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研究生: 張宸
Jhang, Chen
論文名稱: 鎂摻雜之鈦酸鋇的製備、分析與介電性質
Preparation‚Characterization‚and Dielectric Properties of Magnesium-Doped Barium Titanates.
指導教授: 黃啓原
Huang, Chi-Yuen
學位類別: 碩士
Master
系所名稱: 工學院 - 資源工程學系
Department of Resources Engineering
論文出版年: 2021
畢業學年度: 109
語文別: 中文
論文頁數: 96
中文關鍵詞: 鈦酸鋇 、鎂摻雜 、晶體結構 、介電常數 、絕緣電阻
外文關鍵詞: Barium Titanate, Magnesium, Crystal Structure, Dielectric Constant, Insulation Resistance
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  • 目前市面上的多層陶瓷電容為求降低生產成本,多以卑金屬材料作為電極。鈦酸鋇陶瓷為了避免電極氧化而必須在還原氣氛下燒結,因此容易出現半導化的現象,造成整體絕緣電阻下降。為了改善此現象,可以藉由添加低價離子去取代高價離子,形成受體補償以抑制半導化現象。
    本研究使用固態反應法合成出鎂摻雜鈦酸鋇Ba(Ti1-xMgx) O3-x之介電材料,藉由不同添加量之鎂離子取代鈦酸鋇中Ti的位置,了解鎂離子進入鈦酸鋇Ti位置後,對晶體結構、晶格參數、拉曼光譜、比表面積、顯微結構以及介電性質之影響,進而探討此材料在積層陶瓷電容應用之可行性。
    實驗結果顯示,將Ba( Ti1-xMgx) O3-x (x = 0、0.01、0.03) 粉末透過二階段煅燒可以成功合成出無二次相之鎂摻雜鈦酸鋇粉末,再透過Rietveld refinement精算得知,當Mg2+進入鈦酸鋇後,單位晶格內的a軸會伸長、c軸會縮短,造成正方性下降,並使晶格體積上升,此部分結果與文獻[1]中,Mg2+進入Ti位置之結果相符合;拉曼光譜分析中,所有tetragonal phase之特徵峰強度也下降且寬化,此現象表示鈦酸鋇由tetragonal phase漸漸轉變為cubic phase,此結果與Rietveld refinement精算之結果相吻合,證實了Mg2+確實是進入Ti-site,而非相同價數之Ba-site。在介電性質方面,Mg2+添加會使鐵電性降低,得到較低的介電常數,居里溫度會隨著Mg2+添加而下降,使居里溫度往低溫平移,並且造成介電常數峰的寬化。在絕緣電阻方面,Mg2+添加沒有使絕緣電阻能有效提升,推測是因為添加劑成分分布不均勻,導致晶粒大小分布不均使晶界分率降低,所以整體絕緣電阻沒有預期的提升。

    In this study, using solid-state reaction method to synthesize Mg-doped barium titanate Ba(Ti1-xMgx)O3-x dielectric material. Understand the influence of Mg2+ into the Ti-site of BaTiO3 on the crystal structure, lattice parameters, Raman spectrum, specific surface area, microstructure and dielectric properties, and then discuss the feasibility of the application of this material in MLCCs.
    The experimental results show that Ba(Ti1-xMgx)O3-x (x = 0, 0.01, 0.03) powder can be synthesized high purity Mg-doped BaTiO3 powder through two-stage calcination. And then through Rietveld refinement. It is known that when Mg2+ into BaTiO3, the a-axis will be extended and the c-axis will be shortened, and an increase in the volume of the crystal lattice. The result of Ti-site is consistent; in Raman spectroscopy analysis, the characteristic peak intensity of all tetragonal phase also decreases and broadens. This phenomenon indicates that BaTiO3 gradually transforms from tetragonal to cubic phase. This result is consistent with the result of Rietveld refinement. The coincidence confirms that Mg2+ is indeed into Ti-site, not Ba-site. In terms of dielectric properties, the concentration of Mg2+ will reduce the ferroelectricity, resulting in a lower dielectric constant. The Curie temperature will decrease with the concentration of Mg2+, and causing the dielectric constant peak Broaden. In terms of insulation resistance, the Mg-doped did not effectively improve the insulation resistance. It is presumed that the uneven distribution of the additive composition results in uneven grain size distribution and the reduction of the grain boundary fraction, so the overall insulation resistance did not improve as expected.

