AlN/AlGaN/GaN metal insulator semiconductor heterostructure field effect transistor

被引:26
作者
Cho, DH [1 ]
Shimizu, M
Ide, T
Ookita, H
Okumura, H
机构
[1] PERC, Natl Inst Adv Ind Sci & Technol, Tsukuba, Ibaraki, Japan
[2] Adv Power Device Lab, R&D Assoc Future Electron Devices, Tsukuba, Ibaraki, Japan
[3] Ultra Low Loss Power Device Technol Res Body, Tsukuba, Ibaraki, Japan
[4] Meiji Univ, Dept Sci & Technol, Kawasaki, Kanagawa, Japan
[5] Tokyo Univ Sci, Chiba, Japan
来源
JAPANESE JOURNAL OF APPLIED PHYSICS PART 1-REGULAR PAPERS BRIEF COMMUNICATIONS & REVIEW PAPERS | 2002年 / 41卷 / 7A期
关键词
AlN; AlGaN; GaN; MIS; HFET;
D O I
10.1143/JJAP.41.4481
中图分类号
O59 [应用物理学];
学科分类号
摘要
We present the characteristics of a novel AlN/AlGaN/GaN metal insulator semiconductor heterostructure field-effect transistor (MIS-HFET) structure with an AlN cap layer as a gate insulating layer. The gate leakage current for the AlN/AlGaN/GaN MIS-HFET was shown to be more than three orders of magnitude smaller than that for the AlGaN/GaN HFET at around -20V gate bias. This demonstrates that the wide band gap AlN/AlGaN gate structure suppresses the gate leakage current, resulting in improved device characteristics compared with common HFETs in this study. A maximum g(m) of 134 mS/mm was observed at a 4 V drain-source bias of a MIS-HFET with a gate length (L-g) = 0.85 mum, gate width (W-g) = 57 mum, and drain-source spacing (L-ds) = 3 mum. A threshold voltage (V-t) of -3.06 V and a maximum channel current of 551 mA/mm were observed.
引用
收藏
页码:4481 / 4483
页数:3
相关论文
共 10 条
  • [1] Two-dimensional electron gases induced by spontaneous and piezoelectric polarization charges in N- and Ga-face AlGaN/GaN heterostructures
    Ambacher, O
    Smart, J
    Shealy, JR
    Weimann, NG
    Chu, K
    Murphy, M
    Schaff, WJ
    Eastman, LF
    Dimitrov, R
    Wittmer, L
    Stutzmann, M
    Rieger, W
    Hilsenbeck, J
    [J]. JOURNAL OF APPLIED PHYSICS, 1999, 85 (06) : 3222 - 3233
  • [2] LATTICE VIBRATION SPECTRA OF ALUMINUM NITRIDE
    COLLINS, AT
    LIGHTOWLERS, EC
    DEAN, PJ
    [J]. PHYSICAL REVIEW, 1967, 158 (03): : 833 - +
  • [3] The effect of surface passivation on the microwave characteristics of undoped AlGaN/GaN HEMT's
    Green, BM
    Chu, KK
    Chumbes, EM
    Smart, JA
    Shealy, JR
    Eastman, LF
    [J]. IEEE ELECTRON DEVICE LETTERS, 2000, 21 (06) : 268 - 270
  • [4] Advantages of AlN/GaN metal insulator semiconductor field effect transistor using wet chemical etching with hot phosphoric acid
    Ide, T
    Shimizu, M
    Suzuki, A
    Shen, XQ
    Okumura, H
    Nemoto, T
    [J]. JAPANESE JOURNAL OF APPLIED PHYSICS PART 1-REGULAR PAPERS BRIEF COMMUNICATIONS & REVIEW PAPERS, 2001, 40 (08): : 4785 - 4788
  • [5] An AlN/GaN insulated gate heterostructure field effect transistor with regrown n+ GaN source and drain contact
    Kawai, H
    Hara, M
    Nakamura, F
    Asatsuma, T
    Kobayashi, T
    Imanaga, S
    [J]. JOURNAL OF CRYSTAL GROWTH, 1998, 189 : 738 - 741
  • [6] Khan M. A., 1993, Semiconductor Heterostructures for Photonic and Electronic Applications Symposium, P769
  • [7] AlGaN/GaN metal oxide semiconductor heterostructure field effect transistor
    Khan, MA
    Hu, X
    Sumin, G
    Lunev, A
    Yang, J
    Gaska, R
    Shur, MS
    [J]. IEEE ELECTRON DEVICE LETTERS, 2000, 21 (02) : 63 - 65
  • [8] Effect of temperature on Ga2O3(Gd2O3)/GaN metal-oxide-semiconductor field-effect transistors
    Ren, F
    Hong, M
    Chu, SNG
    Marcus, MA
    Schurman, MJ
    Baca, A
    Pearton, SJ
    Abernathy, CR
    [J]. APPLIED PHYSICS LETTERS, 1998, 73 (26) : 3893 - 3895
  • [9] Very high breakdown voltage and large transconductance realized on GaN heterojunction field effect transistors
    Wu, YF
    Keller, BP
    Keller, S
    Kapolnek, D
    Kozodoy, P
    Denbaars, SP
    Mishra, UK
    [J]. APPLIED PHYSICS LETTERS, 1996, 69 (10) : 1438 - 1440
  • [10] High breakdown GaNHEMT with overlapping gate structure
    Zhang, NQ
    Keller, S
    Parish, G
    Heikman, S
    DenBaars, SP
    Mishra, UK
    [J]. IEEE ELECTRON DEVICE LETTERS, 2000, 21 (09) : 421 - 423