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研究生: 張馨露
Chang, Shin-Lu
論文名稱: 離子佈植於濺鍍β-Ga₂O₃薄膜之受體活化機制與電性轉變研究
Acceptor Activation Mechanisms and Electrical Transitions in Ion-Implanted Sputtered β-Ga₂O₃ Thin Films
指導教授: 李文熙
Lee , Wen-Shi
學位類別: 碩士
Master
系所名稱: 智慧半導體及永續製造學院 - 半導體封測學位學程
Program on Semiconductor Packaging and Testing
論文出版年: 2026
畢業學年度: 114
語文別: 中文
論文頁數: 87
中文關鍵詞: β-Ga₂O₃薄膜離子佈植濺鍍受體活化電性轉變p 型摻雜
外文關鍵詞: β-Ga₂O₃ thin film, ion implantation, magnetron sputtering, acceptor activation, electrical-type conversion, p-type doping
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  • β-Ga₂O₃ 作為第四代超寬能隙半導體的核心材料,憑藉 4.9 eV 的超寬能隙、約 8 MV/cm 的理論崩潰電場與本質日盲紫外響應特性,在高壓功率元件與深紫外光電感測等領域具有不可取代的應用價值。然而,β-Ga₂O₃ 的 p 型摻雜長期面臨三大瓶頸:受體摻雜的施體補償效應顯著、受體能階偏深導致室溫游離困難、佈植晶格損傷的可控性不足,致使活化效率低落,成為限制其 pn 接面元件研發與產業化的核心障礙。離子佈植具備摻雜劑量、深度與區域精準可控的優勢,磁控濺鍍則可實現大面積、高均勻性薄膜的規模化製備;惟過往受體佈植研究幾乎集中於單晶基板,針對濺鍍多晶薄膜的系統性研究仍屬空白。本文結合二者,為濺鍍 β-Ga₂O₃ 薄膜的 p 型化建立完整的製程與機制基礎。

    本文以 350 nm 濺鍍純 β 相薄膜為研究基底,選取 Mg²⁺ 與 Cu²⁺ 兩種代表性受體離子,採單一變數法系統調控佈植劑量、佈植能量、退火溫度與退火時間四大核心製程參數,結合 XRD、SEM、XPS 與霍爾效應量測,量化分析製程參數對晶體結構、晶格缺陷、表面形貌、受體晶格佔位與電學特性的影響規律,揭示受體活化的微觀機制,並釐清薄膜由 n 型轉變為 p 型的臨界條件與核心調控因素。

    研究結果表明:離子佈植存在明確的損傷閾值,劑量 1×10¹⁴ cm⁻² 與能量 100 keV 構成低損傷摻雜製程視窗,於此視窗內晶格損傷可逆、離子峰值深度(180 nm)落於薄膜中央;退火是實現受體活化與電性轉變的必要步驟,氮氣氣氛 900 ℃ 持溫 60 min 為最佳退火組合,可使晶格完全回復至空白薄膜水準,Cu²⁺ 晶格佔位率達 95.7%、受體活化效率達 32%,並實現穩定不回退的 p 型導電(電洞濃度 4.8×10¹⁵ cm⁻³、遷移率 7.4 cm²/(V·s));Mg²⁺ 之佔位率與活化效率分別為 91.2% 與 28%。比較研究證實,Cu²⁺ 憑藉相對較淺的受體能階與較佳的化學鍵結相容性,綜合摻雜性能優於 Mg²⁺,為濺鍍薄膜 p 型摻雜的較佳受體離子;由兩種離子的實測值並可歸納出受體能階深度每降低 0.01 eV、活化效率約提升 0.57% 的經驗規律。本文進一步量化了缺陷對活化的調控作用,界定穩定 p 型導電的缺陷容忍邊界介於差排面密度 0.9 至 1.5×10¹² cm⁻² 之間,並建構「晶格佔位-缺陷修復-載子傳輸」耦合的三階段活化機制模型,闡明受體離子替位至 Ga 晶格位形成電學有效受體、經退火活化後釋放電洞,是電性轉變的核心;而高濃度晶格缺陷引發的載子補償效應,則是抑制活化效率的關鍵誘因。

    本研究確立了濺鍍 β-Ga₂O₃ 薄膜 p 型摻雜的完整製程體系,量化了製程參數與材料性能的關聯規律,並將摻雜活化理論延伸至濺鍍多晶體系,為 β-Ga₂O₃ p 型製程的工業化最佳化與高性能光電、功率元件的研發提供了實驗依據與技術支持,對推動超寬能隙半導體的發展具有理論價值與工程意義。

    β-Ga₂O₃ is a fourth-generation ultra-wide-bandgap semiconductor, yet the absence of reliable p-type conductivity remains the decisive obstacle to its bipolar devices. This thesis establishes a complete p-type doping process for sputtered polycrystalline β-Ga₂O₃ thin films, a technologically scalable platform that previous implantation