白光LED用Ce3/Sm3共掺玻璃和微晶玻璃的发光特性及能量传递研究

采用高温熔融法制备了一系列Ce3+/Sm3+共掺透明微晶玻璃,并研究了其发光特性.在微晶玻璃中Ce3+呈现出基于4f 5d跃迁的较强的宽带蓝光发射,通过调节Ce3+/Sm3+离子的掺杂浓度,Ce3+/Sm3+离子共掺微晶玻璃发光的色度逐渐发生变化,当CeO2/Sm2O3掺杂的量比为1∶1时,制得的微晶玻璃发光色坐标为(0.315,0.296).通过光谱和荧光衰减曲线,研究了Ce3+离子到Sm3+离子的能量传递,在SAZKNGC0.6S0.6微晶玻璃中,Ce3+离子向Sm3+离子传递能量效率约为20%.结果表明,Ce3+/Sm3+共掺微晶玻璃是白光LED的一种潜在基质材料     

Research on upconversion codoped oxyfluoride luminescence in new Er^3＋/Yb^3＋ borosilicate glass ceramics

The upconversion luminescence of Er^3＋/Yb^3＋ ions is researched in a novel transparent oxyfluoride borosil- icate glass and glass ceramics under 980-nm excitation. Fluoride nanocrystals Ba2YF7 are successfully precipitated in glass matrix, which is affirmed by the X-ray diffraction results. Compared with the parent glasses, significant enhancement of upconversion luminescence is observed in the Er^3＋/Yb^3＋ codoped transparent glass-ceramics, which may be due to the variation of coordination environment around Er^3＋ and Yb^3＋ ions after crystallization. The possible upconversion mechanism is also discussed.     

掺Er^3＋重金属氧氟硅酸盐玻璃的光谱性质与Judd—Ofelt理论分析

制备了掺Er^3 重金属氧氟硅酸盐玻璃，研究了玻璃的吸收光谱和荧光光谱性质，应用Judd-Ofelt理论计算了强度参数Ωt(t＝2，4，6)、Er^3 离子的振子强度、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数。应用McCCumber理论，计算了能级^413/2→^4I15/2跃迁的受激发射截面。结果表明：掺Er^3 重金属氧氟硅酸盐玻璃具有较宽的荧光半高宽和较大的受激发射截面。对Er^3 离子在不同玻璃基质中带宽特性的比较发现，掺Er^3 重金属氧氟硅酸盐玻璃的带宽特性与碲酸盐和铋酸盐玻璃相当，大于磷酸盐、锗酸盐和硅酸盐玻璃。     

Er3+掺杂重金属氧氟硅酸盐玻璃的上转换发光研究

研究了Er3 掺杂重金属氧氟硅酸盐玻璃的吸收光谱、上转换光谱和拉曼光谱 ,分析了重金属氧氟硅酸盐玻璃中Er3 的上转换发光机理 .结果表明 :通过 975nm的激光二极管激发 ,在室温下同时观察到蓝光 (4 1 1nmj)、绿光(5 2 5和 5 4 3nm)和红光 (6 5 5nm) ,分别是由于Er3 离子2 H9 2 →4 I1 5 2 ,2 H1 1 2 →4 I1 5 2 ,4 S3 2 →4 I1 5 2 ,和4 F9 2 →4 I1 5 2 跃迁 .随Er2 O3浓度的增加 ,蓝光、绿光和红光的发光强度都增强 ,上转换发光机理主要涉及能量转移和激发态吸收 ,强烈的绿光和红光激发是由于双光子吸收过程 ,而微弱的蓝光是由于三光子吸收过程 .拉曼光谱发现 ,对Er3 离子在重金属氧氟硅酸盐玻璃中的上转换发光 ,玻璃结构中的PbF2 起到重要作用     

Effect of concentration quenching on the spectroscopic properties of Er3+/Yb3+ co-doped AlF3-based glasses

A series of highly Er3+/Yb3+ co-doped fluoroaluminate glasses have been investigated in order to develop a microchip laser at 1.54 μm under 980 nm excitation. Measurements of absorption, emission and upconversion spectra have been performed to examine the effect of Er3+/Yb3+ concentration quenching on spectroscopic properties. In the glasses with Er3+ concentrations below 10 mol%, concentration quenching is very low and the Er3+/Yb3+ co-doped fluoroaluminate glasses have stronger fluorescence of 1.54 μm due to the 4I13/2 → 4I15/2 transition than that of Er3+ singly-doped glasses. As Er3+ concentrations above 10 mol% in the Er3+/Yb3+ co-doped samples, concentration quenching of 1.54 μm does obviously occur as a result of the back energy transfer from Er3+ to Yb3+. To obtain the highest emission efficiency at 1.54 μm, the optimum doping-concentration ratio of Er3+/Yb3+ was found to be approximately 1:1 in mol fraction when the Er3+ concentration is less than 10 mol%.     

