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| DC 欄位 | 值 | 語言 |
|---|---|---|
| dc.contributor.advisor | 陳敏璋 | |
| dc.contributor.author | Chung-Yu Yang | en |
| dc.contributor.author | 楊宗諭 | zh_TW |
| dc.date.accessioned | 2021-06-08T06:07:22Z | - |
| dc.date.copyright | 2011-08-10 | |
| dc.date.issued | 2011 | |
| dc.date.submitted | 2011-08-05 | |
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| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/25274 | - |
| dc.description.abstract | 本論文分為兩部分,第一部分為熱門的II-VI 族半導體材料氧化鋅,吾人使用原子層沉積技術(Atomic layer deposition, ALD)成長高品質的氧化鋅做為晶種層,藉此增加基材的導電性,並使得電化學沉積的氧化鋅晶柱有較佳的結晶品質與結晶優選方向。藉由XRD、SEM、PL分析,探討不同電鍍參數,以及熱處理對結晶品質及顯微結構的影響,從而找出結晶品質最佳的電鍍參數。第二部分為透明導電膜二氧化錫之研究,將二氧化錫薄膜上蒸鍍鋁,在不同溫度或時間下進行熱擴散,製備p型導電薄膜。
第一部份為電化學沉積氧化鋅。首先,先藉由循環伏安法,獲得沉積氧化鋅的工作電位,必須要高於-1.2 V(相對於Ag/AgCl參考電極)。接著固定其他參數,分別探討在施加不同過電位、過氧化氫濃度、溫度的影響,XRD分析顯示在-0.95 V、過氧化氫濃度10 mM、80 oC時,具有最大的晶粒尺寸,為50.4 nm。接著探討晶種層的熱處理及電鍍後的熱處理之影響。以ALD成長的氧化鋅晶種層若不退火,由XRD半高寬和PL強度可以得知結晶品質大幅下降,電鍍後退火對晶體品質有改善。XRD及PL兩項分析皆顯示兩段式製程:-1.4 V持續10秒,接著-0.8 V持續5分鐘,可以比一段式製程:-0.8 V持續5分鐘,得到更高結晶品質的氧化鋅。 第二部分為二氧化錫的導電膜的製備,二氧化錫的導電薄膜可以藉由將鋁熱擴散進入二氧化錫薄膜製備而成,在霍爾效應量測中顯示二氧化錫導電薄膜是p型,並且只有在600 oC進行擴散,時間1到2小時,擴散完畢將表層的鋁以稀鹽酸酸蝕後才能得到。比較二氧化錫摻雜鋁在600oC下擴散,以不同轉速塗佈溶膠,以旋轉塗佈轉速4000 rpm均較轉速3000 rpm者具有較佳的電性及穩定性。在旋轉塗佈轉速4000 rpm時,於600 oC擴散兩小時,電洞濃度為3.33x1020 cm-3,載子遷移率為1.24 cm2/V•s,電阻率為0.03 Ω• cm;於600 oC擴散1小時後鹽酸酸蝕者,電洞濃度較高達4.05x1020 cm-3,載子遷移率為0.794 cm2/V•s,電阻率為0.0251 Ω•cm。吾人以此方法製備的二氧化錫之電洞濃度較現今多數文獻高兩個數量級。在製備完成後90天的期間,每30天進行霍爾效應的量測,結果顯示,無論是載子濃度、載子遷移率,電阻率都是穩定的值,顯示此薄膜電性的穩定性相當好。 | zh_TW |
| dc.description.abstract | The contents can be divided into two topics. In the first topic, high quality ZnO films were grown by atomic layer deposition (ALD) as seedlayer on sapphire substrates. Afterwards, the main layer of ZnO was prepared by electrodeposition. The effect of different electrodeposition parameters (applied voltage, precursor concentration, temperature ) and thermal treatment on crystalline quality and microstructures were investigated by XRD, SEM, PL analysis. In the second topic, the p-type conductive oxide, SnO2:Al was investigated. After incorporating Al as dopants into SnO2, the deposited films were annealed at various temperatures for different durations. The p-type conductive films of a high hole concentration and low resistivity were achieved.
