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研究生: 劉政志
Liu, Cheng-Chih
論文名稱: 高頻氮化鋁鎵/氮化鎵與氮化鋁銦/氮化鎵高電子遷移率電晶體之製作與分析
The Fabrication and Analysis of High Frequency AlGaN/GaN HEMT and AlInN/GaN HEMT
指導教授: 黃智方
Huang, Chih-Fang
口試委員: 張慈
Chang, Tsu
劉怡君
Liu, Yi-Chun
黃智方
Huang, Chih-Fang
學位類別: 碩士
Master
系所名稱: 電機資訊學院 - 電子工程研究所
Institute of Electronics Engineering
論文出版年: 2012
畢業學年度: 101
語文別: 中文
論文頁數: 67
中文關鍵詞: 氮化鋁鎵/氮化鎵氮化鋁銦/氮化鎵小訊號電路模型
外文關鍵詞: AlGaN/GaN, AlInN/GaN, small signal model
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  • 本論文將就高阻值矽基板(111)上的氮化鋁鎵/氮化鎵高電子遷移率電晶體與氮化鋁銦/氮化鎵高電子遷移率電晶體的高頻與直流特性以及內部小訊號電路元件參數進行比較與分析。
    在直流特性上以閘極線寬0.15μm,閘極至源極1μm的元件來看,氮化鋁銦/氮化鎵試片之元件其最大飽和電流與最大轉導增益分別為1271mA/mm與231mS/mm,而氮化鋁鎵/氮化鎵試片之最大飽和電流與最大轉導增益分別為900mA/mm與187mS/mm,顯見氮化鋁銦/氮化鎵較高的二維電子氣濃度對於飽和電流即直流轉導增益上當有幫助。然而這也使得氮化鋁銦/氮化鎵元件在漏電上卻較氮化鋁銦/氮化鎵來的大。
    而在高頻特性的部分氮化鋁銦/氮化鎵試片之元件的ft與fmax分別為82GHz與70GHz,其值皆高於氮化鋁鎵/氮化鎵元件的75GHz與60GHz然而在功率特性方面則因為氮化鋁銦/氮化鎵元件漏電較嚴重而沒有氮化鋁鎵/氮化鎵理想。
    最後我們透過小訊號電路模型的萃取,比較兩種試片在內部本質小訊號參數上的差異,透過本質參數的比較可以得知氮化鋁銦/氮化鎵元件在本質轉導上確實因其較高的載子濃度而擁有較高的電流與轉導增益以及高頻特性然而其漏電情況也較嚴重。


    In this thesis, we compare the DC and RF characteristics of AlGaN/GaN and AlInN/GaN HEMTs and their equivalent small signal signal circuit model are constructed and compared.
    For the DC characteristics the saturated current density(Idss) and the transconductance(Gm) of the AlInN/GaN HEMT is 1271mA/mm and 231mS/mm respectively which are higher than the AlGaN/GaN’s value 900mA/mm and 187mS/mm because of the higher 2DEG concentration in AlInN/GaN. But the leakage current of the AlInN/GaN HEMT is also higher than that of AlGaN/GaN HEMT.
    For high frequency characteristics, the AlInN/GaN HEMT shows an ft=82GHz and an fmax=70GHz, which is also higher than the AlGaN/GaN’s numbers because of the higher transconductance of AlInN/GaN HEMT. But for RF power characteristics the AlInN/GaN HEMT is poor than AlGaN/GaN HEMT due to the higher leakage current of AlInN/GaN HEMT.
    Finally we extract small signal parameters, contstruct equivalent circuit models, and compare their intrinsic values. From the extracted values, It is found that the intrinsic gm of AlInN/GaN HEMT is higher than the AlGaN/GaN which is also attributed to the higher carrier density on the AlInN/GaN wafer.

    中文摘要 I 英文摘要 II 目錄 III 圖目錄 VII 表目錄 XI 第一章 緒論 1 1.1前言1 1.2 GaN材料特性介紹 2 1.3 極化效應 3 1.3.1 自發性極化效應(Spontaneous polarization) 3 1.3.2 壓電極化效應(Piezoelectric polarization) 4 1.4 AlGaN/GaN與AlInN/GaN HEMT元件文獻回顧 6 1.5 研究動機 8 1.6 論文架構 9 第二章 高頻量測原理 10 2.1 高頻操作下的參數 10 第三章 元件設計及製程步驟 16 3.1 試片磊晶結構 16 3.2 元件製程 16 第四章 元件量測及分析 23 4.1 直流量測結果與分析 23 4.1.1 AlGaN/GaN試片直流特性 23 4.1.2 AlInN/GaN直流特性分析 27 4.1.3 接觸電阻 31 4.2 高頻S參數量測結果與分析 33 4.2.1 AlGaN/GaN S參數量測結果 33 4.2.2 AlInN/GaN試片 S參數量測結果 36 4.3 高頻功率參數量測結果與分析 41 4.3.1 量測原理 41 4.3.2 功率放大器種類 42 4.3.3 元件高頻功率參數量測結果 43 4.4 總結 46 第五章 HEMT小訊號電路萃取 47 5.1 小訊號電路模型理論 47 5.2 外部寄生元件萃取 49 5.2.1 萃取 Cpg、Cpd、Cpf 49 5.2.2 ColdFET measurement─萃取Ls、Lg、Ld、Rs、Rd、Rg等參數 51 5.3 內部本質元件萃取(Cgs、Cgd、Cds、Ri、Rds、gm、τ) 55 5.4 萃取結果與分析58 第六章 結論 62 參考文獻 65

    [1] J. Millan “Wide band-gap power semiconductor devices” IET Circuits Devices Syst.,vol.1, no.5, pp.372–379,Oct. 2007.