    摘要 I 誌謝 XV 目錄 XVI 表目錄 XIX 圖目錄 XX 第一章 緒論 1 1-1 前言 1 1-2 研究目的 2 第二章 前人文獻回顧及理論基礎 3 2-1 鈦酸鋇晶體結構及性質 3 2-2 鈦酸鋇的介電性質 6 2-3 鈦酸鋇的晶粒效應 9 2-4 鋇鈦比對鈦酸鋇之影響 11 2-4-1 Ba-rich之影響 13 2-4-2 Ti-rich之影響 13 2-5 置換作用 17 2-5-1 置換原理 17 2-5-2 容忍因子 19 2-6 添加物對鈦酸鋇之影響 21 2-6-1 同價離子添加對鈦酸鋇性質之影響 21 2-6-2 異價離子添加對鈦酸鋇性質之影響 23 2-6-3 添加鎂離子對鈦酸鋇之影響 26 2-7 鈦酸鋇半導化現象及改善 30 2-8 拉曼光譜分析 31 2-8-1 拉曼光譜原理 31 2-8-2 拉曼光譜在鈦酸鋇上之研究 31 2-9 介電理論 34 2-9-1 介電常數 34 2-9-2 介電損耗 35 第三章 實驗方法與實驗流程 36 3-1 粉末製備與分析 38 3-1-1 起始原料 38 3-1-2 鎂摻雜鈦酸鋇粉末之製備 38 3-1-3 粉末之熱差/熱重分析 40 3-1-4 X光粉末繞射分析 40 3-1-5 晶格常數之分析 42 3-1-6 拉曼光譜分析 42 3-1-7 掃描式電子顯微鏡與顯微結構分析 42 3-1-8 比表面積分析 44 3-2 陶瓷體製備與分析 45 3-2-1 陶瓷體製備 45 3-2-2 燒結收縮曲線分析 45 3-2-3 陶瓷體密度量測 47 3-2-4 掃描式電子顯微鏡與顯微結構分析 47 3-3 電性分析 48 3-3-1 陶瓷體電性量測樣品準備 48 3-3-2 介電常數與電容變化率 48 3-3-3 絕緣電阻量測 49 第四章 結果與討論 50 4-1 起始粉末分析 50 4-1-1 起始粉末之預燒 50 4-1-2 結晶相分析 50 4-1-3 顯微結構分析 53 4-2 起始混合粉末之熱差/熱重分析 55 4-3 煅燒粉末之分析 58 4-3-1 結晶相分析 58 4-3-2 晶格常數分析 63 4-3-3 拉曼分析 68 4-3-4 比表面積分析 70 4-3-5 顯微結構分析 73 4-4 陶瓷體分析 79 4-4-1 燒結收縮曲線量測 79 4-4-2 陶瓷體密度量測 82 4-4-3 顯微結構分析 84 4-4-4 介電性質與絕緣電阻分析 88 第五章 結論 92 參考文獻 93

    [1] R. Machado, A. Di Loreto, A. Frattini, M. Sepliarsky, and M. Stachiotti, “Site Occupancy Effects of Mg Impurities in BaTiO3,” Journal of Alloys and Compounds, vol. 809, pp. 151847, 2019.
    [2] W. D. Kingery, H. K. Bowen, and D. R. Uhlmann, Introduction to Ceramics, America: John wiley & sons, 1976.
    [3] 吳朗,電工材料: 全華圖書,2012.
    [4] L.-C. Dufour and C. Monty, Surfaces and Interfaces of Ceramic Materials: Springer Science & Business Media, 2012.
    [5] D. Rase and R. Roy, “Phase Equilibria in the System BaO–TiO2,” Journal of the American Ceramic Society, vol. 38, no. 3, pp. 102-113, 1955.
    [6] G. Arlt, D. Hennings, and G. De With, “Dielectric Properties of Fine‐Grained Barium Titanate Ceramics,” Journal of Applied Physics, vol. 58, no. 4, pp. 1619-1625, 1985.
    [7] S. Lee, Z.-K. Liu, M.-H. Kim, and C. A. Randall, “Influence of Nonstoichiometry on Ferroelectric Phase Transition in BaTiO3,” Journal of Applied Physics, vol. 101, no. 5, pp. 054119, 2007.