In the first topic on electrodeposition of ZnO, the potentials at which ZnO can be plated from a specific electrolyte were determined by using cyclic voltammetry. Experimental results indicate that ZnO films can be plated at potentials higher than -1.2 V(vs. Ag/AgCl) .The largest crystal size was 50.4 nm, obtained at the electrodeposition condition of -0.95 V, 10 mM H2O2 and 80 oC. Rapid thermal annealing (RTA) on seedlayer, and the post-deposition RTA treatment after electrodeposition can enhance the crystal quality. The XRD and PL analysis indicated that better ZnO crystal can be obtained by two-step electrodepostion . In the second topic, the p-type conductive SnO2:Al thin films were prepared by the thermal diffusion of Al on SnO2 thin films on glass substrate. Hall measurements revealed that the SnO2:Al films exhibited long-term stable p-type conductivity at a specific diffusion temperature of 600 oC .The p-type SnO2:Al films with a high hole concentration (4.05x1020 cm-3) and a low resistivity (0.0251 Ω•cm) was obtained. | en |
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| dc.description.tableofcontents | 目錄
口試委員會審定書 # 誌謝 ii 摘要 iv Abstract vi 目錄 viii 圖目錄 xi 表目錄 xiv 第一章 序論 1 1.1 研究動機 1 1.2 原子層沉積法(Atomic Layer Deposition, ALD) 2 1.3 電鍍法 5 1.3.1 電鍍法簡介 5 1.3.2 電鍍系統 6 1.3.3 電鍍法製備氧化鋅 7 1.3.4 電鍍參數對製備氧化鋅之影響 8 1.4 二氧化錫製備方法介紹 13 1.4.1 噴塗熱解法(spray pyrolysis) 13 1.4.2 濺鍍法(sputtering) 14 1.4.3 化學氣相沉積法(CVD) 14 1.4.4 溶膠凝膠法(sol-gel) 14 1.5 溶膠凝膠(sol-gel)介紹 15 1.5.1 Sol-gel名詞的由來 15 1.5.2 高分子與金屬氧化物複合材料(polymer/metal-oxide) 15 1.5.3 溶膠凝膠反應(sol-gel reaction) 15 1.5.4 中性結晶型水溶性奈米溶膠溶液 15 第二章 在ALD晶種層上以電化學沉積法製備氧化鋅及其結構與光學性質之研究 17 2.1簡介 17 2.2實驗 18 2.2.1晶種層的生長與前處理 18 2.2.2溶液配置 19 2.2.3電鍍系統架設 19 2.2.4流程圖及本章大綱 21 2.3 原子層沉積技術生長之氧化鋅晶種層 22 2.4 循環伏安法(Cyclic Voltammetry) 22 2.5 沉積電位之影響 24 2.5.1電化學沉積電位對顯微結構之影響 26 2.5.2 XRD分析 26 2.6 過氧化氫濃度的影響 29 2.6.1過氧化氫濃度對顯微結構之影響 29 2.6.2 XRD分析 31 2.7 電鍍溫度的影響 32 2.8 晶種層退火之影響 36 2.9 電鍍後退火之影響 38 2.10兩階段式製程 40 2.11 結論 43 第三章 P型二氧化錫導電薄膜 45 3.1 簡介 45 3.2 實驗流程 46 3.3 結果與討論 48 3.3.1 二氧化錫溶膠鍍膜的SEM分析 48 3.3.2 XRD分析 49 3.3.3 擴散溫度對形成p型二氧化錫薄膜電性之影響 50 3.3.4 擴散時間對形成p-SnO2:Al電性之影響 52 3.4 穿透率 53 3.5 p型二氧化錫薄膜的穩定性 54 3.6 結論 54 第四章 總結 56 參考文獻 58 圖目錄 圖1. 