of the radiative properties, such as luminescence intensity and decay time, was investigated. In particular, the Stokes shift, the mean phonon energy, the redshift, the energy of the f→d and d→f transition and the crystal field splitting of the CaAl2S4:Eu2+ emission were determined. The thermal quenching of the emission was examined. 相似文献
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Nanosized luminescent (Y,Bi)VO4:Eu3+ and Y(V,P)O4:Eu3+ were synthesized at low temperatures either by a coprecipitation method or by a hydrothermal method from aqueous solutions. The effect of Bi3+ ion or P5+ ion content in the lattice, annealing temperature effects on the crystal structure and the particle size, and the luminescence property of (Y,Bi)VO4:Eu3+ and Y(V,P)O4:Eu3+ nanoparticles were examined with a field-enhanced scanning electron microscopy, XRD, and a spectrofluorometer. The pristine YVO4:Eu3+, (Y,Bi)VO4:Eu3+, or Y(V,P)O4:Eu3+ nanoparticles are 35-50 nm in size. The luminescence spectrum of the Eu3+ ion was used to probe its position in the crystal lattice. The dopant ions enter the same lattice sites in the nanocrystalline as in the corresponding bulk material, resulting similar spectral features between them. Photoluminescence intensity is weak for the pristine nanoparticles. Annealing the nanoparticles at temperatures up to 1000 °C results in the increased luminescence intensity (>80% of micrometer-sized phosphors) with the minimal particle growth and the improved particle crystallinity. 相似文献
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Phosphor material BaAl2O4:Eu2+, Dy3+ with varying compositions of Sr substitution were prepared by the solid-state synthesis method. The phosphor compositions were characterized for their phase and crystallinity by XRD, SEM and TEM. Photoluminescence (PL) properties were investigated measuring PL and decay time for varying Ba/Sr compositions. The PL results show the blue shift in the luminescence properties in Sr substituted BaAl2O4:Eu2+, Dy3+ compared to parent BaAl2O4:Eu2+, Dy3+. It is probably due to the influence of 5d electron states of Eu2+ in the crystal field because of atomic size variation causing crystal defects. Dy3+ ion doping in the phosphor generates deep traps, which results in long afterglow phosphorescence. 相似文献
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Fluorescence properties of divalent and trivalent europium ions in CdWO4 single crystals grown by Bridgman method
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Hu Hao-Yang Xia Hai-Ping Hu Jian-Xu Zhang Yue-Pin Jiang Hao-Chuan Chen Hong-Bing 《中国物理 B》2013,22(2):27804-027804
Optical absorption, excitation, and fluorescence were investigated in Eu ion-doped CdWO4 single crystal grown by a modified Bridgman method. The results indicate that Eu2+ and Eu3+ ions coexist in CdWO4 crystal and an energy transfer occurs between these Eu2+ and Eu3+ ions. When the crystal is excited by 266-nm light, the energy corresponding to the 4f65d to 8S7/2 transition of Eu2+ ions results in the excitation of the Eu3+ ions to the 5DJ level. The effect on fluorescence of annealing in oxygen at various temperatures was investigated. The excitation intensity of Eu2+ ions at 266 nm decreases as annealing temperature increases from 300 K to 1073 K, but it remains at a certain equilibrium level when the annealing temperature is further increased. 相似文献
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V.P. Dotsenko S.M. Levshov G.B. Stryganyuk A.S. Voloshinovskii 《Journal of luminescence》2011,131(2):310-315
The luminescent properties of Eu2+ and Ce3+ ions in Li2SrSiO4 have been studied upon excitation in the 2-20 eV region. Based on the results of luminescent measurements, values of the crystal field splitting and the centroid shift of the Ce3+5d configuration in Li2SrSiO4 were found and compared with those of Ce3+ ions in some other inorganic compounds. The Eu2+ ions in Li2SrSiO4 exhibit a broad band emission with a maximum at 576 nm, which is due to the 4f65d→4f7 transition. It was shown that the long-wavelength position of the Eu2+ emission in Li2SrSiO4 is caused by the large crystal-field splitting of the Eu2+ 4f65d configuration and relatively high degree of covalency of the Eu-O bond. The stabilization of Eu2+ ions in Li2SrSiO4 during the synthesis process requires a strong reducing agent. Two phenomenological approaches to explain the low stability of Eu2+ in Li2SrSiO4 are also discussed. 相似文献
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The emission spectra and decay times of the Y2O3 CO-doped with Bi3+ and Eu3+ have been investigated using site-selective excitation and time-resolved spectroscopy in the temperature range 8–296 K. Evidence for an energy transfer from Eu3+(S6) to Eu3+(C2) is given. The critical transfer distance R0 = 8.6 Å was found from the decay curve. 相似文献