| 研究生: |
黃梓庭 Huang, Tzu-Ting |
|---|---|
| 論文名稱: |
基於電卡效應與緩衝層優化摻鋰鈮酸鈉鉀薄膜應用於無鉛壓電式力感測器之研究 Study on Lead-Free Piezoelectric Force Sensors Based on Electrocaloric Effect and Buffer Layer Optimized Li-Doped KNN Thin Films. |
| 指導教授: |
朱聖緣
Chu, Sheng-Yuan |
| 學位類別: |
碩士 Master |
| 系所名稱: |
電機資訊學院 - 電機工程學系 Department of Electrical Engineering |
| 論文出版年: | 2024 |
| 畢業學年度: | 112 |
| 語文別: | 中文 |
| 論文頁數: | 117 |
| 中文關鍵詞: | 溶膠凝膠法 、鈮酸鋰鈉鉀 、壓電 、MEMS力感測器 、電卡效應 |
| 外文關鍵詞: | sol-gel, LKNN, piezoelectric, MEMS force sensor, Electrocaloric effect |
| 相關次數: | 點閱:36 下載:0 |
| 分享至: |
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本研究利用溶膠凝膠法製備厚度約800nm的(Na0.5K0.5)NbO3 壓電薄膜,透過以下三種方法改善其結晶性:(1) 優化熱處理條件、(2) 不同摻雜元素比例以及(3) 添加緩衝層,探討壓電薄膜的機械性質與電性能的影響,包括XRD、SEM、EDS、εr、tanδ、P-E、d33等,找出最佳的材料參數。此外,透過電卡效應的量測,評估其應用於微機電系統(Micro Electro Mechanical Systems, MEMS) 力感測器的潛力。
首先,本研究發現以升溫速率30°C/s,退火溫度為660°C下退火5分鐘的條件下,可達到最佳的薄膜品質。EDS分析顯示(Na+K)/Nb的比例接近理論值1,表現出最佳的 KNN 晶相。第二階段透過摻雜Li元素於KNN晶格的A-site ,有效的改善因高溫而揮發的Na、K離子空缺,在摻雜量為0.06 mol% 時,獲得電性質良好的LKNN薄膜,其在頻率1 kHz下介電常數εr 為515.88、介電損耗tanδ為0.0493,殘餘極化量Pr為23.85 μC/cm2 ,壓電係數d33為68.2 pm/V。
第三階段透過添加緩衝層HfO2,改善薄膜與基板之間的界面應力,楊氏模量從108.7GPa略微下降至93.5GPa,硬度從5.39 GPa 減少至4.68 GPa,更進一步將材料的壓電係數d33提升至76.81 pm/V,殘餘極化量Pr為26.3 μC/cm2。電卡效應量測曲線顯示,在溫度範圍為328-330K時,材料在相對較低的電場變化範圍表現出最大的電熱響應,ΔT=15.31 K, ΔT/ΔE=0.38 Kmm/kV ,獲得和含鉛材料相近的電熱特性。
相比於傳統的壓電材料PZT,本研究製備的KNN 壓電薄膜具有環保無毒性、高壓電係數、高介電常數、低損耗等優點,在未來無鉛MEMS 高靈敏度的力感測器的領域上具有相當大的潛力。
In this study, (Na0.5K0.5)NbO3 piezoelectric thin films (~800 nm) were prepared using the sol-gel method. The crystallinity of the films was improved through: (1) optimizing heat treatment conditions, (2) varying doping element ratios, and (3) adding a buffer layer. Additionally, the potential application as force sensors in Micro Electro Mechanical Systems (MEMS) were evaluated through electrocaloric effect measurements. X-ray diffraction (XRD) and ferroelectric analysis revealed that KNN thin films under a heating rate of 30°C/s and an annealing temperature of 660°C, exhibited favorable film characteristics. Doping the KNN lattice's A-site with Li (0.06 mol) effectively improved the vacancies of Na and K ions caused by high temperatures, resulting in good electrical properties: dielectric constant (εr) of 515.88, dielectric loss (tanδ) of 0.0493, remnant polarization (Pr) of 23.85 μC/cm², and piezoelectric coefficient (d33) of 68.2 pm/V at 1 kHz. Subsequently, adding a HfO2 buffer layer reduced interfacial stress, slightly decreasing Young's modulus from 108.7 GPa to 93.5 GPa and hardness from 5.39 GPa to 4.68 GPa. Further enhanced the piezoelectric coefficient (d33) to 76.81 pm/V and remnant polarization (Pr) to 26.3 μC/cm². Electrocaloric effect measurement showed that material's largest electrothermal response (ΔT=15.31 K, ΔT/ΔE=0.38 Kmm/kV) occurred within the 328-330K range, comparable to lead-containing materials. It demonstrates significant potential for lead-free, high-sensitivity force sensors in future MEMS applications.
