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  1. NTU Theses and Dissertations Repository
  2. 電機資訊學院
  3. 電子工程學研究所
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/77689
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor管傑雄(Chieh-Hsiung Kuan)
dc.contributor.authorHong-Ru Panen
dc.contributor.author潘鴻儒zh_TW
dc.date.accessioned2021-07-10T22:16:04Z-
dc.date.available2021-07-10T22:16:04Z-
dc.date.copyright2017-08-31
dc.date.issued2017
dc.date.submitted2017-08-16
dc.identifier.citation[1] Gordon E. Moore, “Cramming More Components onto Integrate Circuits,” Electronics, pp. 114–117, April 19, 1965.
[2] Lester F. Eastman and U.K. Mishra, “The toughest transistor yet GaN transistors,” IEEE SPECTRUM, vol. 39, pp. 28-33, May 2002.
[3] T. Palacios, 'Beyond the AlGaN/GaN HEMT: new concepts for high-speed transistors,' physica status solidi (a), vol. 206, pp. 1145-1148,2009.
[4] M. A. Khan, J. N. Kuznia, A. Bhattarai and D. T. Olson, “Metal Semiconductor FieldEffect Transistor on single crystal GaN,” Appl. Phys. Lett, vol. 62, pp. 1786-1787, 1986.
[5] U.K. Mishra , P. Parikh, Y.F. Wu,” AlGaN/GaN HEMTs: An overview of device
operation and applications,” Proceedings of the IEEE, vol. 90, pp. 1-16, 2002.
[6] Chung JW, Hoke WE, Chumbes EM, Palacios T. AlGaN/GaN HEMT With 300-
GHz. IEEE Electron Dev Lett 2010;31:195–7.
[7] Selvanathan D, Mohammed FM, Bae JO, Adesida I, Bogart KH. Investigation of
surface treatment schemes on n-type GaN and Al0.20Ga0.80N. J Vac Sci Technol,
B 2005;23:2538–44.
[8] Jia Guo, Guowang Li, Faiza Faria, Yu Cao, Ronghua Wang, Jai Verma, Xiang Gao, Shiping Guo, Edward Beam, Andrew Ketterson, Michael Schuette, Paul Saunier, Mark Wistey, Debdeep Jena, Huili Xing, 'MBE-Regrown Ohmics in InAlN HEMTs With a Regrowth Interface Resistance of 0.05 Ω · mm,' IEEE ELECTRON DEVICE LETTERS, VOL. 33, NO. 4, APRIL 2012
[9] I. P. Smorchkova, C. R. Elsass, J. P. Ibbetson, R. Vetury, B. Heying, P.Fini, et al., 'Polarization-induced charge and electron mobility in AlGaN/GaN heterostructures grown by plasma-assisted molecular-beam epitaxy,' Journal of Applied Physics, vol. 86, p. 4520, 1999.
[10] Wang Chong , Zhao Meng-Di, He Yun-Long, Zheng Xue-Feng, Wei Xiao-Xiao, Mao Wei, Ma Xiao-Hua,Zhang Jin-Cheng, Hao Yue, 'Optimization of ohmic contact for AlGaNGaN HEMT by introducing patterned etching in ohmic area,' Solid-State Electronics 129 (2017) 114–119
[11] Yusuke Takei, Masayuki Kamiya, Kazuo Tsutsui, Wataru Saito, Kuniyuki Kakushima, Hitoshi Wakabayashi, Yoshinori Kataoka, and Hiroshi Iwai, 'Reduction of contact resistance on AlGaN/GaN HEMT structures introducing uneven AlGaN layers,' Phys. Status Solidi A 212, No. 5, 1104–1109 (2015)
[12] S. R. Lee, D. D. Koleske, K. C. Cross, J. A. Floro, and K. E. Waldrip Sandia, “In situmeasurements of the critical thickness for strain relaxation in AlGaN/GaN
heterostructures,” Appl. Phys. Lett, vol. 85, pp. 6164-6166, 2004.
[13] Fabio Sacconi, Aldo Di Carlo, P. Lugli, and Hadis Morkoç, “Spontaneous and
Piezoelectric Polarization Effects on the Output Characteristics of AlGaN/GaN
Heterojunction Modulation Doped FETs,” IEEE Transactions on electron devices, vol. 48,pp. 450-457, 2001.
[14] Abhishek Motayed, Ravi Bathe, Mark C. Wood, Ousmane S. Diouf, R. D. Vispute, S. Noor Mohammad, 'Electrical, thermal, and microstructural characteristics of Ti/Al/Ti/Au multilayer Ohmic contacts to n-type GaN,' JOURNAL OF APPLIED PHYSICS, VOLUME 93, NUMBER 2, 15 JANUARY 2003
[15] Chen-hui Yu, Qing-zhou Luo, Xiang-dong Luo, Pei-sheng Liu, 'Donor-Like Surface Traps on Two-Dimensional Electron Gas and Current Collapse of AlGaN/GaN HEMTs,' The ScientificWorld Journal, Volume 2013, Article ID 931980, 6 pages
[16] T. V. Blank, and Yu. A. Gol’dberg, Semiconductors, vol. 41, no.11, pp. 1263-1292, 2007.
