• Journal of Semiconductors
  • Vol. 40, Issue 4, 042801 (2019)
Shuxin Tan1 and Takashi Egawa2
Author Affiliations
  • 1School of Electronics and Information, Nantong University, Nantong 226019, China
  • 2Research Center for Nano-Device and System, Nagoya Institute of Technology, Gokiso-cho, Showa-ku, Nagoya 466-8555, Japan
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    DOI: 10.1088/1674-4926/40/4/042801 Cite this Article
    Shuxin Tan, Takashi Egawa. Influence of growth conditions of oxide on electrical properties of AlGaN/GaN metal–insulator–semiconductor transistors[J]. Journal of Semiconductors, 2019, 40(4): 042801 Copy Citation Text show less

    Abstract

    AlGaN/GaN metal–insulator–semiconductor high-electron-mobility transistors (MIS-HEMTs) on a silicon substrate were fabricated with silicon oxide as a gate dielectric by sputtering deposition and electron-beam (EB) evaporation. It was found that the oxide deposition method and conditions have great influences on the electrical properties of HEMTs. The low sputtering temperature or oxygen introduction at higher temperature results in a positive equivalent charge density at the oxide/AlGaN interface (Nequ), which induces a negative shift of threshold voltage and an increase in both sheet electron density (ns) and drain current density (ID). Contrarily, EB deposition makes a negative Nequ, resulting in reduced ns and ID. Besides, the maximum transconductance (gm-max) decreases and the off-state gate current density (IG-off) increases for oxides at lower sputtering temperature compared with that at higher temperature, possibly due to a more serious sputter-induced damage and much larger Nequ at lower sputtering temperature. At high sputtering temperature, IG-off decreases by two orders of magnitude compared to that without oxygen, which indicates that oxygen introduction and partial pressure depression of argon decreases the sputter-induced damage significantly. IG-off for EB-evaporated samples is lower by orders of magnitude than that of sputtered ones, possibly attributed to the lower damage of EB evaporation to the barrier layer surface.
    $ {d_{{\rm{ins}}}} = {\varepsilon _{{\rm{ins}}}}{\varepsilon_{\rm{o}}}(1/{C_{{\rm{MIS}}}} - {\rm{ }}1/{C_{{\rm{AlGaN}}}}), $ (1)

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    ${n_{\rm{s}}} = \mathop \smallint \nolimits_{{V_{{\rm{th}}}}}^0 C{\rm{d}}V, $ (2)

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    $n_{\rm{s}}^{{\rm{Schottky}}} = \frac{{{\sigma _{\rm{p}}}}}{q} - \frac{{{C_{{\rm{AlGaN}}}}\left( {{\phi _{\rm{b}}} - \frac{{\Delta {E_{\rm{c}}}}}{q} + \frac{{\Delta E_{\rm{F}}^{{\rm{Schottky}}}}}{{{q}}} - {V_{\rm{G}}}} \right)}}{q},$ (3)

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    $ \begin{split} &n_{\rm{s}}^{{\rm{MIS}}} = \frac{\sigma _{\rm{p}}}{q} -\\ &C_{\rm{MIS}}\frac{{ {\phi _{\rm{b}}^{\rm{'}} - \frac{{\Delta E_{\rm{c}}^{{\rm{ins}}}}}{q} - {\rm{}}\frac{{\Delta {E_{\rm{c}}}}}{q} + \frac{{\Delta E_{\rm{F}}^{{\rm{MIS}}}}}{q} - {V_{\rm{G}}}} }}{{{q}}} + {C_{{\rm{MIS}}}}\frac{{q{N_{{\rm{equ}}}}}}{{{C_{{\rm{ins}}}}}}, \end{split}$ (4)

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    $\Delta{E_{\rm{F}}} = {E_1} + \frac{{\pi {\hbar ^2}}}{{{m^*}}}{n_{\rm{s}}}, $ (5)

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    ${E_1} = {\left( {\frac{{9 \pi \hbar {q^2}}}{{8\sqrt {8{m^*}} {\varepsilon _0}\varepsilon }}{n_{\rm{s}}}} \right)^{2/3}}, $ (6)

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    $\begin{split} n_{\rm{s}}^{{\rm{MIS}}} =\;\,& n_{\rm{s}}^{{\rm{Schottky}}} + \frac{{{C_{{\rm{AlGaN}}}}\left( {{\phi _{\rm{b}}} - \frac{{\Delta {E_{\rm{c}}}}}{q} + \frac{{\Delta E_{\rm{F}}^{{\rm{Schottky}}}}}{q} - {V_{\rm{G}}}} \right)}}{{{q}}}\\ & -{C_{{\rm{MIS}}}}\frac{{ {\phi _{\rm{b}}^{\rm{'}} - \frac{{\Delta E_{\rm{c}}^{{\rm{ins}}}}}{q} - {\rm{}}\frac{{\Delta {E_c}}}{q} + \frac{{\Delta E_{\rm{F}}^{{\rm{MIS}}}}}{q} - {V_{\rm{G}}}} }}{{{q}}} \\ &+ {C_{{\rm{MIS}}}}\frac{{q{N_{{\rm{equ}}}}}}{{{C_{{\rm{ins}}}}}}. \end{split}$ (7)

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    Shuxin Tan, Takashi Egawa. Influence of growth conditions of oxide on electrical properties of AlGaN/GaN metal–insulator–semiconductor transistors[J]. Journal of Semiconductors, 2019, 40(4): 042801
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