[1] W. P. Mason, "Piezoelectricity, its history and applications," The Journal of the Acoustical Society of America, vol. 70, no. 6, pp. 1561-1566, 1981.
[2] J. Rödel and J.-F. Li, "Lead-free piezoceramics: Status and perspectives," MRS Bulletin, vol. 43, no. 8, pp. 576-580, 2018.
[3] S. Priya et al., "A review on piezoelectric energy harvesting: materials, methods, and circuits," Energy Harvesting and Systems, vol. 4, no. 1, pp. 3-39, 2017.
[4] V. T. Rathod, "A review of acoustic impedance matching techniques for piezoelectric sensors and transducers," Sensors, vol. 20, no. 14, p. 4051, 2020.
[5] 邱碧秀, 電子陶瓷材料. 全欣科技圖書, 1997.
[6] L. Jin, F. Li, S. Zhang, and D. J. Green, "Decoding the Fingerprint of Ferroelectric Loops: Comprehension of the Material Properties and Structures," Journal of the American Ceramic Society, vol. 97, no. 1, pp. 1-27, 2013.
[7] C. Warden, "A Brief Overview of Present and Future Random Access Memories," IPI Letters, vol. 1, pp. 56-62, 2023.
[8] A. M. Badr, H. A. Elshaikh, and I. M. Ashraf, "Impacts of temperature and frequency on the dielectric properties for insight into the nature of the charge transports in the Tl2S layered single crystals," Journal of Modern Physics, vol. 2011, 2011.
[9] M. H. Park et al., "Giant Negative Electrocaloric Effects of Hf(0.5) Zr(0.5) O(2) Thin Films," Adv Mater, vol. 28, no. 36, pp. 7956-7961, 2016.
[10] Q. Z. A. S. Mischenko, J. F. Scott, R. W. Whatmore and N. D. Mathur, "Giant Electrocaloric Effect inThin-Film PbZr 0.95Ti0.05 O," American Association for the Advancement of Science, 2006.
[11] Y. Meng, J. Pu, and Q. Pei, "Electrocaloric cooling over high device temperature span," Joule, vol. 5, no. 4, pp. 780-793, 2021.
[12] Q. Z. T. Correia, "Electrocaloric Materials- New Generation of Coolers," Electrocaloric materials, 2014.
[13] K. Shibata, K. Suenaga, A. Nomoto, and T. Mishima, "Curie Temperature, Biaxial Elastic Modulus, and Thermal Expansion Coefficient of (K,Na)NbO3Piezoelectric Thin Films," Japanese Journal of Applied Physics, vol. 48, no. 12, 2009.
[14] S. R. J. Saunders, "Hardness measurement," in Metrology and Properties of Engineering Surfaces, E. Mainsah, J. A. Greenwood, and D. G. Chetwynd Eds. Boston, MA: Springer US, pp. 305-322, 2001.
[15] F. Seitz, D. Turnbull, and H. Ehrenreich, Solid state physics. Academic Press, 1968.
[16] W. Zhang and R. G. Xiong, "Ferroelectric metal-organic frameworks," Chem Rev, vol. 112, no. 2, pp. 1163-95, Feb 8 2012.
[17] J. Wu, D. Xiao, and J. Zhu, "Potassium-sodium niobate lead-free piezoelectric materials: past, present, and future of phase boundaries," Chem Rev, vol. 115, no. 7, pp. 2559-95, Apr 8 2015.
[18] C. Kang, J.-H. Park, D. Shen, H. Ahn, M. Park, and D.-J. Kim, "Growth and characterization of (K0.5 Na0.5)NbO3 thin films by a sol–gel method," Journal of Sol-Gel Science and Technology, vol. 58, no. 1, pp. 85-90, 2010.
