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质子导体SrCe_(0.9)Y_(0.1)O_(3-δ)电解质薄膜的溶胶凝胶法制备 被引量:2

Synthesis of Proton Conducting SrCe_(0.9)Y_(0.1)O_(3-δ) Electrolyte Film by a Sol-Gel Method
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摘要 以硝酸盐为原料,乙二醇为络合剂,采用溶胶凝胶法制备了质子导体SrCe0.9Y0.1O3-δ电解质薄膜。使用TG/DSC和XRD对凝胶前驱体的热分解过程及相组成进行了表征。探讨了溶胶凝胶制备SrCe0.9Y0.1O3-δ电解质的反应过程:凝胶前驱体由C3H3CeO6和Sr(NO3)2构成;Sr(NO3)2在630℃分解,并部分生成SrCO3中间相;SrCO3在865℃分解完全,并与CeO2反应最终得到SrCeO3。900℃热处理得到的SrCe0.9Y0.1O3-δ电解质薄膜致密、均匀,无气孔和微裂纹,为钙钛矿型SrCeO3相。热力学计算表明电解质凝胶前驱体生成SrCeO3的热分解反应过程能够达到的最高理论温度为1455.4℃,高于SrCeO3生成所需温度764.6℃,在热力学上有利于SrCeO3相生成。 The proton conducting SrCe0.9Y0.1O3-δ electrolyte film was synthesized by a sol-gel method using nitrates and ethylene glycol. The thermal decomposition behavior and phases of precursor were characterized by using TG/DSC and XRD. It was found that the precursor was consisted of C3H3 CeO6 and Sr( NO3 )2. At 630 ℃ , Sr( NO3 )2 decomposed and partly formed SrCO3 with ambient CO2. SrCO3 decomposed at 865 ℃ and reacted with CeO2 to form SeCeO3 eventually. XRD result indicated that SrCe0.9Y0.1O3-δ electrolyte film annealed at 900 ℃ was perovskite SrCeO3. The film had a dense and homogeneous microstructure, and no holes or cracks was de- tected. Moreover, the reaction temperature of SrCe0.9Y0.1O3-δ precursor was determined to be 1455.4℃ by thermodynamic calculation, which was higher than the required SrCeO3 synthesis temperature of 764.6 ℃, thus in favor of the formation of SrCeO3.
出处 《稀有金属》 EI CAS CSCD 北大核心 2012年第6期936-941,共6页 Chinese Journal of Rare Metals
基金 国家科技部ITER"973"计划(2010GB113003)资助项目
关键词 质子导体 SrCeO3 电解质薄膜 溶胶凝胶法 :proton conducting electrolyte SrCeO3 electrolyte film sol-gel method
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  • 1伊长虹,胡芳仁,张庆刚,陈莺飞,徐小平,郑东宁.密封容器中后处理制备Tl_2Ba_2CaCu_2O_y高温超导薄膜及其性能研究[J].物理学报,2004,53(10):3525-3529. 被引量:7
  • 2梅贤功,袁明亮,陈荩.论残钠在高铁赤泥煤基直接还原过程中之作用[J].轻金属,1995(4):20-22. 被引量:10
  • 3彭珍珍,郭瑞松,尹自光,李娟,蔡舒.BaZrO_3/NaOH复相质子导体的制备与性能[J].稀有金属材料与工程,2007,36(A02):596-598. 被引量:9
  • 4Sheng Z Z, Hermann A M, El Ali A, Almasan C, Estrada J, Datta T, Matson R J. Superconductivity at 90 K in the TI-Ba-Cu-O system [ J ]. Phys. Rev. Lett. , 1988, 60( 10): 937.
  • 5Sheng Z Z, Herman A M. Superconductivity in the rare-earth-free T1-Ba-Cu-O system above liquid-nitrogen temperature [J]. Nature, 1988, 332(6159): 55.
  • 6Yan S L, Fang L, Song Q X, Yan J, Zhu Y P, Chen J H, Zhang S B. Formation of epitaxial Tl2 Ba2 CaCu2 O8 thin films at low temperature in pure argon [J ]. Appl. Phys. Lett. , 1993, 63(13) : 1845.
  • 7Li S L, Chen Y F, Xu X P. Fabrication of double-si- ded Tl2 Ba2CaCu2O8 thin films on 2-in LaAlO3 substrates by pulsed laser deposition and post-annealing [ J ]. Phys- ica C, 2007, 460-462: 1369.
  • 8Yan S L, Fang L, Si M S, Wang J, Cao H L, Song Q X, Zhou X D, Hao J M. The stability of epitaxial Tl2Ba2CaCu2O8 thin films in water [ J ]. Solid State Comm. , 1996, 98(8) : 723.
  • 9Pica G, Andreone A, Palomba F, Salluzzo M, Vaglio R, Malandrino G, Ancarani V, Fragala I L, Cassinese A, Muller G. Synthesis and microwave properties of Tl2Ba2CaCu2O8 superconducting films grown by MOCVD [J]. Eur. Phys. J. B, 2000, 18(3):405.
  • 10Zhang X F, Sung Y S, Miller D J, Hinds B J, McNeely R J, Studebaker D L, Marks T J. New structural as- pects of Tl2Ba2CaCu2Oy epitaxial thin films grown by MOCVD on LaAIO3 [ J ]. Physica C, 1997, 275 ( 1- 2): 146.

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