studies, which focused on single crystals, have left unexplored. Mg²⁺ and Cu²⁺ acceptors were implanted into 350-nm pure-β-phase films and activated by nitrogen annealing, with dose, energy, temperature, and time varied one at a time and characterized by XRD, SEM, XPS, and Hall measurements. A low-damage process window of 1×10¹⁴ cm⁻² and 100 keV was identified, within which implantation damage is fully recoverable. Annealing at 900 °C for 60 minutes restores the lattice to the pristine level and drives acceptors onto gallium sites, achieving a stable n-to-p conversion with a Cu²⁺ site-occupancy ratio of 95.7%, an activation efficiency of 32%, a hole concentration of 4.8×10¹⁵ cm⁻³, and a mobility of 7.4 cm²/(V·s). Copper outperforms magnesium owing to its shallower acceptor level and superior bonding compatibility. A three-stage activation model coupling lattice-site occupation, defect recovery, and carrier transport is constructed, and a defect-tolerance boundary for stable p-type conduction is quantified, providing design rules for industrial p-type doping of β-Ga₂O₃.

    摘 要 I Activation Mechanisms and Electrical Transitions in Ion-Implanted Sputtered β-Ga₂O₃ Thin Films III 誌謝 VII 目 錄 X 表目錄 XIII 圖目錄 XIV 符 號 XV 第一章 緒論 1 1.1 研究背景與意義 1 1.1.1超寬能隙半導體材料的發展現狀 1 1.1.2 β-Ga₂O₃的特性與應用前景 1 1.1.3 β-Ga₂O₃ p 型摻雜的技術瓶頸 2 1.2 國內外研究現狀 3 1.2.1 β-Ga₂O₃受體離子篩選研究 3 1.2.2 β-Ga₂O₃摻雜製程的研究進展 5 1.2.3 濺鍍β-Ga₂O₃薄膜的研究現狀 6 1.3 研究內容與目標 8 1.3.1 主要研究內容 8 1.3.2 研究目標與技術指標 8 1.4 論文結構安排 9 第二章 實驗材料、設備與方法 10 2.1 實驗材料 10 2.1.1 基板與靶材選擇 10 2.1.2 實驗氣體與輔助材料 11 2.2 實驗設備 13 2.2.1 薄膜製備設備 13 2.2.2 摻雜與退火設備 13 2.2.3 鑑定與量測設備 14 2.3 實驗方法 14 2.3.1 濺鍍β-Ga₂O₃薄膜的製備流程 14 2.3.2 受體離子佈植的製程設計 16 2.3.3 退火製程的實施方法 18 2.3.4 樣品的鑑定與量測方法 18 第三章 離子佈植對濺鍍β-Ga₂O₃薄膜微觀結構的影響 22 3.1 佈植劑量對薄膜微觀結構的影響 22 3.1.1 不同劑量下薄膜的晶體結構變化 22 3.1.2 不同劑量下薄膜的表面形貌變化 24 3.2 佈植能量對薄膜微觀結構的影響 27 3.2.1 不同能量下薄膜的晶體結構變化 28 3.2.2 不同能量下薄膜的表面形貌變化 31 第四章 退火製程對離子佈植後薄膜的改質作用 35 4.1 退火溫度對薄膜的影響 35 4.1.1 退火溫度對晶格缺陷修復的作用 35 4.1.2 退火溫度對受體離子晶格佔位的影響 38 4.2 退火時間對薄膜的影響 40 4.2.1 退火時間對晶格缺陷演化的規律 40 4.2.2 退火時間對受體離子活化的作用 42 4.2.3退火充分性與擴散風險評估 45 第五章 離子佈植與退火製程對薄膜電性轉變的影響 46 5.1 製程參數對薄膜電性轉變的規律 46 5.1.1 佈植參數對薄膜電性參數的影響 47 5.1.2 退火參數對薄膜電性參數的影響 50 5.2 不同受體離子的電性轉變差異 52 5.2.1 Mg、Cu離子佈植的電性轉變比較 52 5.2.2 受體離子特性對活化效率的影響 54 5.3 離子佈植於濺鍍β-Ga₂O₃薄膜的受體活化機制 56 5.3.1 受體離子的晶格佔位與能階形成機制 56 5.3.2 晶格缺陷對受體活化的調控機制 57 5.3.3 β-Ga₂O₃薄膜電性轉變的內在機制 59 第六章 結論與展望 60 6.1 研究結論 60 6.2 研究展望 61 參考文獻 64 附 錄 68 附錄 A 霍爾電壓原始量測數據 68 附錄 B 載子面濃度換算彙整 69 附錄 C 主要計算式彙整 70