    [2] O. Ambacher, J. Smart, J. R. Shealy, Weimann, K.Chu, N. G.Murphy, M.Schaff, W.JEastman, L.F.Dimitrov, R.Wittmer, L. Stutzmann, M.Rieger, J.W.Hilsenbeck “Two-dimensional electron gases induced by spontaneous and piezoelectric polarization charges in N- and Ga-face AlGaN/GaN heterostructures” J. Appl. Phys., vol. 85, no. 6, Mar. 1999.

    [3] S.Kolluri , P.Yi , S. Keller , S.P. Denbaars , U.K. Mishra “RF Performance of N-Polar AlGaN/GaN MIS-HEMTs Grown by MOCVD on Sapphire Substrate,” IEEE Electron Device Lett., vol.30, no.6, pp.584-586, June.2009.

    [4] W.H Man, P.Yi, D.F. Brown, S. Keller, J.S. Speck, U.K. Mishra “High performance N-face GaN microwave MIS-HEMTs with > 70% power-added efficiency,” IEEE Electron Device Lett., vol.30, no.8, pp.802-804, Aug.2009.

    [5] A.Khan, M.Kuznia, J.N. , D.T.Olson, W.J.Schaff,J.W.Burm ,M.S.Shur “Microwave performance of a 0.25 μm gate AlGaN/GaN heterostructure field effect transistor” Applied Physics Letters., vol. 65, no. 9, pp. 1121-1123, Aug 1994.

    [6] J.W.Chung, W.E.Hoke,E.M.Chumbes,T.Palacios “AlGaN/GaN HEMT With 300-GHz fmax” IEEE Electron Device Lett., vol. 31, no. 3, pp. 195-197, Mar. 2010.

    [7] F.Lecourt, Y.Douvry, N.Defrance, V.Hoel, J.C.De Jaeger “High Transconductance AlGaN/GaN HEMT with Thin Barrier on Si(111) Substrate” Solid-State Device Research Conference (ESSDERC), pp281-284 ,14-16 Sept. 2010.

    [8] D.Marti,S.Tirelli,A.R Alt,J.Roberts,C.R.Bolognesi “150-GHz Cutoff Frequencies and 2-W/mm Output Power at 40GHz in a Millimeter-Wave AlGaN/GaN HEMT Technology on Silicon” IEEE Electron Device Lett., vol. 33, no. 10, pp. 1372- 1374 Oct. 2012.

    [9] F.Medjdoub, J.FCarlin , M.Gonschorek, E.Feltin, M.A.Py,D.Ducatteau,C.Gaquiere, N.Grandjean,E.Kohn” Can InAlN/GaN be an alternative to high power / high temperature AlGaN/GaN devices?”Electron Devices Meetin,2006 IEDM 06. International,pp.1-4, Dec. 2006.

    [10] S.Haifeng,A.R.Alt,H.Benedickter,E.Feltin ,J.-F.Carlin, M.Gonschorek,N.Grandjean,C.R.Bolognesi“100-nm-Gate(Al,In)N/GaN HEMTs Grown on SiC With ft=144GHz” IEEE Electron Device Lett, vol. 31, no. 4, pp. 293- 295 Apr. 2010.

    [11] L.S Dong, G.Xiang, G.Shiping,P.Tomás“InAlN/GaN HEMTs With AlGaN Back Barriers” IEEE Electron Device Lett, vol. 32, no. 5, pp. 617- 619 May. 2011.

    [12] S.Tirelli,D.Marti ,S.Haifeng,A.R.Alt,J.-F.Carlin , N. Grandjean,C.R. Bolognesi,” Fully Passivated AlInN/GaN HEMTs With ft/fmax of 205/220 GHz” IEEE Electron Device Lett, vol. 32,no.10,Oct 2011

    [13] P.C. Ely,Jr,” Swept-frequency techniques” Proc. IEEE, vol.55, pp.991-1002,no.6,Jun.1967.

    [14] T.R.Prunty , J.A Smart , E.N Chμmbes , B.K Ridley , L.F. Eastman,J.R.Shealy “Passivation of AIGaN/GaN Heterostructures with Silicon Nitride For Insulated Gate Transistors” in Proc IEEE/Cornell High-Performance Devices Conf, pp. 208–214,2000.

    [15] P.Kordoš,P.K.udela,D.Gregušov´a.D.Donoval1 “The effect of passivation on the performance of AlGaN/GaN heterostructure field-effect transistors,” Semicond. Sci. Technol, vol. 21, no. 12, 2006.

    [16] P.A Lamarre “Developer Selection for T-Shaped Gate FET's Using PMMAIP [MMA-CO-MAAIIPMMA]” IEEE Trans on
    electron devices. vol. 39,no. 8. Aug 1992.

    [17] G.Dambrine,A.Cappy,F.Heliodore,E.Playez “A New Method for Determining the FET Small-Signal Equivalent Circuit” IEEE Trans Microwme Theory Tech, vol. 36, no. 7, pp. 1151-1159,Jul.1988.

    [18] F.Diamand,M.Laviron “Elements of Microwave MESFET under Zero Current Conditions”12 th European Microwave Conference Proceedings, pp. 451-456, Sep. 1982.

    [19] F.Qian,J.H Leach, H.Morkoc ” Small Signal Equivalent Circuit Modeling for AlGaN/GaN HFET: Hybrid Extraction Method for Determining Circuit Elements of AlGaN/GaN HFET” Proc. IEEE, vol. 98, pp.1140-1150, no. 7, Jul. 2010.

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