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研究生: 蔡政宏
Tsai, Jeng-hung
論文名稱: 磊晶氧化鋅共摻雜鈷、鋁之稀磁性半導體磁性來源的研究
The study of magnetic origin from epitaxy of Co & Al codoped ZnO DMS
指導教授: 黃榮俊
Huang, Jung-Chun
學位類別: 碩士
Master
系所名稱: 理學院 - 物理學系
Department of Physics
論文出版年: 2008
畢業學年度: 96
語文別: 中文
論文頁數: 104
中文關鍵詞: 氧化鋅稀磁性半導體
外文關鍵詞: Al, ZnO, DMS, Co
相關次數: 點閱:55下載:2
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  • 本論文利用分子束磊晶系統成長ZnO薄膜,藉由摻雜Co、Al來形成具有良好電性及室溫鐵磁性的樣品,進一步的深入了解磁性的來源。我們設計兩組實驗來對照,實驗(一)調變(Co,ZnO)中Al摻雜的濃度探討傳遞載子對ZnO稀磁性半導體之磁性變化,實驗(二)成長不同結構,將相同濃度的(Co、Al)摻雜入ZnO造成不同結構的(Co、Al)ZnO,研究除了傳遞載子之外,磁性的影響。
    實驗(一),有雜Al的樣品其磁化量較未參雜Al的樣品來的大,而實驗(二)中卻是結構缺陷多的磁化量較結構缺陷少的樣品來的大;由實驗(二)來看磁性似乎還是由結構缺陷所支配,而雜Al的樣品其電性與磁性上沒有明顯的相依性,所以猜測實驗(一)中雜Al的樣品磁性大於未摻雜Al的樣品,可能是因為Al3+(0.39Ǻ)的離子半徑較Zn2+(0.6Ǻ)來的小,當Al3+取代Zn2+時有可能造成微結構的缺陷,而這個微結構的缺陷有可能形成束縛極化子來增加貢獻磁性。
    因此不論在高或低載子濃度區之ZnO稀磁性半導體,磁性來源還是由束縛磁極化子(BMP)所支配。

    We use Molecular Beam Epitaxy (MBE) to deposit ZnO thin films and form fine electrical property and room temperature ferromagnetism (RTFM) by Co、Al codoped,We try to understand the origin of ferromagnetism 。We design two experiments,In group(一) we modify Al quantity in Co/ZnO thin films to discuss that the effect of carrier ,In group(二) we deposit different structure of ZnO that codoped similar quantity of (Co、Al)。
    In group(一) that ferromagnetism of Co/Al/ZnO thin film is
    Greater than Co/ZnO thin film,In group(二) that Co/Al/ZnO thin film which sample have more structural defect that own larger ferromagnetism。
    Regardless of Diluted Magnetic Semiconductor(DMS) of ZnO is in high carrier or low carrier region that the origin of ferromagnetism domainate by Bound Magnetic Polaron Model(BMP)。

    第一章 緒論..................................1 1-1 前言.......................................1 1-2 氧化鋅薄膜特性簡介.........................3 1-3 文獻回顧........................................5 第二章 基本理論介紹.........................19 2-1 薄膜成長理論..............................19 2-1-1 成長模式..............................19 2-2 磁學理論..................................22 2-2-1磁性物質的種類.........................24 2-3磁性來源機制...............................26 2-3-1 超交換偶合機制(superexchange interaction)..26 2-3-2 雙交換耦合機制(Double exchange)..........27 2-2-3 交互巡迴式鐵磁性(Itinerant Ferromagnetism)........28 2-2-4 侷限載子式鐵磁性(Localized Carrier).....................30 2-3-5束縛磁極化子模型(Bound Magnetic Polaron Model) ............................................31 第三章 實驗儀器介紹與實驗步驟...............36 3-1 實驗製程儀器-分子束磊晶系統(Molecular Beam Epitaxy,MBE)..................................36 3-2 實驗量測儀器..................................42 3-2-1 X 光繞射儀(X-ray diffraction)...........42 3-2-2 吸收光譜.................................44 3-2-3 超導量子干涉儀 (簡稱SQUID)..............54 3-2-4 霍爾效應.................................57 3-2-5 直流電阻實驗裝置.........................59 3-2-6 穿透率量測...............................61 3-3 實驗步驟.......................................62 3-3-1 系統真空環境之準備......................62 3-3-2 基板的準備...............................62 3-3-3 樣品成長.................................63 3-3-3 樣品量測.................................65 第四章 結果與討論 4-1 Zn0.95Co0.05O與Zn0.95Co0.05Al0.02O薄膜的結構分析....70 4-1-1 Zn0.95Co0.05O與Zn0.95Co0.05Al0.02O薄膜膜成長在Al2O3(11-20)基板上之XRD結果與討論...........70 4-1-2 Zn0.95Co0.05Al0.02O薄膜成長在Al2O3(11-20)及(0001)基板上XRD的結果與討論........................72 4-2 Zn0.95Co0.05O與Zn0.95Co0.05Al0.02O薄膜的電性分析...77 4-2-1 Zn0.95Co0.05O與Zn0.95Co0.05Al0.02O薄膜成長在Al2O3(11-20)基板上之電性的結果與討論......77 4-2-2 Zn0.95Co0.05Al0.02O薄膜分別成長在Al2O3(11-20)及(0001)基板上電性的結果與討論..............79 4-3 Zn0.95Co0.05O與Zn0.95Co0.05Al0.02O薄膜的磁性分析....81 4-3-1 Zn0.95Co0.05O與Zn0.95Co0.05Al0.02O薄膜成長在Al2O3(11-20)基板上之磁性上結果與討論......81 4-3-2 Zn0.95Co0.05Al0.02O薄膜分別成長在Al2O3(11-20)及(0001)基板上磁性的結果與討論............84 4-3-3 Zn0.95Co0.05Al0.02O與Zn0.95Co0.05O薄膜溫度對磁化量的關係.....................................85 4-3-4 磁性與電性的相依性.......................86 4-4 Zn0.95Co0.05Al0.02O薄膜分別成長在Al2O3(11-20)及(0001)基板上的X光吸收光譜分析..................94 4-4-1前緣吸收光譜(XANES)........................94 4-4-2延伸吸收光譜(EXAFS)........................96 4-5 Zn0.95Co0.05Al0.02O薄膜與Zn0.95Co0.05O薄膜的透光率分析.......................................99 第五章 結論....................................103

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