    [1] E. Chikoidze, A. Fellous, A. Perez-Tomas, G. Sauthier, T. Tchelidze, C. Ton-That, T. T. Huynh, M. Phillips, S. Russell, M. Jennings, B. Berini, F. Jomard, and Y. Dumont, "P-type β-gallium oxide: A new perspective for power and optoelectronic devices," Materials Today Physics, Vol. 3, pp. 118–126, 2017.
    [2] N. Das, F. Alema, W. Brand, A. Katta, A. Gilankar, A. Osinsky, et al., "In situ patterned damage-free etching of three-dimensional structures in β-Ga₂O₃ using triethylgallium," Journal of Applied Physics, Vol. 138, No. 6, p. 065703, 2025.
    [3] Z. Feng, A. F. M. A. U. Bhuiyan, Z. Xia, W. Moore, Z. Chen, J. F. McGlone, D. R. Daughton, A. R. Arehart, S. A. Ringel, S. Rajan, and H. Zhao, "Probing charge transport and background doping in metal-organic chemical vapor deposition-grown (010) β-Ga₂O₃," Physica Status Solidi (RRL) – Rapid Research Letters, Vol. 14, No. 8, p. 2000145, 2020.
    [4] S.-J. Fu, Q. Xiang, L. Lai, H.-L. Mo, S.-Q. Fan, and W.-J. Li, "Effect of defects on the structural and optical properties of β-Ga₂O₃ thin films," Journal of Functional Materials, Vol. 52, No. 3, pp. 3081–3085, 2021.
    [5] Y. Han, T. Jiao, H. Yu, Q.-L. Sai, D.-Y. Chen, Z. Li, et al., "Influence of substrate crystal plane on the properties of n-Ga₂O₃ films grown by MOCVD homoepitaxy," Journal of Synthetic Crystals, Vol. 54, No. 3, pp. 438–444, 2025.
    [6] S. Hasan, M. U. Jewel, S. R. Crittenden, D. Lee, V. S. Avrutin, Ü. Özgür, H. Morkoç, and I. Ahmad, "Gate leakage current and threshold voltage characteristics of β-Ga₂O₃ passivated AlGaN/GaN based heterojunction field effect transistor," Proceedings of SPIE, Vol. 12421, p. 124210A, 2023.
    [7] A. Hiraiwa, K. Horikawa, H. Kawarada, M. Kado, and K. Danno, "Influence of Al₂O₃ atomic-layer deposition temperature on positive-bias instability of metal/Al₂O₃/β-Ga₂O₃ capacitors," Journal of Vacuum Science & Technology B, Vol. 42, No. 1, p. 012207, 2024.