1 以原子層沉積法(ALD)沉積氧化鋅之示意圖 3 圖1. 2 原子層沉積法(ALD)沉積溫度與生長速率(growth rate)關係示意圖 4 圖1. 3 不同過電位的沉積示意圖(a)低過電位(b)高過電位[30] 8 圖1. 4 不同電壓(vs.saturated calomel electrode)下電鍍的SEM表面形貌以及橫截面圖 (a)- 0.5 V (b) -0.6 V (c) -0.8 V (d) -1.0 V, (e)-1.1 V(f) -1.5 V。電化學沉積條件:溫度70oC, 時間一小時, 鋅離子濃度 0.005 M. [31] 9 圖1. 5 不同溫度下電鍍的SEM表面形貌 (a)34 oC(b) 40 oC (c) 50 oC (d) 80 oC(e) 89 oC。電化學沉積條件:5 mM 氯化鋅,0.1 M 氯化鉀,在-0.75 V(vs. NHE )進行反應。[17] 10 圖1. 6 電鍍ZnO在不同溫度下之反應機構示意圖[17] 11 圖1. 7 不同過氧化氫濃度下SEM表面形貌。(a)5 mM(b)25 mM(c)40 mM(d)橫截面條件同(c)。電化學沉積條件:-0.75 V(vs. NHE ),70oC[32] 12 圖2. 1 電鍍系統示意圖 18 圖2. 2 電化學沉積氧化鋅實驗及分析流程示意圖 20 圖2. 3 氧化鋅晶種層退火後之XRD圖 21 圖2. 4 掃描電壓隨時間變化圖 23 圖2. 5 在0.08 M氯化鉀、5 mM氯化鋅,10 mM過氧化氫,70 oC下循環伏安法,掃描速率20 mV/s 23 圖2. 6 不同沉積電位對應SEM形貌(a)-0.75 V(b)-0.85 V(c)-0.95 V(d)-1.05 V(e)-1.15 V。電化學沉積條件:過氧化氫濃度10 mM,溫度70oC,20分鐘。 25 圖2. 7 氧化鋅在電化學沉積電位-0.95 V,過氧化氫濃度10 mM,溫度70 oC之XRD圖 26 圖2. 8 氧化鋅在不同的電化學沉積電位下,對基板訊號做正規化的XRD圖 27 圖2. 9 用Scherrer formula計算出的晶粒大小和過電位關係圖 28 圖2. 10 不同過氧化氫濃度對應之SEM形貌(a)5 mM(b)10 mM(c)15 mM(d)20 mM 30 圖2. 11 氧化鋅在不同的過氧化氫濃度下電鍍,對基板訊號做正規化的XRD圖 30 圖2. 12 Scherrer formula計算出的晶粒大小和過氧化氫濃度關係圖 31 圖2. 13 不同溫度對應之SEM形貌(a)60 oC(b)70 oC(c)80 oC。電化學沉積條件:沉積電位:-0.95 V,過氧化氫濃度:10 mM,沉積時間:20分 33 圖2. 14 氧化鋅在不同的電解液溫度下電鍍,對基板訊號做正規化的XRD圖 34 圖2. 15 用Scherrer formula計算出的晶粒大小和溫度關係圖 35 圖2. 16 晶種層退火對應顯微結構(a)晶種層有退火(b)晶種層沒退火 36 圖2. 17 晶種層是否有退火與PL關係圖 37 圖2. 18 電鍍後退火對顯微結構(a)電鍍後無退火(b)電鍍後退火 38 圖2. 19 電鍍後是否有退火與PL關係圖 39 圖2. 20 兩段式製程,-1.4 V持續10秒後-0.8 V持續電鍍,電流密度與時間關係圖 41 圖2. 21 兩階段式製程對顯微結構之影響(a) -1.4 V持續10秒後-0.8 V持續300秒(b) -0.8 V持續300秒 42 圖2. 22 一段式製程與兩段式製程PL發光頻譜 43 圖3. 1 p型二氧化錫製備實驗流程圖 46 圖3. 2 二氧化錫溶膠以3000 rpm旋轉塗佈10秒的表面形貌 47 圖3. 3 二氧化錫溶膠以3000 rpm旋轉塗佈10秒,燒結後之表面形貌 47 圖3. 4 二氧化錫3000 rpm旋轉塗佈後,蒸鍍鋁後600oC擴散1小時之XRD圖 49 圖3. 5 文獻中以溶膠凝膠法製備的二氧化錫600oC之XRD圖 49 圖3. 6 二氧化錫以3000 rpm旋轉塗佈,蒸鍍鋁後600oC下擴散2小時alpha-stepper表面起伏 50 圖3. 