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Transparent electro-optic (EO) ceramics of La-doped 0.75Pb(Mg1/3Nb2/3)O3–0.25PbTiO3 (0.75PMN–0.25PT) were prepared successfully. High transparency of 69% in the near-infrared (IR) wavelength (1550 nm) was achieved at 2 mol% La doping, meanwhile it shows an extremely high quadratic EO coefficient of 45.4×10−16 m2·V−2, which is indispensable for applications in EO devices. The distribution of a polar nanodomain structure of the samples experiences disorder–order–disorder evolution in a La doping range. It is found that a parallelly-stacked polar nanodomain structure with an easier and faster polarization switching in the 2 mol% La-doped sample suggests that an ordering distribution of polar nanoregions would be critical to inducing large EO effect, transparency, and piezoelectric response. A triple-cavity tunable optical filter (TOF) with a single transmission peak and a tuning voltage below 30 V in a tuning range of 190–197 THz was designed based on our ceramics. The work is believed to bridge the relationship among doping-engineering, EO properties, and polarization behavior, which would guide the further optimization of transparent EO ceramics.


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La-doped PMN–PT transparent ceramics with ultra-high electro-optic effect and its application in optical devices

Show Author's information Ming HuaZhongcan ChangcNan NieaZhujun WancWen Donga,b( )Qiuyun Fua,b( )
School of Integrated Circuits, Wuhan National Laboratory for Optoelectronics & Optical Valley Laboratory, Huazhong University of Science and Technology, Wuhan 430074, China
Research Institute of Huazhong University of Science and Technology in Shenzhen, Shenzhen 518000, China
National Engineering Research Center of Next Generation Internet Access-system, Wuhan 430074, China

Abstract

Transparent electro-optic (EO) ceramics of La-doped 0.75Pb(Mg1/3Nb2/3)O3–0.25PbTiO3 (0.75PMN–0.25PT) were prepared successfully. High transparency of 69% in the near-infrared (IR) wavelength (1550 nm) was achieved at 2 mol% La doping, meanwhile it shows an extremely high quadratic EO coefficient of 45.4×10−16 m2·V−2, which is indispensable for applications in EO devices. The distribution of a polar nanodomain structure of the samples experiences disorder–order–disorder evolution in a La doping range. It is found that a parallelly-stacked polar nanodomain structure with an easier and faster polarization switching in the 2 mol% La-doped sample suggests that an ordering distribution of polar nanoregions would be critical to inducing large EO effect, transparency, and piezoelectric response. A triple-cavity tunable optical filter (TOF) with a single transmission peak and a tuning voltage below 30 V in a tuning range of 190–197 THz was designed based on our ceramics. The work is believed to bridge the relationship among doping-engineering, EO properties, and polarization behavior, which would guide the further optimization of transparent EO ceramics.

Keywords: polarization, transmittance, domain reversal, Pb(Mg1/3Nb2/3)O3–PbTiO3 (PMN–PT) electro-optic (EO) ceramics, tunable optical filter (TOF)

References(37)

