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[Author] Etsumasa KAMEDA(2hit)

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  • A New Test Structure for Precise Location Measurement of Hot-Carrier-Induced Photoemission Peak in Subquarter-Micron MOSFETs

    Toshihiro MATSUDA  Mari FUNADA  Takashi OHZONE  Etsumasa KAMEDA  Shinji ODANAKA  Kyoji TAMASHITA  Norio KOIKE  Ken-ichiro TATSUUMA  

     
    PAPER

      Vol:
    E85-C No:5
      Page(s):
    1125-1133

    A new test structure, which has a 0.5 µm line and space polysilicon pattern of which center is aligned on the MOSFET's gate center, is proposed for hot-carrier-induced photoemission analysis in subquarter micron devices. The photoemission-intensity profiles were measured using the photoemission microscope with a liquid N2 cooled CCD imager. We successfully measured a peak position of photoemission intensity from the center of MOSFET's gate with a spatial resolution sufficiently less than 24 nm at the microscope magnification of 1000. The test structure is useful to study the photoemission effects in semiconductor devices.

  • A Study on Hot-Carrier-Induced Photoemission in n-MOSFETs

    Toshihiro MATSUDA  Naoko MATSUYAMA  Kiyomi HOSOI  Etsumasa KAMEDA  Takashi OHZONE  

     
    PAPER

      Vol:
    E82-C No:4
      Page(s):
    593-601

    Profiles of photoemission induced by hot electrons in LDD-type n-MOSFETs with L = 0.35-2.0 µm were measured with a photoemission microscope, which had a capability of 1000 magnification and a spatial resolution of 27 nm/pixel on a CCD imager sufficient to detect profile changes in the channel length direction. Under the bias condition of maximum substrate current, photoemission peaks were located at the LDD-drain edge and the n+-drain edge for the devices with L = 0.35 and L 0.40 µm, respectively. A peak position, only in the case of the 0.35 µm device, shifted toward the drain side by about 80 nm at VD = 7.0 V. Since VD did not affect peak positions in L 0.40 µm devices, the photoemission mechanisms may be different between L = 0.35 µm and L 0.40 µm devices. The photoemission points due to p-n junction breakdown were located at the cylindrical curvature edge of the n+-drain region. Two-dimensional device simulation, even when the lateral electric field, electron temperature and radiative recombination rate were taken into account, could not explain the experimental results completely.