欢迎登录材料期刊网

材料期刊网

高级检索

利用丝网印刷工艺制备出稀土 Yb3+/Tm3+共掺杂的 Ba0.8 Sr0.2 TiO3铁电陶瓷厚膜,利用 XRD、SEM、EDS、Raman和荧光光谱仪研究了稀土掺杂对厚膜微结构和发光性能的影响.实验发现,在低掺杂量时Yb3+、Tm3+离子在BST晶格中首先替代B位离子,高掺杂量时则同时占据 A位和B位离子.掺杂后的厚膜仍表现为典型的铁电四方相结构.在800 nm近红外激光激发下,共掺杂的 BST 厚膜中的 Tm3+离子通过Yb3+离子的敏化作用在468与533 nm处实现了间接上转换蓝色与绿色荧光输出,分别对应于Tm3+离子的1 G4→3 H6跃迁和1 D2→3 F4跃迁.468 nm蓝色荧光强度随着 Yb3+、Tm3+离子比的增加先增强后减弱,在 Yb3+、Tm3+离子共掺比为2∶1达到最大,并对上转换发光的机理进行了分析.

The Yb3+/Tm3+ co-doped BST thick films were prepared by screen printing process on alumina sub-strates.The effect of rare earth ions doping on the microstructure and photoluminescence properties were inves-tigated.It was found that Tm3+ and Yb3+ ions substituted for B site ions when the concentration was small.The RE ions can substitute both A site and B site with increasing RE ions concentration.The PL spectra of the Yb, Tm co-doped BST thick films were measured with 800 nm excitation source at room temperature.The 468 nm blue up-conversion luminescence was assigned to 1 G4→3 H6 transition of the Tm3+,and the 533 nm green up-conversion luminescence was assigned to 1 D2→3 F4 transition of the Tm3+ with the sensitization of Yb3+.The in-tensity of the 468 nm luminescence peeks first became stronger then decreased as increasing the ratio of the Yb3+ and Tm3+,the luminescence intensity reached the maximum at the ratio of 2∶1 for Yb3+ and Tm3+.The mechanism of indirect up-conversion luminescence was also studied.

