阳离子对Er3+掺杂硼酸盐玻璃结构和发光特性的影响

针对Si/Al掺杂量增大使BaO-(1-x)SiO₂-xAl₂O₃-B₂O₃-0.005Er³⁺(x=0,0.5,1,摩尔分数)玻璃样品的1 540 nm红外发光和540 nm上转换发光强度呈现相反的变化趋势,讨论了阳离子掺杂对稀土离子周边对称性和电负性变化与荧光行为的内在关系。红外傅里叶透射光谱显示,不同掺杂浓度下样品的最大声子能量没有明显变化,说明光谱随掺杂浓度的变化与玻璃体系的最大声子能量无关。根据Judd-Ofelt理论计算了⁴I_13/2和⁴S_3/2能级的光学参数,通过比较两能级的跃迁几率(A)、寿命(τ)、荧光分支比(β)和受激发射截面(σ)等光学参数,发现⁴I_13/2能级和⁴S_3/2能级的相关参数呈现相反的趋势。最后测试了样品⁴I_13/2能级下1 540 nm的寿命,进一步从电负性角度考虑了样品的发光效率。理论计算和实验结果相符。     

Influence of Si4+ substitution on the temperature-dependent characteristics of Y3Al5O12:Ce

A series of Y3Al5O12:Ce(YAG:Ce) phosphors doped with different Si 4+ concentrations is prepared by solid-state reaction.The temperature dependent characteristics of luminescent spectrum and decay time of Ce 3+ are investigated.With Si 4+ doped,the emission spectrum shows a blue shift due to a decrease of the splitting of 5d levels of Ce 3+ ion.The thermal stability is greatly improved by adding Si 4+ because the activation energy E increases from 0.1836 eV to 0.2401 eV.The study of the decay times against temperature for various doping concentrations of Si 4+ shows that the calculated nonradiative decay rate is affected by Si 4+ substitution.The results are explained by the configurational coordinate diagram.     

Influence of Si^4＋ substitution on the temperature-dependent characteristics of YaAl5O12：Ce

A series of aAl5O12：Ce （YAG：Ce） phosphors doped with different Si4＋ concentrations is prepared by solid-state reaction. The temperature dependent characteristics of luminescent spectrum and decay time of Ce3＋ are investigated. With Si4＋ doped, the emission spectrum shows a blue shift clue to a decrease of the splitting of 5d levels of Ce3＋ ion. The thermal stability is greatly improved by adding Si4＋ because the activation energy AE increases from 0.1836 eV to 0.2401 eV. The study of the decay times against temperature for various doping concentrations of Si4＋ shows that the calculated nonradiative decay rate is affected by Si4＋ substitution. The results are explained by the configurational coordinate diagram.     

The influence of cation additives on the NIR luminescence intensity of Er3+-doped borate glasses

Er3+-doped 25BaO-(25-x)SiO2-xAl2O3-25B2O3 transparent glasses are prepared with x = 0,12.5 and 25 by a solid-state reaction.The Er-related NIR luminescence intensity,which corresponds to the transition of 4I15/2-4I13/2,is obviously altered with different silicon/aluminum ratios.The Judd-Ofelt parameters of the Er3+ ions are adopted to explain the intensity change in the NIR fluorescence,and the Raman scattering intensity versus the amount of Al and/or Si components are discussed.The spectra of the three samples are quite similar in the peak positions,but different in intensity.The maximal phonon density of state for the samples is calculated from the Raman spectra and is correlated to the NIR luminescence efficiency.     

Er3+在KPb2Br5晶体中的选择替位对上转换发光光谱的影响

通过高温固相法制备了不同Er³⁺掺杂浓度的KPb₂Br₅多晶粉末样品. 由980 nm半导体激光器激发下得到的上转换发射光谱显示, 当掺杂浓度为2.5 mol%时, 样品主要表现为530 nm 和550 nm上转换发射, 分别对应激发态²H_11/2和⁴S_3/2向基态⁴I_15/2的跃迁; 掺杂浓度增加到5 mol%时样品以490 nm上转换发射为主, 对应由激发态⁴F_7/2向⁴I_15/2的跃迁; 当掺杂浓度达到7.5 mol%时, 样品的上转换发射强度相比低浓度时大幅度下降, 主要以激发态⁴F_9/2 向基态⁴I_15/2跃迁的690 nm处发光为主. 利用第一性原理结合Judd-Ofelt理论讨论认为, Er³⁺ 离子优先替代Pb (1) 的位置, 随着浓度的提高, 部分Er³⁺ 离子会替代Pb (2) 格位上的离子, 不同晶格位置的Er³⁺ 离子所处的晶体场的对称性有所不同, 从而影响了发光中心不同能级的跃迁概率, 体现在上转换发光光谱的差异上. 蓝、绿区域的上转换发光在高浓度掺杂下显示了明显的浓度猝灭, 此时样品以红色上转换发光为主. 关键词： 2Br₅：Er³⁺')" href="#">KPb₂Br₅：Er³⁺ Judd-Ofelt理论 第一性原理 上转换发射     

The influence of cation additives on the NIR luminescence intensity of Er³⁺-doped borate glasses

Er3+-doped 25BaO-(25-x)SiO2-xAl2O3-25B2O3 transparent glasses are prepared with x = 0,12.5 and 25 by a solid-state reaction.The Er-related NIR luminescence intensity,which corresponds to the transition of 4I15/2-4I13/2,is obviously altered with different silicon/aluminum ratios.The Judd-Ofelt parameters of the Er3+ ions are adopted to explain the intensity change in the NIR fluorescence,and the Raman scattering intensity versus the amount of Al and/or Si components are discussed.The spectra of the three samples are quite similar in the peak positions,but different in intensity.The maximal phonon density of state for the samples is calculated from the Raman spectra and is correlated to the NIR luminescence efficiency.