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[Author] Naoteru SHIGEKAWA(3hit)

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  • Improved Carrier Confinement by a Buried p-Layer in the AlGaN/GaN HEMT Structure

    Kenji SHIOJIMA  Naoteru SHIGEKAWA  Tetsuya SUEMITSU  

     
    LETTER-Semiconductor Materials and Devices

      Vol:
    E83-C No:12
      Page(s):
    1968-1970

    The authors have demonstrated AlGaN/GaN HEMTs with lightly-doped buried p-layers under the channel for the first time. A 1.5-µm-gate device showed good pinch-off characteristics, gm of 25 mS/mm, and breakdown voltage of 70-90 V. Carrier confinement by the p-n junction was confirmed by capacitance-voltage measurements. These results indicate the potential of p-layer insertion into GaN-based FETs.

  • Analysis of Passivation-Film-Induced Stress Effects on Electrical Properties in AlGaN/GaN HEMTs

    Naoteru SHIGEKAWA  Suehiro SUGITANI  

     
    PAPER-GaN-based Devices

      Vol:
    E93-C No:8
      Page(s):
    1212-1217

    Effects of stress in passivation films on the electrical properties of (0001) AlGaN/GaN HEMTs are numerically analysed in the framework of the edge force model with anisotropical characteristics in elastic properties of group-III nitrides explicitly considered. Practical compressive stresses in passivation films induce negative piezoelectric charges below the gates and bring forth a-few-volt shallower threshold voltages. In addition, the shift in the threshold voltage due to the compressive stress is proportional to LG-1.1-1.5 with gate length LG, which is comparable to the expectation based on the charge balance scheme. These result suggest that passivation films with designed stress might play a crucial role in realising AlGaN/GaN HEMTs with shallow or positive threshold voltages.

  • Dependence of Electrical Properties of InAlN/GaN and InAlN/AlGaN/GaN Heterostructures FETs on the AlN Interlayer Thickness

    Masanobu HIROKI  Narihiko MAEDA  Naoteru SHIGEKAWA  

     
    PAPER-Compound Semiconductor Devices

      Vol:
    E93-C No:5
      Page(s):
    579-584

    We investigated the influence of the thickness of the AlN interlayer for InAlN/GaN and InAlN/AlGaN/GaN heterostructures. The AlN thickness strongly affects the surface morphology and electron mobility of the InAlN/GaN structures. The rms roughness of the surface increases from 0.35 to 1.2 nm with increasing AlN thickness from 0 to 1.5 nm. Large pits are generated when the AlN is thicker than 1 nm. The highest electron mobility of 1470 cm2/VS is obtained for a 0.75-nm-thick AlN interlayer. The mobility, however, becomes lower with increasing deviation from 0.75 nm. It is only 200 cm2/VS for the 0-nm thick AlN. Inserting AlGaN between AlN and InAlN suppresses the influence of the AlN interlayer thickness. A smooth surface with rms roughness of 0.35 nm is obtained for all samples with 0-1.5-nm-thick AlN. The electron mobility ranges from 1000 to 1690 cm2/VS. The variation is smaller than that for InAlN/GaN. We fabricated field effect transistors (FETs) with gate length of 2 µm. The electron mobility in the access region affects the transconductance (gm) of FETs. As a results, the influence of the AlN thickness for InAlN/GaN FETs is larger than that for InAlN/AlGaN/GaN FETs, which reduces gate leakage current. The transconductance varies from 93 to 235 mS/mm for InAlN/GaN FETs. In contrast, it varies from 180 to 230 mS/mm for InAlN/AlGaN/GaN FETs. These results indicate that the InAlN/AlGaN/GaN heterostructures could lead to the development of GaN-based FETs.