[19] G. Yu, H. Zhang, B.-P. Zhang, and J. Zhang, "Cu-particle-dispersed (K0.5Na0.5)NbO3 composite thin films derived from sol–gel processing," Journal of Sol-Gel Science and Technology, vol. 61, no. 2, pp. 403-410, 2011.
[20] K. L. A. H. D. M. A. C. SAKOWSKI-COWLEY, "The Structure of Sodium Niobate at Room Temperature, and the Problem of Reliability in Pseudosymmetrie Structures," Structural Science, Crystal Engineering and Materials, 1968.
[21] H. Jaffe, "Piezoelectric Ceramics," Journal of the American Ceramic Society, vol. 41, no. 11, pp. 494-498, 2006.
[22] R. Cui, K. Tang, D. Zhu, C. Yue, and L. Yang, "Sm3+-doped KNNS ferroelectric ceramics with enhanced photoluminescence by polarization-field-modulation," Journal of Materials Science: Materials in Electronics, vol. 31, no. 1, pp. 480-487, 2019.
[23] J. Wu, "Advances in Lead-Free Piezoelectric Materials, " Materials Chemistry and Physics, 2018.
[24] K. Tanaka, H. Hayashi, K.-i. Kakimoto, H. Ohsato, and T. Iijima, "Effect of (Na,K)-Excess Precursor Solutions on Alkoxy-Derived (Na,K)NbO3 Powders and Thin Films," Japanese Journal of Applied Physics, vol. 46, no. 10S, 2007.
[25] L. Wang et al., "Preparation and characterization of sol–gel derived (Li,Ta,Sb) modified (K,Na)NbO3 lead-free ferroelectric thin films," Materials Chemistry and Physics, vol. 130, no. 1-2, pp. 165-169, 2011.
[26] C.-R. Cho and A. Grishin, "Background oxygen effects on pulsed laser deposited Na0.5K0.5NbO3 films: From superparaelectric state to ferroelectricity," Journal of Applied Physics, vol. 87, no. 9, pp. 4439-4448, 2000.
[27] L. Wang, W. Ren, K. Yao, P. Shi, X. Wu, and X. Yao, "Effects of thickness on structures and electrical properties of K0.5Na0.5NbO3 thick films derived from polyvinylpyrrolidone-modified chemical solution," Ceramics International, vol. 38, pp. S291-S294, 2012.
[28] C. W. Ahn et al., "The effect of K and Na excess on the ferroelectric and piezoelectric properties of K0.5Na0.5NbO3thin films," Journal of Physics D: Applied Physics, vol. 42, no. 21, 2009.
[29] X. Yang et al., "Structural and ferroelectric properties of textured KNN thick films prepared by sol-gel methods," Integrated Ferroelectrics, vol. 176, no. 1, pp. 171-178, 2016.
[30] H. Bruncková, Ľ. Medvecký, P. Hvizdoš, and J. Ďurišin, "Structural and nanomechanical properties of sol–gel prepared (K, Na)NbO3 thin films," Surface and Interface Analysis, vol. 47, no. 11, pp. 1063-1071, 2015.
[31] Y. Nakashima, W. Sakamoto, H. Maiwa, T. Shimura, and T. Yogo, "Lead-Free Piezoelectric (K,Na)NbO3 Thin Films Derived from Metal Alkoxide Precursors," Japanese Journal of Applied Physics, vol. 46, no. 4L, 2007.
[32] D. Bokov et al., "Nanomaterial by Sol-Gel Method: Synthesis and Application," Advances in Materials Science and Engineering, vol. 2021, pp. 1-21, 2021.
[33] W. Zhang, H. Zhu, X. Zhang, H. Wu, J. Bao, and F. Hu, "Structural and electrical study of highly (100)-oriented KNN films fabricated by a sol-gel non-alkoxide process," Ceramics International, vol. 45, no. 17, pp. 22156-22162, 2019.
[34] D. Frederichi, M. Scaliante, and R. Bergamasco, "Low temperature growth and characterization of (Na,K)NbOx thin films," Journal of Crystal Growth, vol. 28, no. 19, pp. 23610-23633, May 2003.
[35] R. Kumar, S. Rab, B. D. Pant, and S. Maji, "Design, development and characterization of MEMS silicon diaphragm force sensor," Vacuum, vol. 153, pp. 211-216, 2018.
