欢迎登录材料期刊网

材料期刊网

高级检索

以NH4HCO3、NH3·H2O混合溶液为沉淀剂,用共沉淀法结合后续煅烧制备了铈掺杂钇铝石榴石(YAG∶Ce)荧光粉,并采用热分析、红外光谱、X射线衍射、场发射扫描电镜等对粉体进行了研究,分析了铈掺杂浓度对粉体发射光谱和激发光谱的影响.结果表明:共沉淀法制备的铈掺杂钇铝石榴石经过1 000℃煅烧2 h,得到纳米晶YAG∶Ce荧光粉;随着铈浓度的增加,荧光粉发射光谱发生红移,激发光谱基本不变.

参考文献

[1] Xiong Zhaoxian,Song Chunxiao,Wu Wei,Qiu Hong.Effect of Sintering Time on Luminescent Properties of YAG:Ce3+ Phosphors[J].稀土学报(英文版),2004(z1):137-139.
[2] Ruan SK.;Zhong AM.;Duan JF.;Yang XB.;Su MZ.;Zhou JG. .Synthesis of Y3Al5O12 : Eu3+ phosphor by sol-gel method and its luminescence behavior[J].Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics,1998(0):72-75.
[3] Xia Li;Hong Liu;Jiyang Wang;Hongmei Cui;Feng Han .YAG:Ce nano-sized phosphor particles prepared by a solvothermal method[J].Materials Research Bulletin: An International Journal Reporting Research on Crystal Growth and Materials Preparation and Characterization,2004(12):1923-1930.
[4] Fangli Yuan;Hojin Ryu .Ce-doped YAG phosphor powders prepared by co-precipitation and heterogeneous precipitation[J].Materials Science & Engineering, B. Solid-State Materials for Advanced Technology,2004(1):14-18.
[5] Ji-Guang Li;Takayasu Ikegami .Co-precipitation synthesis and sintering of yttrium aluminum garnet (YAG) powders: the effect of precipitant[J].Journal of the European Ceramic Society,2000(14/15):2395-2405.
[6] 童祜嵩.颗粒粒度与比表面测量原理[M].上海:上海科学技术文献出版社,1989
[7] 陈积阳;施鹰;施剑林.复合沉淀法制备(Y,Gd)2O3:Eu纳米粉体及其发光性能[J].
[8] 闻雷,孙旭东,马伟民.共沉淀法制备YAG超细粉及透明陶瓷[J].功能材料,2004(01):89-91.
[9] 吴瑾光.近代博里叶变换红外光谱技术及应用[M].北京:科学技术文献出版社,1994
[10] 苏静;张庆礼;谷长江.共沉淀法YAG、Nd∶YAG纳米粉体的制备、结构与光谱性能研究[J].
[11] 姚光庆,冯艳娥,段洁菲,林建华.氮化镓发光二级管蓝光转换材料的合成和发光性质[J].物理化学学报,2003(03):226-229.
[12] 刘如熹,石景仁.白光发光二极管用钇铝石榴石萤光粉配方与机制研究[J].中国稀土学报,2002(06):495-501.
[13] Yonghui Zhou;Jun Lin;Min Yu .Synthesis-dependent luminescence properties of Y_3Al_5O_(12):Re~(3+) (Re = Ce, Sm, Tb) phosphors[J].Materials Letters,2002(5):628-636.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%