Theory of dopant diffusion assuming nondilute concentrations of dopant-defect pairs

Abstract
Current dopant diffusion theory is based on dopant‐point‐defect interaction, and assumes that the number of dopant‐defect pairs is much smaller than the unpaired dopant concentration. In cases where a large number of excess defects are created from implantation damage, this may no longer be a valid assumption. A new derivation of the dopant and defect equations is presented which is valid for any concentration of dopant‐defect pairs.