7 康寧玻璃、二氧化錫薄膜、二氧化錫摻雜鋁的薄膜穿透率隨波長的變化 53 表目錄 表 1.1 不同過氧化氫濃度及沉積時間下,理論厚度與量測厚度,滴定厚度之比較[32] 12 表2. 1 氧化鋅晶種層退火後電性 22 表2. 2 氧化鋅(0 0 0 2)在XRD圖下的峰值位置,半高寬(FWHM),Scherrer formula計算出來的晶粒大小隨電化學沉積電位的變化 27 表2. 3 氧化鋅(0 0 0 2)在XRD圖下的峰值位置,半高寬(FWHM),Scherrer formula計算出來的晶粒大小隨過氧化氫濃度的變化 31 表2. 4 氧化鋅(0 0 0 2)在XRD圖下的峰值位置,半高寬(FWHM),Scherrer formula計算出來的晶粒大小隨電解液溫度的變化 34 表2. 5 氧化鋅(0 0 0 2)在XRD圖下的峰值位置,半高寬(FWHM),Scherrer formula計算出來的晶粒大小對於是否有做晶種層退火之比較 37 表2. 6 氧化鋅(0 0 0 2)在XRD圖下的峰值位置,半高寬(FWHM),Scherrer formula計算出來的晶粒大小對於是否有做電鍍後退火之比較 39 表2. 7 氧化鋅(0 0 0 2)在XRD圖下的峰值位置,半高寬(FWHM),Scherrer formula計算出來的晶粒大小對於是否有做電鍍後退火之比較 41 表3. 1 二氧化錫溶膠以3000 rpm旋轉塗佈10秒的EDAX成分分析 48 表3. 2 不同旋轉塗佈速率,在不同溫度下熱擴散2小時,霍爾效應量測的電性。x:無法量測到有意義的數據。o:可量測到有意義的數據 51 表3. 3 不同旋轉塗佈速率,在600oC下熱擴散2小時的二氧化錫薄膜電性 51 表3. 4 600oC擴散1小時後鹽酸酸蝕後,霍爾效應量出的電性 52 表3. 5 二氧化錫以4000 rpm旋轉塗佈,蒸鍍鋁後600oC下擴散2小時,霍爾效應量測的電性隨時間的變化 54 | |
| dc.language.iso | zh-TW | |
| dc.subject | 二氧化錫 | zh_TW |
| dc.subject | 電化學沉積 | zh_TW |
| dc.subject | 氧化鋅原子層沉積技術 | zh_TW |
| dc.subject | 奈米溶膠 | zh_TW |
| dc.subject | p型導電膜 | zh_TW |
| dc.subject | p-type conductive oxide | en |
| dc.subject | SnO2 | en |
| dc.subject | electrodeposition | en |
| dc.subject | sol-gel | en |
| dc.subject | nanoparticles | en |
| dc.subject | Atomic Layer Deposition(ALD | en |
| dc.subject | ZnO | en |
| dc.title | 氧化鋅及二氧化錫光電性質之研究 | zh_TW |
| dc.title | Study of Optical and Electrical Properties of ZnO and SnO2 | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 99-2 | |
| dc.description.degree | 碩士 | |
| dc.contributor.oralexamcommittee | 林招松,謝宗霖,陳忠詰 | |
| dc.subject.keyword | 氧化鋅原子層沉積技術,電化學沉積,二氧化錫,奈米溶膠,p型導電膜, | zh_TW |
| dc.subject.keyword | ZnO,Atomic Layer Deposition(ALD,electrodeposition,SnO2,nanoparticles,sol-gel,p-type conductive oxide, | en |
| dc.relation.page | 62 | |
| dc.rights.note | 未授權 | |
| dc.date.accepted | 2011-08-05 | |
| dc.contributor.author-college | 工學院 | zh_TW |
| dc.contributor.author-dept | 材料科學與工程學研究所 | zh_TW |
| 顯示於系所單位: | 材料科學與工程學系 | |
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