[17] Pallab Bhattacharya, Roberto Fornari, Hiroshi Kamimura, ‘’Comprehensive Semiconductor Science and Technology,’’ 6-Volume Set p.108, 2011.
[18] Ting-Wei Liao, Chien-Wei Chiu, Chieh-Hsiung Kuan, Tsung-Yi Huang, Tsung-Yu Yang, 'Utilizing Ge interlayer and patterned substrate to improve the contact resistance of n-GaN,' 10.1109/INEC.2014.7460449.
[19] Donghyun Jin, Jesús A. del Alamo, 'Methodology for the Study of Dynamic
ON-Resistance in High-Voltage GaN Field-Effect Transistors,' IEEE TRANSACTIONS ON ELECTRON DEVICES, VOL. 60, NO. 10, OCTOBER 2013
[20] 鍾政桓,'電子束微影之低溫短顯影研究,'國立臺灣大學電機資訊學院電子工程學研究所碩士論文, July 2016
[21] 葉伯淳,' 增強型鰭狀氮化鋁鎵/氮化鎵金氧半高電子遷移率電晶體之研製,'國立臺灣大學電機資訊學院光電工程學研究所博士論文, July 2015
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/77689-
dc.description.abstract氮化鎵(GaN)所擁有的寬能隙、高飽和速度、高崩潰電場…等特性皆使其成為在製作高功率及高頻元件元件的材料選擇上為一時之選,而氮化鋁鎵/氮化鎵異質結構所擁有的高濃度的二維電子氣(2DEG),使其能有較高的電子遷移率及優異的載子傳輸特性,以此結構所製作出的氮化鋁鎵/氮化鎵高電子遷移率電晶體為現今實現高頻及高功率元件的熱門選擇之一。
從許多研究中皆能了解到接觸電阻值深深影響著元件特性的表現,因此為了有效降低接觸電阻值,本論文研究嘗試在原有之氮化鋁鎵/氮化鎵基板上,於蒸鍍歐姆接觸金屬前在金屬/半導體接面之半導體表面事先以特殊圖案設計之奈米孔洞進行特定深度蝕刻,基於其邊緣效應的影響及側壁面積增加,並由實驗結果皆證實了如此設計的有效性。
首先在不同幾何圖案設計的實驗中,由TLM量測結果得到經過奈米孔洞蝕刻後皆能使接觸電阻值降低,且由對稱排列的圓形孔洞之幾何圖形設計之接觸電阻從1.345(Ω.mm)降至0.994(Ω.mm),而特徵接觸電阻值則由1.63×10-4(Ω.cm2)降低至5.30×10-5(Ω.cm2);根據前項實驗結果,並且考量在基板上成長氮化鎵層的過程中所產生的錯位差排一路竄升上去而形成的介面缺陷密度後,經數學計算出所設計的奈米孔洞應小於20奈米才能形成奈米接觸,再由TLM量測結果可得特徵接觸電阻值由5.862×10-4(Ω.cm2)下降至1.345×10-5(Ω.cm2)較先前大尺寸孔洞擁有更高程度的改善;最後將此設計應用於元件上,經直流量測可得到最大飽和汲極電流從319.486(mA/mm)上升至498.785(mA/mm),轉導特性則由80(mS/mm)上升至137.875(mA/mm),導通電阻(On-resistance)則由1.03(Ω‧mm)減少至 0.89(Ω‧mm),由此結果可知元件特性皆有顯著提升,並由兩項實驗皆能歸納出接觸電阻將隨著奈米孔洞尺寸變小而降低的趨勢。
zh_TW
dc.description.abstractProperties Gallium nitride (GaN) have including large bandgap, high saturation velocity, high breakdown field… making it become a good material of manufacturing high power and high frequency devices. High concentration of two dimensional electron gas resulting from heterogeneous structure AlGaN/GaN makes it have much higher electron mobility and nice carrier transport property. Based on this structure, AlGaN/GaN HEMT becomes a popular device realizing these requirements.
Alot of evidences figure out the contact resistance is the key point affecting the performance of devices. In order to reduce the contact resistance, this thesis introduce a new method which is using special geometrical pattern etching with particular etching depth on the original substrate surface between metal and semiconductor before deposing ohmic contact metal. Since the fringing effect and increasing surface of sidewall, the result of experiment is again proving the validity of this design.