Effect of concentration quenching on the spectroscopic properties of Er~(3+)/Yb~(3+) co-doped AlF_3-based glasses

A series of highly Er~(3+)/Yb~(3+) co-doped fluoroaluminate glasses have been investigated in order to develop a microchip laser at 1.54 μm under 980 nm excitation. Measurements of absorption, emission and upconversion spectra have been performed to examine the effect of Er~(3+)/Yb~(3+) concentration quenching on spectroscopic properties. In the glasses with Er~(3+) concentrations below 10 mol%, concentration quenching is very low and the Er~(3+)/Yb~(3+) co-doped fluoroaluminate glasses have stronger fluorescence of 1.54μm due to the ~4I_(13/2)→~4I_(15/2) transition than that of Er~(3+) singly-doped glasses. As Er~(3+) concentrations above 10 mol% in the Er~(3+)/Yb~(3+) co-doped samples, concentration quenching of 1.54μm does obviously occur as a result of the back energy transfer from Er~(3+) to Yb~(3+). To obtain the highest emission efficiency at 1.54μm, the optimum doping-concentration ratio of Er~(3+)/Yb~(3+) was found to be approximately 1:1 in mol fraction when the Er~(3+) concentration is l     

全光纤传感用磁光玻璃的研究进展

随着电力需求的不断增长，竞争日益剧烈的电力市场迫切需要高带宽、宽动态测量范围的小型传感器，全光纤传感器因其具有测量精度高、响应速度快、体积小和易安装等特点而引起了人们的广泛关注：在用于全光纤传感器的基质材料中，稀土离子掺杂的磁光玻璃因其各向均匀性好、磁光性能优异和成本低廉而成为首选材料之一，因而得到了广泛研究。基于目前磁光玻璃的研究成果，本文对有可能应用于全光纤传感器的高掺稀土玻璃材料进行了介绍，并对当前磁光玻璃研究中存在的问题进行了讨论。     

新型掺铒铋酸盐玻璃上转换发光研究

制备了新型掺Er3 铋铅锶玻璃,研究了玻璃的吸收光谱和上转换光谱性质,应用Judd-Ofelt理论计算了铋铅锶玻璃的3个强度参量Ωt(t=2,4,6),分别为Ω2=3.27×10-20 cm2,Ω4=1.15×10-20cm2,Ω6=0.38×10-20 cm2.计算了Er3 离子的振子强度、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数.研究了上转换发光强度随泵浦激光功率的变化,上转换荧光525,546和657 nm曲线的斜率分别为1.86,1.88和1.85,表明红、绿光发射均为双光子吸收过程.     

用于白光LED的规则球形YAG:Ce3+荧光粉制备及封装性能研究（英文）

采用高温固相法和筛分法合成了YAG:Ce3+系列黄色荧光粉。采用X射线衍射仪(XRD)、电子扫描显微镜(SEM)、激光粒度分布仪及荧光分光光度计对所制备样品进行了表征。结果表明:所得3种样品形貌规则成球形,粒度分布集中,其中心粒径(D50)分别为29.59,17.40,9.56μm,粒径分布离散度分别为0.85,0.80和0.87。通过Reitveld精修拟合发现,随着荧光粉粒径大小的变化,基质的晶格常数并未发生明显变化。随着中心粒径(D50)逐渐变小,其荧光发射强度逐渐降低,且发生明显的蓝移,同时对蓝光的吸收逐渐减弱。通过对荧光粉与蓝光芯片配合所得白光LED的发光效率、显色指数及色温进行测试发现,当使用相同粉胶比浓度、相同点胶量时,随着荧光粉粒径的减小,所得白光LED的流明效率从109.95 lm/W降低到了99.85 lm/W,而显色指数和色温同时升高。     

Er3+/Yb3+共掺杂氧氟硅酸盐玻璃的上转换发光

研究了Er^3 ／Yb^3 共掺氧氟硅酸盐玻璃的吸收光谱、上转换光谱和拉曼光谱。分析了氧氟硅酸盐玻璃中Yb”敏化Er^3 的上转换发光机理。结果表明：通过975nm的激光二极管激发,在室温下同时观察到蓝光(408nm)、绿光(529nm和545nm)和红光(667nm),分别是由于Er^3 离子。H9/2→^4I15/2,H11/2→^4I15/2,H3/2→^4I15/2和H9/2→^4I15/2跃迁。随Yb2O3浓度的增加。Yb^3 对Er^3 的能量转移增强,因此蓝光、绿光和红光的发光强度都增强,强烈的绿光和红光激发是由于双光子吸收过程,而微弱的蓝光是由于三光子吸收过程。拉曼光谱发现,对Er^3 离子在氧氟硅酸盐玻璃中的上转换发光。玻璃结构中的PbF2起到重要作用。