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研究生: 蘇宏迪
Su, Hung-Ti
論文名稱: 濺鍍電漿製程反應器內中性氣體動力行為之DSMC模擬
DSMC Simulation of Neutral Gas Dynamics within a Plasma Sputtering Chamber
指導教授: 邱政勳
Chiou, Jeng-Shing
學位類別: 碩士
Master
系所名稱: 工學院 - 機械工程學系
Department of Mechanical Engineering
論文出版年: 2005
畢業學年度: 93
語文別: 中文
論文頁數: 98
中文關鍵詞: 蒙地卡羅法電漿濺鍍腔體
外文關鍵詞: DSMC, Plasma, Sputtering Chamber
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  •   由於半導體工業的迅速發展,電漿製程也愈受關切,故本文中針對一濺鍍電漿製成反應器內分析注入之中性氣體的分佈狀況,以期能對電漿製程有所改進;因為電漿濺鍍腔體之腔內壓力甚低,約在3mtorr左右,流體過渡稀薄而無法以一般連續流的Navier-Stokes方程式來分析;故本文採用直接蒙地卡羅法來求解腔內之密度與溫度之分佈。

      文中所模擬之反應腔體腔壓為0.4Pa,直徑為600mm高為480mm,注入之氣體為氬氣注入率分別為5、10、15sccm,而托盤溫度則分別為300K、500K、700K的情況下,去探討反應器內密度與溫度分佈的狀況。

      模擬結果顯示,在固定入口流率下,當托盤溫度上升時,將導致腔內核心關鍵區域中的標準差密度不變與標準差溫度上升;而在固定托盤溫度下,當流率上升時,則核心區中的標準差密度上升與標準差溫度不變;因此欲得到更均勻流場,就必須將托盤溫度下降到邊界溫度附近以及限制入口流率使其不致過大。托盤溫度與入口流率雖對流場之均勻度都有影響,但是由模擬結果比較下來,下降入口流率之影響要比下降托盤溫度來得更明顯,所以入口流率實是影響著腔體內區域中均勻度的一個關鍵性變數。

     The plasma fabrication process is attracting more attentions as the semiconductor industry is still growing up. In this study , the dynamic behavior of neutral gases within a plasma sputtering chamber (under 3 mtorr pressure) is simulated by the direct simulation Monte Carlo (DSMC) method.

     From the simulated results such as the density and temperature distributions within the chamber can hopefully provide the useful information to improve the chamber design.

     Argon was considered as the neutral gas to injected into the sputtering chamber under 0.4Pa pressure with the diameter of 600mm and the height of 480mm. Different injection rates varied as 5,10 and 15 sccm under different temperature of the target holder (which are 300K,500Kand 700K) are all simulated and analyzed.

     Results indicate that the stardand deviation density (STD_D) inside the block 1 zone (key space inside the chamber) is invariable and the stardand deviation temperature is increasing when the holder temperature is decreasing while the injection is fixed.
    And STD_D is increasing and STD_T is invariable when the injection is increasing while the holder temperature is fixed.
     
     In order to get more uniform flux , we compare the influence of the holder temperature and the injection rate. Finally we get the conclusion which is the injection rate have more powerful influence, so it is a key parmameter.

    目 錄 中文摘要 Ⅰ 英文摘要 Ⅱ 誌謝 Ⅳ 目錄 Ⅵ 圖目錄 Ⅸ 表目錄 ⅩⅢ 符號說明 ⅩⅣ 第一章 緒論 1 1-1 研究背景與目的 1 1-2 濺鍍(Sputtering) 3 1-3 稀薄氣體與納森數(Kn) 6 1-4 直接蒙地卡羅法(DSMC) 9 1-5 文獻回顧 11 1-6 本文架構 15 第二章 分子氣體動力學之相關理論 16 2-1 簡單氣體 16 2-2 速度分佈函數 21 2-3 三種具代表性的分子熱速率 26 2-4 單位面積的數通量 28 2-5 二體彈性碰撞 30 2-5-1 動量與能量守恆 30 2-5-2 碰撞動力學 32 2-6 VHS分子模型 36 第三章 直接模擬蒙地卡羅法(DSMC) 38 3-1 直接模擬蒙地卡羅法(DSMC) 之假設及流程 38 3-1-1 DSMC的基本假設 39 3-1-2 DSMC的基本流程 40 3-1-3 平行化DSMC的流程 41 3-2 程式核心 45 3-2-1 粒子的移動 45 3-2-2 排序與粒子的碰撞 48 3-2-3 抽樣 50 3-2-4 巨觀量的表示 51 3-3 DSMC模擬之問題及調適 53 3-3-1 變數時間間格法 53 3-3-2 中斷續跑法 56 第四章 電漿反應器中性氣體的模擬 57 4-1 腔體的物理模型尺寸與網格 57 4-2 模擬的簡化、假設與設定 63 4-3 腔內擋版有無對其內流場之影響 66 4-4 腔壓對其內流場分佈均勻度之影響 68 4-5 修正當腔壓為0.4Pa時,出口端之溫度疊代 70 4-6 模擬的案例 74 4-6-1 案例之介紹 74 4-6-2 案例之討論 83 第五章 結論與建議 92 5-1 結論 92 5-2 建議 93 參考文獻 94 自述 98

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