    [8] S. Lee, C. A. Randall, and Z. K. Liu, “Modified Phase Diagram for the Barium Oxide–Titanium Dioxide System for the Ferroelectric Barium Titanate,” Journal of the American Ceramic Society, vol. 90, no. 8, pp. 2589-2594, 2007.
    [9] Y. Hu, M. P. Harmer, and D. M. Smyth, “Solubility of BaO in BaTiO3,” Journal of the American Ceramic Society, vol. 68, no. 7, pp. 372-376, 1985.
    [10] S. H. Yoon, J. H. Lee, D. Y. Kim, and N. M. Hwang, “Effect of the Liquid‐Phase Characteristic on the Microstructures and Dielectric Properties of Donor‐(Niobium) and Acceptor‐(Magnesium) Doped Barium Titanate,” Journal of the American Ceramic Society, vol. 86, no. 1, pp. 88-92, 2003.
    [11] R. Sharma, N. H. Chan, and D. Smyth, “Solubility of TiO2 in BaTiO3,” Journal of the American Ceramic Society, vol. 64, no. 8, pp. 448-451, 1981.
    [12] C. G. Bergeron and S. H. Risbud, Introduction to Phase Equilibria in Ceramics, America: Wiley, 1984.
    [13] R. D. Shannon, “Revised Effective Ionic Radii and Systematic Studies of Interatomic Distances in Halides and Chalcogenides,” Acta Crystallographica Section A: Crystal Physics, Diffraction, Theoretical and General Crystallography, vol. 32, no. 5, pp. 751-767, 1976.
    [14] O. Muller and R. Roy, The Major Ternary Structural Families, Berlin-Heidelberg-New York: Springer-Verlag, 1974.
    [15] C. Schinzer, "Distortion of Perovskites," Retrieved, 2012.
    [16] J. Lin and T. Wu, “Effects of Isovalent Substitutions on Lattice Softening and Transition Character of BaTiO3 solid Solutions,” Journal of Applied Physics, vol. 68, no. 3, pp. 985-993, 1990.
    [17] D. Hennings, A. Schnell, and G. Simon, “Diffuse Ferroelectric Phase Transitions in Ba(Ti1‐yZry)O3 Ceramics,” Journal of the American Ceramic Society, vol. 65, no. 11, pp. 539-544, 1982.
    [18] D. Makovec, Z. Samardžija, U. Delalut, and D. Kolar, “Defect Structure and Phase Relations of Highly Lanthanum‐Doped Barium Titanate,” Journal of the American Ceramic Society, vol. 78, no. 8, pp. 2193-2197, 1995.
    [19] S. Sato, Y. Nakano, A. Sato, and T. Nomura, “Effect of Y-Doping on Resistance Degradation of Multi-Layer Ceramic Capacitors With Ni Electrodes under the Highly Accelerated Life Test,” Japanese Journal of Applied Physics, vol. 36, no. 9S, pp. 6016, 1997.
    [20] 汪建民,陶瓷技術手冊: 中華民國產業科技發展協進會,中華民國冶金學會,1999.
    [21] L. A. Xue, Y. Chen, and R. J. Brook, “The Influence of Ionic Radii on the Incorporation of Trivalent Dopants into BaTiO3,” Materials Science and Engineering: B, vol. 1, no. 2, pp. 193-201, 1988.
    [22] J. Jeong and Y. H. Han, “Effects of MgO-Doping on Electrical Properties and Microstructure of BaTiO3,” Japanese Journal of Applied Physics, vol. 43, no. 8R, pp. 5373, 2004.
    [23] M. T. Buscaglia, V. Buscaglia, M. Viviani, and P. Nanni, “Atomistic Simulation of Dopant Incorporation in Barium Titanate,” Journal of the American Ceramic Society, vol. 84, no. 2, pp. 376-84, 2001.
    [24] T. Nagai, K. Iijima, H. J. Hwang, M. Sando, T. Sekino, and K. Niihara, “Effect of MgO Doping on the Phase Transformations of BaTiO3,” Journal of the American Ceramic Society, vol. 83, no. 1, pp. 107-12, 2000.
    [25] S. T. Bae, D. K. Yim, K. S. Hong, J. S. Park, H. Shin, and H. S. Jung, “Role of Liquid Phase in Achieving a Fine Microstructure and Diffusive Phase Transition of MgO‐Doped BaTiO3,” International Journal of Applied Ceramic Technology, vol. 6, no. 6, pp. 679-686, 2009.
