The prefactor of the log-fit for various , , and is displayed in Fig. 6.13. In agreement with previous experiments, it is observed that low results in small temperature activation, while larger than the operating voltage of the MOSFET gives a notable activation energy of . Note that this value is in agreement with activation energies extracted at long stress times [106]. Fitting the data to a power-law results in an exponent for short-term stress, roughly a third of the often reported of the long-term behavior. This is in very good accordance with the standard for NBTI stress and accounts for a strong dependence, excluding elastic hole tunneling.
Figure 6.14 represents the prefactor plotted for different at different temperatures. In the devices with , all the stress voltages are above the operating voltage and result in a marked temperature activation. For the transition from no temperature activation to temperature activation is observed between and for . For the thickest oxides used in this study, , the applied stress fields are too small to lead to a meaningful degradation2 . Therefore no objective statement can be made on temperature activation concerning the here presented devices with .
However, the experiments performed on devices with smaller oxide thicknesses support thermally activated tunneling mechanism [98] rather than elastic (and thus temperature-independent) hole tunneling [94].