• DocumentCode
    1025619
  • Title

    Sodium distribution in thermal oxide on silicon by radiochemical and MOS analysis

  • Author

    Yon, E. ; Ko, W.H. ; Kuper, A.B.

  • Author_Institution
    Case Institute of Technology, Cleveland, Ohio
  • Issue
    2
  • fYear
    1966
  • Firstpage
    276
  • Lastpage
    280
  • Abstract
    Direct comparison has been made between Na distribution determined radiochemically and electrically in 6000 Å thermal oxide on 10Ω-cm n-type Si. Na within \\tilde{<} 1000 Å of Si/SiO2interface correlates in most cases with MOS flat band voltage shift, i.e. NNa( \\tilde{<} 1000 Å) ≈ +ΔQMOS. Appreciable Na, which does not appear to affect Si surface potential, is found through the bulk of the oxide. Neutron activation of "clean" oxide (grown in wet or dry oxygen) showed ∼1 ppm Na throughout, ∼10 ppm at free surface. Gold was also identified at ppm concentrations but did not correlate with ΔQMOS. The U-shaped profile seen after diffusion (300 to 1000°C in dry N2) or in-drift (∼200°C, 5 × 105V/cm) is believed due to rate limitation at the free surface; electrostatic binding plus enhanced solubility at the Si/SiO2interface. Time dependence was observed in diffusion at 500 and 800°C, which is not expected from the fast diffusion of Na. This is also attributed to the surface rate limitation. The anion significantly affects Na diffusion kinetics and distribution in contamination experiments with radiotracer Na24OH, Na24Cl, and Na24Br82. Br is found to accompany Na diffusion, suggesting anion neutralization of Na within the bulk oxide. P2O5. SiO2is seen to "getter" Na from the oxide. These results support the suggestion of Snow et al. that Na is responsible for uncontrolled drift of surface potential in oxidized Si devices.
  • fLanguage
    English
  • Journal_Title
    Electron Devices, IEEE Transactions on
  • Publisher
    ieee
  • ISSN
    0018-9383
  • Type

    jour

  • DOI
    10.1109/T-ED.1966.15680
  • Filename
    1474270