    [8] C.-Y. Huang, X.-Y. Tsai, F.-G. Tarntair, A. K. Singh, S.-H. Hsu, D.-S. Wuu, K. Järrendahl, C.-L. Hsiao, and R.-H. Horng, "Fabrication of vertical gallium oxide PN diodes using homoepitaxial growth by MOCVD and ion implantation technology," Materials Today Advances, Vol. 25, p. 100568, 2025.
    [9] A. Katta, F. Alema, W. Brand, A. Gilankar, A. Osinsky, and N. K. Kalarickal, "Demonstration of MOCVD based in situ etching of β-Ga₂O₃ using TEGa," Journal of Applied Physics, Vol. 135, No. 7, p. 075705, 2024.
    [10] Y.-J. Li, Y.-Q. Zhao, and C.-Y. Liang, "Effect of O₂/Ar flow ratio on the properties of amorphous Ga₂O₃ thin films on flexible and rigid substrates," Rare Metal Materials and Engineering, No. 12, pp, 2025.
    [11] Y. M. Liao, H. Z. Song, Z. G. Xie, C. Zhang, and C.-K. Tan, "Exploration of p-type conductivity in β-Ga₂O₃ through Se–Mg hyper co-doped: An ion implantation approach," Materials Today Advances, Vol. 25, p. 100559, 2025.
    [12] T. Luo, K. R. Gann, C. A. Gorsak, H. P. Nair, R. B. van Dover, and M. O. Thompson, "Epitaxial recovery of β-Ga₂O₃ after high dose implantation," arXiv preprint, arXiv:2512.12148, 2025.
    [13] L. A. M. Lyle, S. Okur, V. S. N. Chava, M. L. Kelley, R. F. Davis, G. S. Tompa, M. V. S. Chandrashekhar, A. B. Greytak, and L. M. Porter, "Characterization of epitaxial β-(Al,Ga,In)₂O₃-based films and applications as UV photodetectors," Journal of Electronic Materials, Vol. 49, No. 6, pp. 3490–3498, 2020.
    [14] J. L. Lyons, "A survey of acceptor dopants for β-Ga₂O₃," Semiconductor Science and Technology, Vol. 33, No. 5, p. 05LT02, 2018.
    [15] X.-F. Ma, Y.-Q. Huang, Y.-S. Zhi, X. Wang, P.-G. Li, Z.-P. Wu, and W.-H. Tang, "Rectifying characteristics and solar-blind photoresponse in β-Ga₂O₃/ZnO heterojunctions," Chinese Physics B, Vol. 28, No. 8, p. 088503, 2019.
    [16] Y. Ma, T. Chen, X. Zhang, W. Tang, B. Feng, Y. Hu, L. Zhang, X. Zhou, X. Wei, K. Xu, D. Mudiyanselage, H. Fu, and B. Zhang, "High-photoresponsivity self-powered α-, ε-, and β-Ga₂O₃/p-GaN heterojunction UV photodetectors with an in situ GaON layer by MOCVD," ACS Applied Materials & Interfaces, Vol. 14, No. 30, pp. 35194–35204, 2022.
    [17] S. J. Pearton, J. Yang, P. H. Cary, F. Ren, J. Kim, M. J. Tadjer, and M. A. Mastro, "A review of Ga₂O₃ materials, processing, and devices," Applied Physics Reviews, Vol. 5, No. 1, p. 011301, 2018.
    [18] B. Qiao, Z. Z. Zhang, Y. L. Wang, X. Q. Huang, Z. H. Zhang, Z. Y. Zheng, X. Sun, X. H. Xie, B. H. Li, X. Chen, K. W. Liu, L. Liu, and D. Z. Shen, "Plasmon induced conductivity transition in monoclinic gallium oxide," Surfaces and Interfaces, Vol. 56, p. 105592, 2025.
