通过高温固相法在还原气体保护下合成Ba4(SiaO8)2:Eu2+,Prf3+样品及一系列参比样品.分别利用两种模式测得光致发光与余辉光谱.结果显示:光致发光与余辉的发光中心均是Eu2.卜离子;共掺Pr3+在基质中引入新的俘获载流子的缺陷.热释光与余辉衰减测试表明,与单掺Eu2+所形成的陷阱深度相比,共掺pr3+导致余辉强度增强是归因于:在浅陷阱区(T1区)的陷阱深度变得更浅.而余辉时间增长是归因于:在深陷阱区(T2区1深陷阱密度大幅度减少.同时发现在不同激发波长下激发,余辉机理中的激发路径归结于以下两种过程.其一:268nm激发时,是基质中的电子被直接激发至陷阱.其二:330nm或365nm激发时,电子从Eu2+基态激发至激发态.随后部分电子通过导带运输被陷阱中心所俘获.因此,余辉强度的不同归结为以上两种载流子俘获路径的不同.
A bluish-green long persistent luminescence material Ba4(Si3Os)2:Eu2+, Pr3+, was synthesized by traditional solid state method in a reductive atmosphere According to the photoluminescence and afterglow spectra measurement, the emission center is the cation Eu2+ in the photoluminescence and afterglow procedure. The Pr3+ co-doped sample forms new defects which could capture current carriers after excitation. On the basis of thermoluminescence and afterglow decay measurement, the afterglow intensity of Pra+ co-doped sample sharply enhances as compared with Eu2+ doped one, the reason is that the lower depth traps are generated in the shallow trap areas (T1 region). At the same time, the Pr3+ co-doped sample have longer afterglow decay than that doped with only Eu2+; the reason is that the deep traps concentration decreases in the deep trap areas (T2 region). The afterglow mechanism of Pra+ co-doped sample have two of different excitation paths, path 1: the electron of the host is directly projected to traops at 268 nm excitation; path 2: the electron of the Eu2+ corresponds to the transitions from the ground state to the 5d excited state at 330 nm excitation. Then the different afterglow mechanism of phosphor was produced.