Based on the SRH theory, many models have been developed in order to describe
hole capture in oxide defects. Unfortunately, most attempts fail for bias
temperature instability, be it because of the missing field dependence or because
of the weak temperature dependence. By using a thermally activated barrier
in the capture and emission rates of the SRH model, Kirton and Uren already
identified that structural relaxation might play an important role to explain the
large timescales observed in
-noise. Their approach is further developed in
the NMP model, where the strong electron-phonon interaction is used
to not only explain the temperature dependence of BTI, but also its
field dependence. Unfortunately not all effects of BTI can be modeled
with the simple rates given by the NMP model. The field dependence
experimentally observed exhibits a stronger than linear dependence and
furthermore no full decorrelation between the capture and emission time
constants is obtained by the simple NMP model. For this reason the NMP
model will be extended to so-called metastable defect states in the next
chapter.