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稀土离子(Gd3+,Eu3+)加载于纳米介孔ZrO2中的发光 总被引:2,自引:0,他引:2
水热合成法制备的高度有序多孔ZrO2具有规则六角排列,均匀纳米孔洞(约1.8nm),丰富的表面,界面态及比表面积和强的蓝-(近)紫外光发射,使其较常规体材料有更优异的性质,以稀土离子为探针,研究了Gd^3 ,Eu^3 在这些纳米微孔中的发光行为,结果表明,500摄氏度下,介孔ZrO2与稀土离子相作用并有效地将能量传递给稀土离子,增进稀土离子发光,而在ZrO2:Gd-Eu体系中,Gd^3 在ZrO2与Eu3 间起桥梁作用,使基质ZrO2→Eu^3 的能量传递更为有效。 相似文献
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研究了BiTaO4∶Pr3+, BiTaO4的光致发光性质, 测量了BiTaO4的红外透射和漫反射光谱. BiTaO4的光致发光光谱发射峰位于约420, 440, 465 nm; 其激发谱在约330~370 nm范围有明显的激发. BiTaO4∶Pr3+的光致发光光谱为Pr3+的特征发射, 主峰为606 nm, 来自Pr3+的3P0→3H6跃迁; 其激发谱由来自于基质的峰值为325 nm和范围在375~430 nm的宽激发带以及Pr3+的特征激发组成, 325 nm, 375~430 nm的激发带可能分别来自钽酸根团的电荷迁移跃迁和基质的带间缺陷能级的吸收; 在BiTaO4∶Pr3+中存在着基质→Pr3+的能量传递. 由于BiTaO4∶Pr3+基质的密度和Pr3+的发光强度均超过PbWO4, 因此BiTaO4∶Pr3+可能是潜在的重闪烁体. 相似文献
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Full-profile fitting of emission spectrum to determine transition intensity parameters of Yb~(3+):GdTaO_4 下载免费PDF全文
The Judd-Ofelt theoretic transition intensity parameters A_(tp)~k of luminescence of rare-earth ions in solids are important for the quantitative analysis of luminescence.It is very difficult to determine them with emission or absorption spectra for a long time.A "full profile fitting" method to obtain A_(tp)~k in solids with its emission spectrum is proposed,in which the contribution of a radiative transition to the emission spectrum is expressed as the product of transition probability,line profile function,instrument measurement constant and transition center frequency or wavelength,and the whole experimental emission spectrum is the sum of all transitions.In this way,the emission spectrum is expressed as a function with the independent variables intensity parameters A_(tp)~k,full width at half maximum(FWHM) of profile functions,instrument measurement constant,wavelength,and the Huang-Rhys factor S if the lattice vibronic peaks in the emission spectrum should be considered.The ratios of the experimental to the calculated energy lifetimes are incorporated into the fitting function to remove the arbitrariness during fitting A_(tp)~k and other parameters.Employing this method obviates measurement of the absolute emission spectrum intensity.It also eliminates dependence upon the number of emission transition peaks.Every experiment point in emission spectra,which usually have at least hundreds of data points,is the function with variables A_(tp)~k and other parameters,so it is usually viable to determine A_(tp)~k and other parameters using a large number of experimental values.We applied this method to determine twenty-five A_(tp)~k of Yb~(3+) in GdTaO_4.The calculated and experiment energy lifetimes,experimental and calculated emission spectrum are very consistent,indicating that it is viable to obtain the transition intensity parameters of rare-earth ions in solids by a full profile fitting to the ions' emission spectrum.The calculated emission cross sections of Yb~(3+):GdTaO_4 also indicate that the F-L formula gives larger values in the wavelength range with reabsorption. 相似文献
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Absorption spectra of BiSbO4 are studied. The electronic structure calculated by the DFT shows that BiSbO4 is a semiconductor, with direct band gap 2.96 eV, which is consistent with UV-visible diffuse reflectance experiment. The host lattice emission band is located at 440 nm under VUV excitation. Eu^3+ and Pr^3+ doped samples have high luminescence efficiency in emitting red and green light, respectively. From the partial density of states, Eu^3+ doped emitting spectrum, and the host crystal structure parameters, the relationship between structure and optical properties is discussed. It is found that the Eu^3+ ions occupied Bi^3+ sites, and there could be an energy transfer from Bi^3+ ions to RE^3+ ions. 相似文献
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本文综述了近年来使用同步辐射研究稀有气固体、碱卤化物、碱土卤化物以及含稀土的离子晶体等宽禁带、绝缘体材料在激子动力学特性方面所取得的主要进展。包括激子的基本特性,激子与晶格的相互作用,特别是激子的自陷与激子激励的解吸附,激子与稀土中心间的能量传递,高激子态的弛予以及团簇中的激子特性等。最后简介典型的实验系统。 相似文献
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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。 相似文献
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本文报道了纳米Gd203:(Ce^3 ,En^3 )的紫外与真空紫外(UV-VUV)激发谱及其选择激发下的荧光光谱。这些光谱实数表明,除了Gd2O3基质与Ce^3 ,Eu^3 离子之间的能量传递外,还存在着Gd^3 与Ce^3 、Eu^3 间的能量传递,即存在Gd^3 →Ce^3 →Eu^3 三种稀土离子间的级联传递。 相似文献