[36] A. S. Fiorillo, C. D. Critello, and S. A. Pullano, "Theory, technology and applications of piezoresistive sensors: A review," Sensors and Actuators A: Physical, vol. 281, pp. 156-175, 2018.
[37] K. Kim, J. Kim, X. Jiang, T. Kim, and M. Gasulla, "Static Force Measurement Using Piezoelectric Sensors," Journal of Sensors, vol. 2021, pp. 1-8, 2021.
[38] C.-H. Lin and B.-Y. Guo, "Investigating capacitive force sensors with 3D printed flexible structures as dielectric layers," Materials Research Express, vol. 10, no. 8, 2023.
[39] C. Groppi, L. Mondonico, F. Maspero, C. Rinaldi, M. Asa, and R. Bertacco, "Effect of substrate preparation on the growth of lead-free piezoelectric (K0.5Na0.5)NbO3 on Pt(111)," Journal of Applied Physics, vol. 129, no. 19, 2021.
[40] W. C. Oliver and G. M. Pharr, "An improved technique for determining hardness and elastic modulus using load and displacement sensing indentation experiments," Journal of Materials Research, vol. 7, no. 6, pp. 1564-1583, 2011.
[41] L. Jin, F. Li, and S. Zhang, "Decoding the Fingerprint of Ferroelectric Loops: Comprehension of the Material Properties and Structures," Journal of the American Ceramic Society, vol. 97, no. 1, pp. 1-27, 2014.
[42] X. Yan, W. Ren, X. Wu, P. Shi, and X. Yao, "Lead-free (K, Na)NbO3 ferroelectric thin films: Preparation, structure and electrical properties," Journal of Alloys and Compounds, vol. 508, no. 1, pp. 129-132, 2010.
[43] K.-S. Hwang, "Preparation of Epitaxial Pb(Zr, Ti)O3 Thin Films on Nb-Doped SrTiO3 (100) Substrates by DippingPyrolysis Process," Japanese Journal of Applied Physics, 1997.
[44] W. Zhang, J. Bao, H. Zhu, X. Zhang, Z. Jiang, and F. Hu, "Highly (h00)-oriented KNN homo-multilayer films grown on Si by sol-gel process via an alternating non-alkoxide and alkoxide route," Ceramics International, vol. 47, no. 1, pp. 87-93, 2021.
[45] C. K. Jeong et al., "Flexible highly-effective energy harvester via crystallographic and computational control of nanointerfacial morphotropic piezoelectric thin film," Nano Research, vol. 10, no. 2, pp. 437-455, 2016.
[46] F. Lai and J.-F. Li, "Sol-gel processing of lead-free (Na,K)NbO3 ferroelectric films," Journal of Sol-Gel Science and Technology, vol. 42, no. 3, pp. 287-292, 2007/06/01 2007.
[47] R. Pinho et al., "Low-temperature solution processing route for potassium sodium niobate (KNN) thin films," Journal of the European Ceramic Society, vol. 43, no. 11, pp. 4740-4747, 2023.
[48] W. Xu, Q. Li, Z. Yin, W. Wang, S. Chu, and H. Zou, "Effect of Gd doping on crystalline orientation, structural and electric properties of PZT thin films prepared by Sol-Gel methods," Integrated Ferroelectrics, vol. 183, no. 1, pp. 100-109, 2017.
[49] Y. Kizaki, Y. Noguchi, and M. Miyayama, "Defect control for low leakage current in K0.5Na0.5NbO3 single crystals," Applied Physics Letters, vol. 89, no. 14, 2006.
[50] F. Söderlind, P.-O. Käll, and U. Helmersson, "Sol–gel synthesis and characterization of Na0.5K0.5NbO3 thin films," Journal of Crystal Growth, vol. 281, no. 2-4, pp. 468-474, 2005.
[51] S. W. Zhang, J. Luo, Z. Zhou, and J. F. Li, "Sol‐gel processed highly (100)‐textured (K, Na) NbO3‐based lead‐free thin films: Effect of pyrolysis temperature," Journal of the American Ceramic Society, vol. 102, no. 5, pp. 2696-2705, 2019.
[52] L. Guo et al., "Orientation dependence of dielectric and piezoelectric properties of tetragonal relaxor ferroelectric single crystals by alternate current poling," Journal of Applied Physics, vol. 127, no. 18, 2020.
