透過您的圖書館登入
IP:3.147.47.108
  • 學位論文

P型氮化鎵MOS-HEMT模擬與設計

Simulation and Design of P-GaN MOS-HEMT

指導教授 : 黃智方
若您是本文的作者,可授權文章由華藝線上圖書館中協助推廣。

摘要


在本篇論文中,首先利用TCAD擬和氮化鋁鎵/氮化鎵異質結構的Transmission Line Model(TLM)模型,再進一步模擬自熱效應觀察元件內部現象。利用建立好的模型模擬氮化鋁鎵/氮化鎵雙金屬蕭基二極體,其電流誤差在±10%。 此外設計P型氮化鎵MOS-HEMT達到常關型元件,使用氧化鋁材料作為閘極介電質可降低漏電流,藉由調變通道長度及摻雜濃度可有效調整元件達最佳化。加入本質氮化鎵當作通道,可以提升特性元件,大幅降低臨界電壓達到更高的飽和電流,並估算在通道長度為0.4µm且閘極-汲極長度為10µm的本質氮化鎵通道MOS-HEMT,導通電阻為3.7 mΩ•cm2,而通道導通電阻為0.41mΩ•cm2,佔總阻值的11%,最大阻值來源於閘極-汲極端約1.75 mΩ•cm2佔總阻值的47%。

並列摘要


In this thesis, we used TCAD for fitting AlGaN/GaN heterojunction Transmission Line Model (TLM) I-V characteristics. A physics-based model of self-heating is included in TCAD simulations to investigate the internal device behavior. A dual metal Schottky Barrier Diode (SBD) is also simulated with the constructed models. The fitting errors of less than ±10% for DC I-V characteristics in both cases have been achieved. Another topic of this thesis is to design a normally-off p-GaN MOS-HEMT. A p-GaN MOS-HEMT with Al2O3 as the gate dielectric can significantly reduce the gate leakage current and achieve normally-off operation. To build the best performing device we optimized the channel length and doping concentration of the p-GaN. A p-GaN MOS-HEMT performance can also be improved by adding an i-GaN layer as the channel layer. Compared with a p-GaN MOS-HEMT, the i-GaN layer design reduced the threshold voltage and increased the saturation current. The i-GaN channel MOS-HEMT with a channel length of 0.4µm and a gate-drain length of 10µm shows a specific on-resistance as low as 3.7mΩ•cm2. The channel region resistance is 0.41mΩ•cm2 which contributes about 11% of the total resistance. The largest part of the total resistance is 1.75mΩ•cm2 from the gate-drain distance and it contributes about 47%.

並列關鍵字

GaN MOS-HEMT

參考文獻


[1]J. Liu, Y. G. Zhou, R. M. Chu, Y. Cai, K. J. Chen, and K. M. Lau, “Highly Linear Al0.3Ga0.7N-Al0.05Ga0.95N-GaN Composite- Channel HEMTs,” IEEE Electron Device Lett., vol. 26, no. 3, pp. 145–147, Mar. 2005.
[2]T. P. Chow and R. Tyagi, “Wide Bandgap Compound Semiconductors for Superior High-Voltage Unipolar Power Devices,” IEEE Trans. Electron Devices, vol. 41, no. 8, pp. 1481–1483, Aug. 1994.
[3]F. Ren, M. Hong, S. N. G. Chu, M. A. Marcus, M. J. Schurman, A. Baca, S. J. Pearton, and C. R. Abernathy, “Effect of temperature on Ga2O3(Gd2O3)/GaN metal-oxide-semiconductor field-effect transistors,” Applied Physics Lett., vol. 73, no. 26, pp. 3893–3895, Dec. 1998.
[4]M. A. Khan, J. N. Kuznia, J. M. V. Hove, N. Pan, and J. Carter, “Observation of a two-dimensional electron gas in low pressure metalorganic chemical vapor deposited GaN-AlxGa1-xN heterojunctions,” Applied Physics Lett., vol. 60, no. 24, pp. 3027–3029, Jun. 1992.
[5]M. A. Khan, M.S. Shur, and Q. Chen, “High transconductance AlGaN/GaN optoelectronic heterostructure field effect transistor,” IEEE Electronics Lett., vol. 31, no. 24, pp. 2130–2131, Nov. 1995.

延伸閱讀