参考文献

[1] Kenyon A J .Recent developments in rare-earth doped ma-terials for optoelectronics[J].Progress in Quantum Electronics,2002,26:225-284.
[2] Animesh J .A review of visible,near-IR,and mid-IR transitions in rare-earth doped glass waveguides for re-mote sensing and LIDAR[J].Proc Spie,2006,6409:640918.1-64098.12.
[3] Aggarwal I D;Shaw B L;Sanghera J S .Chalcogenide glass fiber-based MID-IR sources and applications[J].Proc Spie,2007,6453:645312.1-645312.10.
[4] Huang ZM.;Jiang CP.;Yu JA.;Sun JL.;Chu JH.;Zhang ZH. .Infrared optical properties of Ba0.8Sr0.2TiO3 ferroelectric thin films[J].Applied physics letters,2000(22):3651-3653.
[5] N. K. Pervez;P. J. Hansen;R. A. York .High tunability barium strontium titanate thin films for rf circuit applications[J].Applied physics letters,2004(19):4451-4453.
[6] Ruan Kaibin;Chen Xinman;Liang Tong et al.Photolu-minescence and electrical properties of highly transparent(Bi,Eu)Ti3 O12 ferroelectric thin films on indium-tin-ox-ide-coated glass substrates[J].Journal of Applied Physics,2008,103:074101.1-074101.4.
[7] Jayadevan KP.;Tseng TY. .Composite and multilayer ferroelectric thin films: processing, properties and applications [Review][J].Journal of Materials Science. Materials in Electronics,2002(8):439-459.
[8] Xu Jin;Menesklou W;Ivers-Tiffee E .Processing and properties of BST thin films for tunable microwave de-vices[J].J Euro Ceram Soci,2004,24:1735-1739.
[9] Shou-Yi Kuo;Wen-Feng Hsieh .Structural and optical properties of erbium-doped Ba_(0.7)Sr_(0.3)TiO_(3) thin films[J].Journal of Vacuum Science & Technology, A. Vacuum, Surfaces, and Films,2005(4):768-772.
[10] R. Pazik;D. Hreniak;W. Strek;A. Speghini;M. Bettinelli .Structural and luminescence properties of Eu~(3+) doped Ba_xSr_(1-x)TiO_3 (BST) nanocrystalline powders prepared by different methods[J].Optical materials,2006(11):1284-1288.
[11] Zhang TJ;Wang J;Jiang J;Pan RK;Zhang BS .Microstructure and photoluminescence properties of Ho-doped (Ba,Sr)TiO3 thin films[J].Thin Solid Films: An International Journal on the Science and Technology of Thin and Thick Films,2007(20/21):7721-7725.
[12] Ryu JH;Choi JJ;Hahn BD;Park DS;Yoon WH .Ferroelectric and piezoelectric properties of 0.948(K0.5Na0.5)NbO3-0.052LiSbO(3) lead-free piezoelectric thick film by aerosol deposition[J].Applied physics letters,2008(1):12905-1-12905-3-0.
[13] Xu BM;White D;Zesch J;Rodkin A;Buhler S;Fitch J;Littau K .Characteristics of lead zirconate titanate ferroelectric thick films from a screen-printing laser transfer method[J].Applied physics letters,2005(19):2902-1-2902-3-0.
[14] Zhang Tianjin;Animesh J;Shen Shaoxiong et al.Lat-tice strain dependent optical transitions in Ho3+-ion doped barium strontium titante thin films[J].J MaterSci:Mater Electron,2009,20:190-194.
[15] Jingji Zhang;Jiwei Zhai;Xiujian Chou;Xi Yao .Influence Of Rare-earth Addition On Microstructure And Dielectric Behavior Of Ba_(0.6)sr_(0.4)tio_3 Ceramics[J].Materials Chemistry and Physics,2008(2/3):409-413.
[16] Naik R;Nazarko J J;Flattery C S et al.Temperature de-pendence of the Raman spectra of polycrystalline Ba1-x SrxTiO3[J].Physical Review B:Condensed Matter,2000,61(17):11367-11372.
[17] Tenne DA;Soukiassian A;Xi XX;Choosuwan H;Guo R;Bhalla AS .Lattice dynamics in BaxSr1-xTiO3 thin films studied by Raman spectroscopy[J].Journal of Applied Physics,2004(11):6597-6605.
[18] Yuzyuk YI.;Alyoshin VA.;Zakharchenko IN.;Sviridov EV.;Almeida A. Chaves MR. .Polarization-dependent Raman spectra of heteroepitaxial (Ba,Sr)TiO3/MgO thin films - art. no. 134107[J].Physical Review.B.Condensed Matter,2002(13):4107-0.
[19] 孟超,孟广政,宋增福.上转换发光的有效增强机制--上转换敏化[J].光谱学与光谱分析,2001(02):142-146.
[20] Lilia C C;Izilda M R;Luís V G et al.Enhancement of blue upconversion mechanism in YLiF4:Yb,Tm,Nd crystals[J].Journal of Applied Physics,2005,98:113504.1-113504.3.
[21] Duan Zhouchao;Zhang Junjie;He Dongbing et al.Up-conversion luminescence of Tm3+/Yb3+ codoped oxyflu-oride glasses pumped at 970 nm[J].Acta Optica Sinica,2005,25:1659-1663.
[22] Miniscalco W.J. .Erbium-doped glasses for fiber amplifiers at 1500 nm[J].Journal of Lightwave Technology: A Joint IEEE/OSA Publication,1991(2):234-250.
[23] Frangois Auzel .Upconversion and Anti-Stokes Processes with f and d Ions in Solids[J].Chemical Reviews,2004(1):139-173.
[24] 孙丽娜,谭俊,巴德纯,原培新.Er3+-Tm3+-Yb3+掺杂Bi4Ti3O12薄膜的上转换白色荧光和铁电性能[J].金属学报,2014(01):88-94.
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%