[1]
Jiang H, Zou YK, Chen Q, et al. Transparent electro-optic ceramics and devices. In: Proceedings of the Optoelectronic Devices and Integration, Beijing, China, 2005: 380–394.
DOI
[2]
Ji J, Zheng SL, Jin XF, et al. Optical variable gain tilt filter with temperature compensation. Microw Opt Techn Let 2010, 52: 1906–1909.
[3]
Ye Q, Qiao L, Gan JL, et al. Fiber Sagnac π-shifted interferometer for a polarization-independent PMNT high-speed electro-optic switch. Opt Lett 2010, 35: 4187–4189.
[4]
Zhang XJ, Ye Q, Qu RH, et al. High-power electro-optic switch technology based on novel transparent ceramic. Chin Phys B 2016, 25: 034202.
[5]
Zhu B, Zeng X, Qiu PS, et al. Effects of Bi3+ doping on the optical and electric-induced light scattering performance of PLZT (8.0/69/31) transparent ceramics. Materials 2019, 12: 1437.
[6]
Shopa M, Shopa Y, Kostenyukova E, et al. Optical activity and electro-optic effect of L-arginine doped KDP single crystals. Opt Laser Technol 2019, 119: 105655.
[7]
Zou KY, Zhang R, Chen CM, et al. The field induced scattering in PLZT electro-optic materials. In: Proceedings of the Conference on Lasers and Electro-Optics, Baltimore, USA, 2003: CWA21.
[8]
Ruan W, Li GR, Zeng JT, et al. Large electro-optic effect in La-doped 0.75Pb(Mg1/3Nb2/3)O3–0.25PbTiO3 transparent ceramic by two-stage sintering. J Am Ceram Soc 2010, 93: 2128–2131.
[9]
Londono FA, Eiras JA, Garcia D. New transparent ferroelectric ceramics with high electro-optical coefficients: PLMN–PT. Ceramica 2011, 57: 404–408. (in Portuguese)
[10]
Badillo FAL, Eiras JA, Milton FP, et al. Preparation and microstructural, structural, optical and electro-optical properties of La doped PMN–PT transparent ceramics. Opt Photonics J 2012, 2: 157–162.
[11]
Si SY, Zhang CJ, Li XH, et al. Microstructure analysis on the high transparent 0.88PMN–0.12PT ferroelectric ceramics prepared by pressureless sintering. Journal of Chinese Electron Microscopy Society 2014, 33: 495–498. (in Chinese)
[12]
Ji WL, He XY, Zeng X, et al. Effects of PMN/PT ratio on optical and electro-optic properties of PLMNT transparent ceramics. Ceram Int 2015, 41: 10387–10393.
[13]
Fujii I, Nakashima S, Wada T. Fabrication and electro-optic properties of 0.9Pb[(Mg,Zn)1/3Nb2/3]O3–0.1PbTiO3 transparent ceramics by a conventional sintering technique. Jpn J Appl Phys 2017, 56: 10PC04.
[14]
Fang Z, Jiang XD, Tian X, et al. Ultratransparent PMN–PT electro-optic ceramics and its application in optical communication. Adv Opt Mater 2021, 9: 2002139.
[15]
Zhou S, Lin DB, Su YM, et al. Enhanced dielectric, ferroelectric, and optical properties in rare earth elements doped PMN–PT thin films. J Adv Ceram 2021, 10: 98–107.
[16]
Zheng FJ, Tian X, Fang Z, et al. Sm-doped PIN–PMN–PT transparent ceramics with high Curie temperature, good piezoelectricity, and excellent electro-optical properties. ACS Appl Mater Interfaces 2023, 15: 7053–7062.
[17]
Swartz SL, Shrout TR. Fabrication of perovskite lead magnesium niobate. Mater Res Bull 1982, 17: 1245–1250.
[18]
Kang W, Zheng SL, Zhang XM, et al. Quadratic electro-optic properties of Pb(Mg1/3Nb2/3)O3–PbTiO3 transparent ceramics under both DC and AC bias. Appl Optics 2012, 51: 2870–2876.
[19]
Haertling GH. Ferroelectric ceramics: History and technology. J Am Ceram Soc 1999, 82: 797–818.
[20]
Winter MR, Pilgrim SM, Lejeune M. Study on the effects of lanthanum doping on the microstructure and dielectric properties of 0.9Pb(Mg1/3Nb2/3)O3–0.1PbTiO3. J Am Ceram Soc 2001, 84: 314–320.
[21]
Song ZZ, Zhang YC, Lu CJ, et al. Fabrication and ferroelectric/dielectric properties of La-doped PMN–PT ceramics with high optical transmittance. Ceram Int 2017, 43: 3720–3725.
