研究生: |
李威德 Wei-te Li |
---|---|
論文名稱: |
以反應性濺鍍選擇性成長氧化釕奈米桿 Selective Growth of RuO2 Nanorods Using Reactive Sputtering |
指導教授: |
蔡大翔
Dah-Shyang Tsai |
口試委員: |
黃鶯聲
Ying-Sheng Huang 洪儒生 Lu-Sheng Hong 呂宗昕 Chuan-Hsin Lu |
學位類別: |
碩士 Master |
系所名稱: |
工程學院 - 化學工程系 Department of Chemical Engineering |
論文出版年: | 2007 |
畢業學年度: | 95 |
語文別: | 中文 |
論文頁數: | 100 |
中文關鍵詞: | 二氧化釕 、奈米桿 、選擇性成長 |
外文關鍵詞: | RuO2, nanorod, selective growth |
相關次數: | 點閱:255 下載:3 |
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本論文藉由反應性濺鍍的方法,研究在濺鍍矽網印於SA(100)及SA(012)基板上,選擇性區域成長二氧化釕奈米桿。二氧化釕奈米桿垂直成長於SA(100)基板上,傾斜35o成長於SA(012)基板,利用SEM與XRD觀察其形貌及結晶性。XPS分析結果顯示氧化釕奈米桿表面具有高於計量比的釕,可能是沉積時以富釕的沉積物種進行沉積。選區成長的原理可追溯至其初期成長時在不同表面上的成核情形,二氧化釕在SA(100)及SA(012)表面上成核相當迅速,而在氧化矽表面上則不易成核,藉由二氧化釕於不同表面上成核能障的差異,以實現選區成長。實驗顯示當濺鍍瓦數為50W,基板溫度控制在200oC時,可得到最佳二氧化釕奈米桿的選擇性成長結果;若當基板溫度低於180oC時,於成長區內只能形成二氧化釕的薄膜,且因沉積物種在基板上的移動能力較差,易於停留在非成長區內沉積,造成選區成長失敗。而當基板溫度高於230oC時,由於物種脫附效應逐漸主導了整個成長過程,故可以相當清楚的定義出成長區與非成長區,但是亦失去了一維奈米結構的特徵,轉變為一顆顆的氧化釕晶柱。接著再改變沉積時的濺鍍功率,匹配不同的基板溫度,整理出不同濺鍍功率和基板溫度彼此之間對選擇性成長的關係,試圖發展出可兼顧二氧化釕一維奈米結構及優良之選擇性成長的最適成長範圍。
The technique of area-selective growth of RuO2 nanorods via reactive sputtering is explored in this master thesis. The substrates are sapphire (100) and (012), denoted as SA(100) and SA(012), patterned with SiO2 using a copper grid mask. The RuO2 nanorods are vertically aligned on SA(100), tilted 35 with respect to the substrate normal on SA(012). Each nanorod is a RuO2 single crystal, confirmed by scanning electron microscopy (SEM) and X-ray diffraction analysis (XRD). The Ru:O ratio on the surface of sputtered RuO2 nanorods is higher than the stoichiometric 1:2 ratio, measured by X-ray photoelectron spectroscopy.
The success of area-selective growth relies on the difference between nucleation barriers on the noncrystalline SiO2 and the sapphire surfaces. RuO2 nucleates with ease on SA(100) and SA(012) surface, but slowly on the noncrystalline SiO2 surface. When the RuO2 clusters constantly diffuse away from the nongrowth area of SiO2 surface, meanwhile nucleate and grow in the growth area of SA(100) or SA(012), a pattern of RuO2 nanorods can be achieved. Our experimentation shows that the optimum conditions for selective growth of RuO2 nanorods were sputtering power at 50 W and substrate temperature at 200C. If the substrate temperature was less than 180C, the less mobile growth species tend to deposit in the nongrowth region, and the RuO2 film (not rods) grow in the growth region. If the substrate temperature is higher than 230C, a clearly defined pattern can be achieved, but the nanorods lose their one-dimensional feature and become stout rods. When the sputtering power is raised to 60 W, the selective growth temperature region for nanorods decreases. In this work we have outlined the growth domain for area-selective growth of RuO2 nanorods and discuss the morphological variation of RuO2 crystals.
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