First in the experiment of different geometric pattern design, considering the result of transmission line measurement, all of the pattern with geometric pattern etching have lower contact resistance, especially the pattern in hole square design has the best performance which reducing contact resistance from 1.345(Ω.mm) to 0.994(Ω.mm) and specific contact resistance from 1.63×10-4(Ω.cm2) to 5.30×10-5(Ω.cm2). Based on this result, further considering the interface-trap density resulting from the threading dislocation of GaN layer which come from epitaxy on the substrate, it can be calculated out the size of Nano-hole should be smaller than 20nm, which make it become Nano-Contact. We found it have a much higher improving comparing with previous bigger size of Nano-hole on contact resistance which decreasing from 5.862×10-4(Ω.cm2) to 1.345×10-5(Ω.cm2). Finally, with this design on our former devices, the performance of devices can get a huge improving such as maximum saturation drain current from 319.486(mA/mm)to 498.785(mA/mm), transconductance (Gm) from 80(mS/mm)to 137.875(mA/mm), and On-resistance from 1.03(Ω‧mm)to 0.89(Ω‧mm). Also, we can conclude a trend that the contact resistance will decrease following the decreasing of Nano-hole size.
en
dc.description.provenanceMade available in DSpace on 2021-07-10T22:16:04Z (GMT). No. of bitstreams: 1
ntu-106-R04943107-1.pdf: 3666898 bytes, checksum: 87990a6f8ebf1d943833a83155801e87 (MD5)
Previous issue date: 2017
en
dc.description.tableofcontents口試委員會審訂書 I
誌謝 II
中文摘要 V
Abstract VI
目錄 VII
圖目錄 X
表目錄 XII
第一章 緒論 1
1.1 前言 1
1.2 研究動機 5
1.3 論文架構 7
第二章 AlGaN/GaN HEMTs元件介紹及原理基礎 9
2.1 氮化鎵(Gallium-Nitride,GaN)晶格結構 9
2.2 氮化鋁鎵/氮化鎵異質接面 10
2.2.1 極化效應 10
2.2.2 二維電子氣(2DEG)形成機制 13
2.2.3 氮化鋁鎵(AlGaN)臨界厚度 14
2.3 氮化鋁鎵/氮化鎵高電子遷移率電晶體結構介紹 17
2.4 奈米接觸(Nano-Contact)原理 19
2.5 金屬/半導體接觸原理 21
2.5.1 蕭特基接觸(Schottky contact)原理 21
2.5.2 歐姆接觸(Schottky contact)原理 22
第三章 實驗儀器與元件製備 24
3.1 實驗儀器簡介 24
3.1.1 金屬有機化學氣相沉積(MOCVD) 24
3.1.2 電子束微影系統(Electron Beam Lithography System) 25
3.1.3 電子束蒸鍍系統(Electron Beam Evaporator) 27
3.1.4 感應式耦合電漿反應離子蝕刻(ICP-RIE) 29
3.1.5 快速熱退火處理系統(RTA) 30
3.1.6 掃描式電子顯微鏡(SEM) 31
3.2 元件製程介紹 32
3.2.1 Nano-Contact製程設計 32
3.2.2 元件結構設計 34
3.2.3 元件製作流程 36
第四章 實驗設計及量測結果與分析 45
4.1 奈米洞幾何圖案比較實驗 45
4.1.1 實驗設計 45
4.1.2 TLM量測結果及分析 46
4.2 奈米洞尺寸差異比較實驗 48
4.2.1 實驗設計 48
4.2.2  TLM量測結果及分析 49
4.2.3 元件直流I-V量測結果及分析 50
第五章 結論與未來展望 54
5.1 結論 54
5.2 未來展望 55
參考文獻 56
dc.language.isozh-TW
dc.subject接觸電阻zh_TW
dc.subject氮化鋁鎵/氮化鎵高電子遷移率電晶體zh_TW
dc.subject錯位差排zh_TW
dc.subject介面缺陷密度zh_TW
dc.subject奈米洞蝕刻zh_TW
dc.subject奈米接觸zh_TW
dc.subjectAlGaN/GaN HEMTen
dc.subjectcontact resistanceen
dc.subjectNano-Contacten
dc.subjectNano-hole etchingen
dc.subjectinterface-trap densityen
dc.subjectthreading dislocationen
dc.title利用奈米接觸設計以降低氮化鋁鎵/氮化鎵高電子遷移率電晶體之接觸電阻zh_TW
dc.titleUtilizing Nano-Contact to Reduce the Contact Resistance of AlGaN/GaN High Electron Mobility Transistoren
dc.typeThesis
dc.date.schoolyear105-2
dc.description.degree碩士
dc.contributor.oralexamcommittee吳肇欣(Chao-Hsin Wu),林瑞明(Ray-Ming Lin),孫建文(Jian-Wen Sun),徐大正(Ta Cheng Hsu)
dc.subject.keyword氮化鋁鎵/氮化鎵高電子遷移率電晶體,錯位差排,介面缺陷密度,奈米洞蝕刻,奈米接觸,接觸電阻,zh_TW
dc.subject.keywordAlGaN/GaN HEMT,threading dislocation,interface-trap density,Nano-hole etching,Nano-Contact,contact resistance,en
dc.relation.page58
dc.identifier.doi10.6342/NTU201703646
dc.rights.note未授權
dc.date.accepted2017-08-17
dc.contributor.author-college電機資訊學院zh_TW
dc.contributor.author-dept電子工程學研究所zh_TW
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