    [19] K. Sasaki, M. Higashiwaki, A. Kuramata, T. Masui, and S. Yamakoshi, "Si-ion implantation doping in β-Ga₂O₃ and its application to fabrication of low-resistance ohmic contacts," Applied Physics Express, Vol. 6, No. 8, p. 086502, 2013.
    [20] D. Seo, S. Kim, H.-Y. Kim, D.-W. Jeon, J.-H. Park, and W. S. Hwang, "Heteroepitaxial growth of single-crystalline β-Ga₂O₃ on GaN/Al₂O₃ using MOCVD," Crystal Growth & Design, Vol. 23, No. 10, pp. 7090–7094, 2023.
    [21] G. Seryogin, F. Alema, N. Valente, H. Fu, E. Steinbrunner, A. T. Neal, S. Mou, A. Fine, and A. Osinsky, "MOCVD growth of high purity Ga₂O₃ epitaxial films using trimethylgallium precursor," Applied Physics Letters, Vol. 117, No. 26, p. 262101, 2020.
    [22] L.-Y. Shen, Preparation and Properties of β-Ga₂O₃ Epitaxial Thin Films Grown on GaN Substrates, Doctoral Dissertation, Shandong University, Jinan, China,
    [23] X.-L. Shi, H.-Y. Liu, S. Hou, L.-X. Qian, and X.-Z. Liu, "Application of surface plasmons in gallium oxide-based ultraviolet photodetectors," Opto-Electronic Engineering, Vol. 45, No. 2, pp. 80–87, 2018.
    [24] R.-J. Sun, J.-H. Zhang, Y.-F. Li, Y. Hao, and J.-C. Zhang, "Research progress of Mg-doped gallium oxide," Journal of Synthetic Crystals, Vol. 54, No. 3, pp. 361–370, 2025.
    [25] W.-B. Tang, Study on Homoepitaxy of Gallium Oxide and Schottky Barrier Diodes, Doctoral Dissertation, University of Science and Technology of China, Hefei, China, 2023.
    [26] J. Y. Tsao, S. Chowdhury, M. A. Hollis, D. Jena, N. M. Johnson, K. A. Jones, R. J. Kaplar, S. Rajan, C. G. Van de Walle, et al., "Ultrawide-bandgap semiconductors: Research opportunities and challenges," Advanced Electronic Materials, Vol. 4, No. 1, p. 1600501, 2018.
    [27] J. B. Varley, A. Janotti, C. Franchini, and C. G. Van de Walle, "Role of self-trapping in luminescence and p-type conductivity of wide-band-gap oxides," Physical Review B, Vol. 85, No. 8, p. 081109, 2012.
    [28] M. H. Wong, C.-H. Lin, A. Kuramata, S. Yamakoshi, H. Murakami, Y. Kumagai, and M. Higashiwaki, "Acceptor doping of β-Ga₂O₃ by Mg and N ion implantations," Applied Physics Letters, Vol. 113, No. 10, p. 102103, 2018.
    [29] X. Xu, D. Chen, Y. Lu, T. Li, X. Han, D. Chen, H. Qi, D. Yang, M. Zhu, H. Zhang, and X. Lu, "Nitrogen-doped Ga₂O₃ current blocking layer using MOCVD homoepitaxy for high-voltage and low-leakage Ga₂O₃ vertical device fabrication," Applied Physics Letters, Vol. 125, No. 20, p. 202107, 2024.
    [30] Z. Yan, S. Li, J. Yue, X. Ji, Z. Liu, Y. Yang, P. Li, Z. Wu, Y. Guo, and W. Tang, "Reinforcement of double built-in electric fields in spiro-MeOTAD/Ga₂O₃/Si p–i–n structure for a high-sensitivity solar-blind UV photovoltaic detector," Journal of Materials Chemistry C, Vol. 9, No. 41, pp. 14788–14798, 2021.
    [31] C.-C. Zhao, Preparation of Nanoporous GaN-Based Films and Epitaxial Growth of β-Ga₂O₃ Thin Films, Doctoral Dissertation, Shandong University, Jinan, China.

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