7.3 Extraction Routine

The determination of the curvature following bias temperature stress is displayed in Fig. 7.5. First, each relaxation of V
 TH   is referred to its initial V
 TH,0   and is plotted as ΔVTH   as a function of log(t)  . The first decades as well as the last decade in time are used to fit the experimental data with a logarithm of the form a+ b log(t)  , giving the initial and long term recovery behavior. Eventually, the intersection of the two fits results in the “kink points” τA   and τB   . While τA   is used to describe the initial recovery phase generally observed after PBTI, τB   is used for the long term recovery as observed after NBTI. These two cases are depicted in the right of Fig. 7.4. However, the kink-point-method does not work properly with too similar logarithmic prefactors b1   and b2   due to glancing intersection, compare Eox = ±6MV   ∕cm  and tstr = 100s  in Fig. 7.5. For the already discussed complete recovery trace with its S-shape, the first and second fit become nearly parallel resulting in an undetermined kink point.


PIC


Figure 7.5: The relaxation behavior starts to deviate from the logarithmic shape at harsher stress conditions. By fitting the beginning and the end of the recovery traces separately, a kink point τA   or τB   at the extrapolated intersection of the fits can be obtained, which characterizes the curvature. Comparing kink points of the same electric field and oxide thickness for different stress times (connected by dotted lines) shows that this curvature is stronger at longer stress times and delayed with time.