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研究生: 錢彥興
Yen-Hsing Chien
論文名稱: 鋁掺入極薄氧化鉿高介電係數閘極介電層之效應
The Effect of Aluminum (Al) Incorporation in Ultra-Thin HfO2 High-k Gate Dielectrics
指導教授: 劉傳璽
Liu, Chuan-Hsi
阮弼群
Juan, Pi-Chun
學位類別: 碩士
Master
系所名稱: 機電工程學系
Department of Mechatronic Engineering
論文出版年: 2011
畢業學年度: 99
語文別: 中文
論文頁數: 95
中文關鍵詞: 高介電係數氧化鋁鉿共濺鍍技術
英文關鍵詞: High-k, HfAlO, co-sputtering technique
論文種類: 學術論文
相關次數: 點閱:321下載:39
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  • 氧化鉿薄膜為一良好的高介電係數材料,適合使用在MOS元件,但相較於其他介電材料,結晶溫度過低為其一大缺點,本論文主要將氧化鋁鉿材料取代傳統MOS元件上之閘極氧化層,利用摻雜鋁元素,製備氧化鋁鉿薄膜,以提高氧化鉿薄膜的結晶溫度,並針對其電性、物性做分析與探討。
    本研究使用射頻共濺鍍技術,在常溫、充滿氬氣的真空腔體,將高純度的氧化鉿及鋁之靶材,濺射沉積在矽基板上,形成一層厚度7 奈米的氧化鋁鉿薄膜,之後在充滿氮氣的真空腔體中,分別執行650℃、750℃、850℃的快速熱退火,然後鍍上鋁製成閘極電極;最後再利用電流-電壓、電壓-電壓量測儀、穿透式電子顯微鏡、能量散佈分析儀、原子力顯微鏡、X光繞射儀、橢圓測厚儀、X光反射儀等,分析探討氧化鋁鉿薄膜的電性及物性。
    實驗結果顯示,氧化鋁鉿薄膜擁有良好的結晶溫度、介電係數、及閘極漏電流,在750℃的快速熱退火後,得到的相對介電係數為14.6,閘極漏電流方面,閘極注入電壓為-1 V時,漏電流大小約為10-6 ~ 10-7 A/cm2,基板注入電壓為1 V時,漏電流大小約在10-5 ~ 10-6 A/cm2,漏電流機制符合蕭基發射,其鋁與介電層間、介電層與矽基板間之蕭基能障分別為0.48 eV及0.72 eV。

    HfO2 thin film is a good high-k gate dielectric material for MOS devices, but one main drawback is its relatively low crystallization temperature. In this thesis, the gate dielectric of MOS devices is replaced by HfAlO. Aluminum (Al) has been introduced into HfO2 thin films to form HfAlO films in order to raise the crystallization temperature of HfO2. The electrical and physical characteristics of the MOS devices with HfAlO gate dielectrics were analyzed and discussed in this study.
    The high-k HfAlO thin films (7 nm) were deposited by RF co-sputtering technique using highly pure HfO2 and Al as the sputtering targets in Ar ambient at room temperature, followed by RTA at 650, 750 or 850 ℃ in N2 ambient. Al was then formed as the gate electrode. The electrical and physical properties of the capacitors were evaluated through I-V (current-voltage), C-V (capacitance-voltage), TEM, EDS, AFM, XRD, ellipsometer, and XRR.
    The results revealed that the HfAlO thin films have satisfactory crystallization temperature, dielectric constant, and gate leakage current. The relative dielectric constant of the HfAlO film is 14.6 after 750℃ rapid thermal annealing. The gate leakage current is 10-6-10-7 or 10-5-10-6 A/cm2 at a gate bias of 1 or -1 V, respectively. Moreover, the Schottky barrier height at the Al/HfAlO interface or HfAlO/p-Si interface is about 0.48 or 0.72 eV, respectively.

    第一章 緒論 1 1-1 金氧半場效電晶體 1 1-2 金氧半電容器 1 1-3 高介電係數材料之閘極介電層 1 1-4 高介電係數介電層電容器製備 2 1-5 本論文研究方向 2 第二章 文獻探討 3 2-1 金氧半場效電晶體 3 2-1-1電晶體的結構 4 2-1-2 電晶體的運作 5 2-1-3 電晶體的性能 6 2-2 金氧半電容器 8 2-2-1 金氧半電容器的結構 8 2-2-2金氧半電容器的運作 9 2-2-3 MOS電容器的介面電荷陷阱 10 2-3 MOS電容器之漏電流機制 13 2-3-1直接穿隧 14 2-3-2 傅勒-諾德翰穿隧 15 2-3-3 蕭基發射 16 2-3-4 普爾-夫倫克爾發射 17 2-4 高介電係數閘極氧化層之電容器 (一) 20 2-4-1 介電係數 20 2-4-2 高介電係數 22 2-5 高介電係數閘極氧化層 (二) 23 2-5-1 高介電係數材料 23 2-5-2 高介電係數材料Al2O3 25 2-5-3 高介電係數材料La2O3 27 2-5-4 高介電係數材料Y2O3 27 2-5-5 高介電係數材料CeO2 30 2-5-6 高介電係數材料ZrO2 31 2-5-7 高介電係數材料HfO2 31 第三章 實驗設計 36 3-1 研究動機 36 3-2 氧化鋁鉿薄膜電容器實驗流程 36 3-3 高介電電容器之製備與機台介紹 40 3-3-1 基板準備 40 3-3-2 薄膜濺鍍沉積 40 3-3-3 熱退火處理 45 3-3-4 鋁電極製作 47 3-4 實驗量測儀器原理 47 3-4-1 X光繞射儀 47 3-4-2 X光反射率 49 3-4-3 橢圓偏光儀 50 3-4-4 原子力顯微鏡 51 3-4-5 穿透式電子顯微鏡 52 3-4-6 電容器的電性量測 52 第四章 結果與討論 53 4-1 HfAlO薄膜基本性質量測分析 53 4-1-1 X光繞射量測分析 53 4-1-2 X光反射率量測分析 60 4-1-3 橢圓偏光儀量測分析 64 4-1-4 原子力顯微鏡量測分析 65 4-1-5 穿透式電子顯微鏡及能量散佈分析儀分析 69 4-1-6 HfAlO電性量測:電容-電壓 71 4-1-7 HfAlO電性量測:電流-電壓 75 4-1-8 HfAlO電性量測:漏電流傳導機制--蕭基發射 78 第五章 結論與未來展望 86 5-1 Al/HfAlO/Si電容器的物性與電性 86 5-1-1 Al/HfAlO/Si電容器的物性 86 5-1-2 Al/HfAlO/Si電容器的電性 87 5-1-3 Al/HfAlO/Si電容器實驗總結 88 5-2 未來展望 88 參考文獻 90

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