ABSTRACT

A doped semiconductor can be viewed as a mixed electronic-ionic conductor, with the dopants as mobile ions. Normally the temperature range where this becomes true is not even close to that where the (opto)electronic properties of the material are of interest. However notable exceptions exist and some examples of these are reviewed here. We limit ourselves to those cases where semiconductivity is preserved when the (mobile) dopant concentration changes and ambipolar behaviour can be obtained by dopant mobility. Dopant diffusion and drift are of interest not only in materials such as Si:Li, known from its use in radiation detectors, but also in ternary semiconductors, such as (Hg,Cd)Te and CuInSe2. Understanding the phenomena is important not only for low-temperature doping, but also because of the implications that it has for device miniaturization, as dopant diffusion and drift impose chemical limits on device stability.