[53] W. Chen et al., "Crystalline phase and electrical properties of lead‐free piezoelectric KNN‐based films with different orientations," Journal of the American Ceramic Society, vol. 100, no. 7, pp. 2965-2971, 2017.
[54] H. Li et al., "Improved ferroelectric properties of (100)-oriented PZT thin films deposited on stainless steel substrates with La 0.5 Sr 0.5 CoO 3 buffer layers," Journal of Materials Science: Materials in Electronics, vol. 29, pp. 14651-14656, 2018.
[55] J. J. Choi, G. T. Park, S. M. Lee, and H. E. Kim, "Sol–Gel Preparation of Thick PZN–PZT Film Using a Diol‐Based Solution Containing Polyvinylpyrrolidone for Piezoelectric Applications," Journal of the American Ceramic Society, vol. 88, no. 11, pp. 3049-3054, 2005.
[56] F. Lai and J.-F. Li, "Sol-Gel Processing and Characterization of (Na,K)NbO3Lead-Free Ferroelectric Films," Ferroelectrics, vol. 358, no. 1, pp. 181-187, 2007.
[57] L. Wang et al., "Effect of Pyrolysis Temperature on K0.5Na0.5NbO3 Thick Films Derived from Polyvinylpyrrolidone‐Modified Chemical Solution," Journal of the American Ceramic Society, vol. 93, no. 11, pp. 3686-3690, 2010.
[58] X. Bu, C. Yang, M. Fan, W. Wang, X. Lin, and S. Huang, "Ferroelectric and piezoelectric properties of lead-free Li0.06(K0.5Na0.5)0.94NbO3 thin films," Journal of Advanced Dielectrics, vol. 13, no. 03, 2023.
[59] O. Tokay and M. Yazıcı, "A review of potassium sodium niobate and bismuth sodium titanate based lead free piezoceramics," Materials Today Communications, vol. 31, 2022.
[60] W. Chen et al., "Effect of BaZrO3 amounts on the domain structure and electrical properties of lead-free piezoelectric KNN-based films," Materials Science and Engineering: B, vol. 276, 2022.
[61] M. H. M. Akmal and A. R. M. Warikh, "Electrical behaviour of yttrium-doped potassium sodium niobate thin film for piezoelectric energy harvester applications," Journal of the Australian Ceramic Society, vol. 57, no. 2, pp. 589-596, 2021.
[62] P. Chin Goh, K. Yao, and Z. Chen, "Lithium diffusion in (Li, K, Na)NbO3 piezoeletric thin films and the resulting approach for enhanced performance properties," Applied Physics Letters, vol. 99, no. 9, 2011.
[63] F. Lai, J.-F. Li, Z.-X. Zhu, and Y. Xu, "Influence of Li content on electrical properties of highly piezoelectric (Li,K,Na)NbO3 thin films prepared by sol-gel processing," Journal of Applied Physics, vol. 106, no. 6, 2009.
[64] K. Tanaka, K.-I. Kakimoto, H. Ohsato, and T. Iijima, "Composition Dependence of Crystallinity for Lead-Free (Li, Na, K)NbO3Powder and Thin Films Fabricated by Sol-Gel Process," Ferroelectrics, vol. 358, no. 1, pp. 175-180, 2007.
[65] H. Du, F. Tang, D. Liu, D. Zhu, W. Zhou, and S. Qu, "The microstructure and ferroelectric properties of (K0.5Na0.5)NbO3–LiNbO3 lead-free piezoelectric ceramics," Materials Science and Engineering: B, vol. 136, no. 2-3, pp. 165-169, 2007.
[66] J. Pérez de la Cruz, E. Joanni, P. M. Vilarinho, and A. L. Kholkin, "Thickness effect on the dielectric, ferroelectric, and piezoelectric properties of ferroelectric lead zirconate titanate thin films," Journal of Applied Physics, vol. 108, no. 11, 2010.
[67] Y. Ren, X. Zhu, C. Zhang, J. Zhu, J. Zhu, and D. Xiao, "High stable dielectric permittivity and low dielectric loss in sol–gel derived BiFeO3 thin films," Ceramics International, vol. 40, no. 1, pp. 2489-2493, 2014.
