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外延PbZr_(0.4)Ti_(0.6)O_3薄膜的电光效应

The Electro-optic Effects in Epitaxial PbZr_(0.4)Ti_(0.6)O_3 Thin Films
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摘要 从Landau-Devonshire唯象理论出发,通过热力学分析得到PbZr0.4Ti0.6O3薄膜的电光效应与厚度和外加电场的关系。结果表明,生长在SrTiO3衬底上的PbZr0.4Ti0.6O3薄膜,其线性电光系数和二次电光系数都随薄膜厚度的增加而增大,且在临界厚度附近趋于饱和,对50nm厚的PbZr0.4Ti0.6O3薄膜,线性电光系数和二次电光系数分别为7.2×10-11m/V和0.31×10-18m2/V2,双折射变化随外加电场改变,由线性电光效应引起的双折射变化比二次电光效应引起的双折射变化明显。 The relationship between the electro-optic(EO) effect of PbZr0.4Ti0.6 O3 thin film and the film thickncss and the additional electric field has been obtained by using the thermodynamic analysis via the Landau-Devonshire's phenomenological theory. The results show that the linear andquadratic EO coefficients increase with the increase of film thickness and become saturated when the film thickness is close to the critical thickness of PbZr0. 4 Ti0.6 O3 thin film on SrTiO3 substrate. The linear and quadratic EO coefficients are about 7.2 × 10^-11 m/V and 0.31 × 10^-18 m^2/V^2 respectively for 50 nm PbZr0.4Ti0.6 O3 thin film. The hirefringence change depends on the electric field, and the change resulted from the linear EO effect is more prominent than that resulted from the quadratic EO effect.
出处 《压电与声光》 CSCD 北大核心 2009年第5期728-731,共4页 Piezoelectrics & Acoustooptics
基金 "九七三"前期研究专项基金资助项目(2007CB616910) 国家自然科学基金资助项目(50572021) 河北省自然科学基金资助项目(E2005000130) 国家人事部留学人员择优基金资助项目(G05-06) 教育部留学回国人员科研启动基金资助项目(2005-546) 河北大学科研基金资助项目
关键词 铁电薄膜 电光效应 电光系数 ferroelectric thin film electro-optic effect electro-optic coefficient
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参考文献20

  • 1KANG Y M, BAIK S. Microstructure and optical loss in epitaxial (Pb, La)TiO3 thin films on (001) MgO [J]. J Mater Res,1998,13(4):995-1 001.
  • 2LINES M E,GLASS A M. Principles and applications of ferroelectrics and related material [M]. Oxford: Clarendon Press, 1977.
  • 3陈捷,曹永良,章献民,陈抗生,邹英寅.基于透明铁电陶瓷的高速可变光衰减器[J].压电与声光,2006,28(1):21-22. 被引量:3
  • 4熊和金,李兴教.铁电畴层波的电光效应[J].压电与声光,1996,18(4):252-254. 被引量:1
  • 5BLOMQVIST M, KHARTSEV S, GRISHIN A. Electrooptic /erroelectric Na0.5 K0.5 NbO3 films [J]. IEEE Photonics Technol Lett, 2005, 17(8) : 1 638-1 640.
  • 6DIDOMENICO M J R, WEMPLE S H. Oxygen- octahedra ferroeleetrics I theory of electro-optical and nonlinear optical effects [J]. J Appl Phys, 1969, 40(2): 720-734.
  • 7REITZE D H,HATON E,RAMESH R,et al. Electrooptic properties of single crystalline ferroelectric thin films [J]. Appl Phys Lett, 1993, 63(5): 596-598.
  • 8KIM D Y, MOON S E, KIM E K, et al. Electro-optic characteristics of (001)-oriented Ba0.6 Sr0.4 TiO3 thin films [J].Appl Phys Lett, 2003, 82(9) : 1 455-1 457.
  • 9WANG D Y,WANG J ,CHAN H L W,et al. Structur-al and electro-optic properties of Ba0.7 Sr0.3 TiO3 thin films grown on various suhstrates using pulsed laser deposition [J]. J Appl Phys, 2007, 101(4):043515 (1-6).
  • 10QIU J H,JIANG Q. Film thickness dependence of electro-optic effects in epitaxial Ba0.7 Sr0.3 TiO3 thin films[J].J ApplPhys, 2007, 102(7): 074101(1-5).

二级参考文献31

  • 1曾华荣,余寒峰,初瑞清,李国荣,殷庆瑞,唐新桂.PZT铁电薄膜纳米尺度铁电畴的场致位移特性[J].物理学报,2005,54(3):1437-1441. 被引量:11
  • 2郑分刚,陈建平,李新碗.(111)择优取向的Pb(Zr_(0.52)Ti_(0.48))O_3铁电薄膜的制备及研究[J].物理学报,2006,55(6):3067-3072. 被引量:8
  • 3GR-910-CORE. Telcordia's Generic Requirements for Fiber Optic Attenuators[S].
  • 4BASHIR A, KATILA P. A MEMS-based VOA with very low PDL[J]. IEEE Photon Technol Lett, 2004,16(4):1 047-1 049.
  • 5SATO K,AOKI T. Development of a variable optical attenuator[J]. Furukawa Review, 2001(20) :15-20.
  • 6HIRABYASHI K, AMANO C. Feed-forward continuous and complete polarization control with a PLZT rotatable-variable waveplate and inline polarimeter[J].J Lightwave Technol, 2003, 21(9): 1 920-1 932.
  • 7李兴教,Ferroelectrics,1983年,47卷,3页
  • 8李兴教,J Appl Phys,1989年,66卷,10期,4928页
  • 9李兴教,J Appl Phys,1987年,61卷,6期,2327页
  • 10李兴教,华中理工大学学报,1985年,13卷,1页

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