• Journal of Semiconductors
  • Vol. 42, Issue 9, 092802 (2021)
Changxi Chen1、2, Quan Wang1、3, Wei Li1, Qian Wang1, Chun Feng1、2, Lijuan Jiang1、2, Hongling Xiao1、2, and Xiaoliang Wang1、2
Author Affiliations
  • 1Key Lab of Semiconductor Materials Science, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
  • 2Center of Materials Science and Optoelectronics Engineering and School of Microelectronics, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, China
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    DOI: 10.1088/1674-4926/42/9/092802 Cite this Article
    Changxi Chen, Quan Wang, Wei Li, Qian Wang, Chun Feng, Lijuan Jiang, Hongling Xiao, Xiaoliang Wang. Effect of the post-gate annealing on the gate reliability of AlGaN/GaN HEMTs[J]. Journal of Semiconductors, 2021, 42(9): 092802 Copy Citation Text show less

    Abstract

    In this paper, we investigated the effect of post-gate annealing (PGA) on reverse gate leakage and the reverse bias reliability of Al0.23Ga0.77N/GaN high electron mobility transistors (HEMTs). We found that the Poole–Frenkel (PF) emission is dominant in the reverse gate leakage current at the low reverse bias region (Vth < VG < 0 V) for the unannealed and annealed HEMTs. The emission barrier height of HEMT is increased from 0.139 to 0.256 eV after the PGA process, which results in a reduction of the reverse leakage current by more than one order. Besides, the reverse step stress was conducted to study the gate reliability of both HEMTs. After the stress, the unannealed HEMT shows a higher reverse leakage current due to the permanent damage of the Schottky gate. In contrast, the annealed HEMT shows a little change in reverse leakage current. This indicates that the PGA can reduce the reverse gate leakage and improve the gate reliability.
    $ E = \frac{{q[{\sigma _{\rm{p}}} - {n_{\rm{s}}}\left( V \right)]}}{{{\varepsilon _0}{\varepsilon _{\rm{r}}}}}, $ (1)

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    $ J = AE\,{{\exp}}\left[ { - \frac{{{{\phi} _{\rm{t}}} - \sqrt {{q^3}E/\pi {\varepsilon _0}{\varepsilon _{\rm{s}}}\left( h \right)} }}{{{k_{\rm{B}}}T}}} \right]{\rm{,}} $ (2)

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    $ {\rm{ln}}\frac{J}{E} = C\left( T \right)\sqrt E + B\left( T \right){\rm{,}} $ (3)

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    $ C\left( T \right) = \frac{q}{{{k_{\rm{B}}}T}}\sqrt {\frac{q}{{{\varepsilon _0}{\varepsilon _{\rm{s}}}\left( h \right)}}} , $ (4)

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    $ B\left( T \right) = \frac{{q{\phi _{\rm{t}}}}}{{{k_{\rm{B}}}T}} + {\rm{ln}}\, m {\rm{.}} $ (5)

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    Changxi Chen, Quan Wang, Wei Li, Qian Wang, Chun Feng, Lijuan Jiang, Hongling Xiao, Xiaoliang Wang. Effect of the post-gate annealing on the gate reliability of AlGaN/GaN HEMTs[J]. Journal of Semiconductors, 2021, 42(9): 092802
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