    [26] F. Kröger and H. Vink, Solid State Physics, New York: Academic Press, 1956.
    [27] O. Saburi, “Properties of Semiconductive Barium Titanates,” Journal of the Physical Society of Japan, vol. 14, no. 9, pp. 1159-1174, 1959.
    [28] 汪建民,材料分析: 中國材料科學學會發行,1998.
    [29] G. Burns and B. A. Scott, “Lattice Modes in Ferroelectric Perovskites: PbTiO3,” Physical Review B, vol. 7, no. 7, pp. 3088, 1973.
    [30] J. Freire and R. Katiyar, “Lattice Dynamics of Crystals with Tetragonal BaTiO3 Structure,” Physical Review B, vol. 37, no. 4, pp. 2074, 1988.
    [31] J. T. Last, “Infrared-Absorption Studies on Barium Titanate and Related Materials,” Physical Review, vol. 105, no. 6, pp. 1740, 1957.
    [32] U. D. Venkateswaran, V. M. Naik, and R. Naik, “High-Pressure Raman Studies of Polycrystalline BaTiO3,” Physical Review B, vol. 58, no. 21, pp. 14256, 1998.
    [33] A. C. Larson and R. B. Von Dreele, General Structure Analysis System (GSAS), New Mexico: Los Alamos National Laboratory, 2004.
    [34] H. Rietveld, “Line Profiles of Neutron Powder-Diffraction Peaks for Structure Refinement,” Acta Crystallographica, vol. 22, no. 1, pp. 151-152, 1967.
    [35] T. Nishino, “Formation Process of Metastable Phase (δ) of Alkaline‐Earth Carbonate,” Journal of the American Ceramic Society, vol. 70, no. 7, pp. C‐162-C‐164, 1987.
    [36] 張育綸,鹼土碳酸鹽與氧化物的固態反應過程中相生成及物質擴散之研究,資源工程學系碩博士班,國立成功大學,台南市,2010.
    [37] 王婉寧,氧化鎂及氧化釔添加對鈦酸鋇結構與介電性質之影響,資源工程學系碩博士班,國立成功大學,台南市,2012.
    [38] 張哲源,鈦酸鋇介電陶瓷之成分調整與結構及電容率平坦化的關聯,資源工程學系碩博士班,國立成功大學,台南市,2013.
    [39] E. Mejia-Uriarte, R. Sato-Berru, M. Navarrete, M. Villagrán-Muniz, C. Medina-Gutiérrez, and C. Frausto-Reyes, “Phase Transition of Polycrystalline BaTiO3 at High-Pressure Detected by a Pulsed Photoacoustic Technique,” Measurement Science and Technology, vol. 17, no. 6, pp. 1319, 2006.
    [40] C. Perry and D. Hall, “Temperature Dependence of the Raman Spectrum of BaTiO3,” Physical Review Letters, vol. 15, no. 17, pp. 700, 1965.
    [41] D. E. McCauley, M. S. Chu, and M. H. Megherhi, “PO2 Dependence of the Diffuse‐Phase Transition in Base Metal Capacitor Dielectrics,” Journal of the American Ceramic Society, vol. 89, no. 1, pp. 193-201, 2006.
    [42] D. P. Dutta, M. Roy, N. Maiti, and A. K. Tyagi, “Phase Evolution in Sonochemically Synthesized Fe3+ Doped BaTiO3 Nanocrystallites: Structural, Magnetic and Ferroelectric Characterisation,” Physical Chemistry Chemical Physics, vol. 18, no. 14, pp. 9758-9769, 2016.
    [43] Y. Yang, H. Hao, L. Zhang, C. Chen, Z. Luo, Z. Liu, Z. Yao, M. Cao, and H. Liu, “Structure, Electrical, and Dielectric Properties of Ca Substituted BaTiO3 Ceramics,” Ceramics International, vol. 44, no. 10, pp. 11109-11115, 2018.
    [44] H. Gong, X. Wang, S. Zhang, H. Wen, and L. Li, “Grain Size Effect on Electrical and Reliability Characteristics of Modified Fine-Grained BaTiO3 Ceramics for MLCCs,” Journal of the European Ceramic Society, vol. 34, no. 7, pp. 1733-1739, 2014.

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