[68] F. Ni et al., "Piezoelectric enhancement and vacancy defect reduction of lead-free Bi0.5Na0.5TiO3-based thin films," Ceramics International, vol. 48, no. 9, pp. 12601-12607, 2022.
[69] S. Y. Lee et al., "Effect of Mn substitution on ferroelectric and leakage current characteristics of lead-free (K0.5Na0.5)(Mn Nb1−)O3 thin films," Current Applied Physics, vol. 11, no. 3, pp. S266-S269, 2011.
[70] K. Vojisavljevic, T. Vrabelj, H. Ursic, and B. Malic, "Effects of strontium doping on microstructure and functional properties of solution-derived potassium sodium niobate thin films," Processing and Application of Ceramics, vol. 14, no. 3, pp. 231-241, 2020.
[71] S. Y. Lee et al., "Enhanced piezoelectric properties of Ta substituted-(K0.5Na0.5)NbO3 films: A candidate for lead-free piezoelectric thin films," Journal of Alloys and Compounds, vol. 509, no. 20, pp. L194-L198, 2011.
[72] C.-C. Lin, C.-C. Chen, C.-M. Weng, S.-Y. Chu, C.-S. Hong, and C.-C. Tsai, "Effects of lithium doping on microstructure, electrical properties, and chemical bonds of sol-gel derived NKN thin films," Journal of Applied Physics, vol. 117, no. 8, 2015.
[73] L. Xu et al., "Buffer electrode layers tuned electrical properties, fatigue behavior and phase transition of KNN-based lead-free ferroelectric films," Journal of Materials Chemistry C, vol. 11, no. 40, pp. 13794-13802, 2023.
[74] M. H. Park et al., "Ferroelectricity and antiferroelectricity of doped thin HfO2-based films," Adv Mater, vol. 27, no. 11, pp. 1811-31, Mar 18 2015.
[75] L. Wang, W. Ren, P. Shi, X. Wu, and X. Yao, "Effects of thickness on structures and electrical properties of Mn-doped K0.5Na0.5NbO3 films," Journal of Alloys and Compounds, vol. 582, pp. 759-763, 2014.
[76] W. Luo, C. Kirchlechner, J. Li, G. Dehm, and F. Stein, "Composition dependence of hardness and elastic modulus of the cubic and hexagonal NbCo2Laves phase polytypes studied by nanoindentation," Journal of Materials Research, vol. 35, no. 2, pp. 185-195, 2020.
[77] H. G. Xiaodong Li, "Nanoindentation of Cu2O Nanocubes," NANO LETTERS, 2004.
[78] W. Tang, L. Shen, and K. Xu, "Hardness and elastic modulus of Au/NiCr/Ta multilayers on Al2O3 substrate by nanoindentation continuous stiffness measurement technique," Thin Solid Films, vol. 485, no. 1-2, pp. 72-76, 2005.
[79] R. B. King, "Elastic analysis of some punch problems for a layered medium," International Journal of Solids and Structures, vol. 23, no. 12, pp. 1657-1664, 1987.
[80] B. Zhou and B. C. Prorok, "A Discontinuous Elastic Interface Transfer Model of Thin Film Nanoindentation," Experimental Mechanics, vol. 50, no. 6, pp. 793-801, 2009.
[81] G. Huajian, C. Cheng-Hsin, and L. Jin, "Elastic contact versus indentation modeling of multi-layered materials," International Journal of Solids and Structures, vol. 29, no. 20, pp. 2471-2492, 1992.
[82] H. Bruncková, Ľ. Medvecký, and P. Hvizdoš, "Effect of substrate on microstructure and mechanical properties of sol–gel prepared (K, Na)NbO3 thin films," Materials Science and Engineering: B, vol. 178, no. 4, pp. 254-262, 2013.
[83] A. Barman, S. Kar‐Narayan, and D. Mukherjee, "Caloric Effects in Perovskite Oxides," Advanced Materials Interfaces, vol. 6, no. 15, 2019.
[84] D. Shan, K. Pan, Y. Liu, and J. Li, "High fidelity direct measurement of local electrocaloric effect by scanning thermal microscopy," Nano Energy, vol. 67, 2020.
