An experimental study investigates the oxidation-enhanced diffusion of phosphorus in silicon in both heavily doped boron and arsenic backgrounds at 900 and 1100~ This data can be modeled using the interstitial charge state levels to control the equilibrium concentration as a function of doping. The interstitials are assumed to be composed of only positive, negative, and neutral interstitial defects. The same values for the charge states are used to model previously published investigations of boron oxidation-enhanced diffusion under extrinsic isoeoncentration conditions. This indicates that these effects are not strongly dependent on the value of the fractional interstitialey, since two different dopants exhibit similar behavior.Understanding oxidation enhanced diffusion is important for modern process fabrication technology. The use of the lightly doped drain (LDD) MOS devices for channel lengths below 2 izm is critical for reliability concerns. One final step in a typical LDD process involves the anneal of the n § source/drain in dry oxygen to regrow the oxide on the silicon surface. Only through the complete understanding of the processes involved can optimization of the device structure be done. Controlling the junction depth can influence such factors as the diffusion spread under the masks and the depletion capacitance in the well.Shockley and Last 1 derived relationships for the thermal equilibrium concentration of charged defects in semiconductors. These relationships arewhere Eg is the bandgap as a function of temperature, C~ is the concentration of interstitials with the superscript +, o, -refer to the positive, neutral, and negative charge states, respectively, EF and Er are the negative and positive charge state levels, and E~ and E~ refer to the conduction and valence band energies. In thermal equilibrium the total concentration is given by the sum of all the concentrations in the various charge states, and is dependent on the electron concentration. During oxidation, interstitials are injected from and recombine at the surface. Hu 2 derived the surface boundary condition for interstitials during oxidation10_12 V is the surface injection, kl is the surface recombi-] where gl nation rate, D~ is the interstitial diffusivity, and C* is the