[22]
Haertling GH. PLZT electrooptic materials and applications—A review. Ferroelectrics 1987, 75: 25–55.
[23]
Li F, Cabral MJ, Xu B, et al. Giant piezoelectricity of Sm-doped Pb(Mg1/3Nb2/3)O3–PbTiO3 single crystals. Science 2019, 364: 264–268.
[24]
Luo C, Karaki T, Wang ZK, et al. High piezoelectricity after field cooling AC poling in temperature stable ternary single crystals manufactured by continuous-feeding Bridgman method. J Adv Ceram 2022, 11: 57–65.
[25]
Chu F, Reaney IM, Setter N. Spontaneous (zero-field) relaxor-to-ferroelectric-phase transition in disordered Pb(Sc1/2Nb1/2)O3. J Appl Phys 1995, 77: 1671–1676.
[26]
Wang HX, Xu HQ, Luo HS, et al. Dielectric anomalies of the relaxor-based 0.9Pb(Mg1/3Nb2/3)O3–0.1PbTiO3 single crystals. Appl Phys Lett 2005, 87: 012904.
[27]
Ruan W, Li GR, Zeng JT, et al. Origin of the giant electro-optic Kerr effect in La-doped 75PMN–25PT transparent ceramics. J Appl Phys 2011, 110: 074109.
[28]
Chen QS, Jiang H, Zou YK, et al. Fast, widely tunable electro-optic Fabry–Perot filter. In: Proceedings of the Quantum Electronics and Laser Science Conference 2005, Baltimore, USA, 2005: JTuC66.
[29]
Xu ZW, Zeng X, Cao ZD, et al. Effects of barium substitution on the optical and electrical properties of PLZT transparent electro-optical ceramics. Ceram Int 2019, 45: 17890–17897.
[30]
Westphal V, Kleemann W, Glinchuk MD. Diffuse phase transitions and random-field-induced domain states of the “relaxor” ferroelectric PbMg1/3Nb2/3O3. Phys Rev Lett 1992, 68: 847–850.
[31]
Hilton AD, Barber DJ, Randall CA, et al. On short range ordering in the perovskite lead magnesium niobate. J Mater Sci 1990, 25: 3461–3466.
[32]
Xu GY, Zhong Z, Bing Y, et al. Electric-field-induced redistribution of polar nano-regions in a relaxor ferroelectric. Nat Mater 2006, 5: 134–140.
[33]
Hirota K, Ye ZG, Wakimoto S, et al. Neutron diffuse scattering from polar nanoregions in the relaxor Pb(Mg1/3Nb2/3)O3. Phys Rev B 2002, 65: 104105.
[34]
Slodczyk A, Daniel P, Kania A. Local phenomena of (1−x)PbMg1/3Nb2/3O3xPbTiO3 single crystals (0 ≤ x ≤ 0.38) studied by Raman scattering. Phys Rev B 2008, 77: 184114.
[35]
Chen C, Wang Y, Li ZY, et al. Evolution of electromechanical properties in Fe-doped (Pb,Sr)(Zr,Ti)O3 piezoceramics. J Adv Ceram 2021, 10: 587–595.
[36]
Zhao XH, Qu WG, He H, et al. Influence of cation order on the electric field-induced phase transition in Pb(Mg1/3Nb2/3)O3-based relaxor ferroelectrics. J Am Ceram Soc 2006, 89: 202–209.
[37]
Janner D, Tulli D, García-Granda M, et al. Micro-structured integrated electro-optic LiNbO3 modulators. Laser Photonics Rev 2009, 3: 301–313.
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Received: 02 April 2024
Revised: 04 December 2024
Accepted: 05 April 2024
Published: 19 June 2023
Issue date: July 2023

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© The Author(s) 2023.

Acknowledgements

This work was supported by the National Natural Science Foundation of China (Grant No. 61971459), the Fund from Science, Technology and Innovation Commission of Shenzhen Municipality (Grant No. JCYJ20190809095009521), and the Innovation Team Program of Hubei Province, China (Grant No. 2019CFA004), the Innovation Fund of Wuhan National Laboratory for Optoelectronics & Optical Valley Laboratory (WNLO), and 2022 Shenzhen Central Leading Local Science and Technology Development Special Funding Program Virtual University Park Laboratory Project. The authors thank the Analytical and Testing Center, Huazhong University of Science and Technology (HUST) for providing the SEM, PFM, and XRD measurements.

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