[85] M. H. Park, H. J. Kim, Y. J. Kim, T. Moon, K. D. Kim, and C. S. Hwang, "Toward a multifunctional monolithic device based on pyroelectricity and the electrocaloric effect of thin antiferroelectric Hf x Zr 1−x O 2 films," Nano Energy, vol. 12, pp. 131-140, 2015.
[86] K. Wang, B. Malič, and J. Wu, "Shifting the phase boundary: Potassium sodium niobate derivates," MRS Bulletin, vol. 43, no. 8, pp. 607-611, 2018.
[87] D. Liu, G. Bai, and C. Gao, "Phase diagrams classification based on machine learning and phenomenological investigation of physical properties in K1 − xNaxNbO3 thin films," Journal of Applied Physics, vol. 127, no. 15, 2020.
[88] X. Feng et al., "Enhanced electrocaloric effect in KNN-based ceramic via polymorphic phase transition," Ceramics International, vol. 50, no. 1, pp. 1788-1794, 2024.
[89] G. Bai, Y.-H. Han, and C.-F. Gao, "Phase transitions and electrocaloric effects of (111)-oriented K0.5Na0.5NbO3 epitaxial films: effect of external stress and misfit strains," Acta Physica Sinica, vol. 71, no. 9, 2022.
[90] J. Yang and X. Hao, "Electrocaloric effect and pyroelectric performance in (K,Na)NbO3‐based lead‐free ceramics," Journal of the American Ceramic Society, vol. 102, no. 11, pp. 6817-6826, 2019.
[91] S. G. Lu et al., "Organic and inorganic relaxor ferroelectrics with giant electrocaloric effect," Applied Physics Letters, vol. 97, no. 16, 2010.
[92] Y. Wu, Y. Ou, J. Peng, and C. Lei, "Phase Structures, Electromechanical Responses, and Electrocaloric Effects in K0.5Na0.5NbO3 Epitaxial Film Controlled by Non-Isometric Misfit Strain," Crystals, vol. 13, no. 9, 2023.
[93] J. H. Qiu, J. N. Ding, N. Y. Yuan, X. Q. Wang, and J. Yang, "Effect of misfit strain on the electrocaloric effect of P(VDF-TrFE) copolymer thin films," The European Physical Journal B, vol. 84, no. 1, pp. 25-28, 2011.
[94] G. Akcay, S. P. Alpay, G. A. Rossetti, and J. F. Scott, "Influence of mechanical boundary conditions on the electrocaloric properties of ferroelectric thin films," Journal of Applied Physics, vol. 103, no. 2, 2008.
[95] B. Peng, H. Fan, and Q. Zhang, "A Giant Electrocaloric Effect in Nanoscale Antiferroelectric and Ferroelectric Phases Coexisting in a Relaxor Pb0.8Ba0.2ZrO3 Thin Film at Room Temperature," Advanced Functional Materials, vol. 23, no. 23, pp. 2987-2992, 2013.
[96] T. M. Correia et al., "PST thin films for electrocaloric coolers," Journal of Physics D: Applied Physics, vol. 44, no. 16, 2011.
[97] M. Ye et al., "A giant negative electrocaloric effect in Eu-doped PbZrO3 thin films," Journal of Materials Chemistry C, vol. 4, no. 16, pp. 3375-3378, 2016.
[98] J. Chen, Z. Tang, Q. Lu, and S. Zhao, "Giant negative electrocaloric effect over a broad temperature range in lead-free based Bi0.5(K0.15Na0.85)0.05TiO3 relaxor ferroelectric films," Journal of Alloys and Compounds, vol. 756, pp. 62-67, 2018.
[99] S. E. Shirsath et al., "Interface-Charge Induced Giant Electrocaloric Effect in Lead Free Ferroelectric Thin-Film Bilayers," Nano Lett, vol. 20, no. 2, pp. 1262-1271, Feb 12 2020.
[100] X. Liu, Y. Dai, X. Pei, and W. Chen, "Giant room-temperature electrocaloric effect within wide temperature span in Sn-doped Ba0.85Ca0.15Zr0.1Ti0.9O3 lead-free thin films," Ceramics International, vol. 49, no. 2, pp. 1846-1854, 2023.
[101] A. Barman et al., "Large electrocaloric effect in lead-free ferroelectric Ba0.85Ca0.15Ti0.9Zr0.1O3 thin film heterostructure," APL Materials, vol. 9, no. 2, 2021.
校內:2029-07-31公開