The results suggest that the state transition of defective nanomagnet element highly depends on defect type and device's aspect ratio, and the defect type Bd needs the largest coercive field, while the defect type D requires the largest null field for switching.
It is unsurprising that this was the largest null allele class as missing genotypes can be observed regardless of the other genotypes in a family but whether there can be genotype incompatibilities will depend on which genotypes are present.
When the absolute value of the Z score is large, the null hypothesis can be rejected.
As dominance variance was lowered from large to null, the posterior mean of the number of nonzero dominance effects in the model decreased from 58.4 to 4.1 (Table 2).
Adopting a large-aperture null corrector is usually inevitable, and it is imperative to certify the large-aperture null optics in case incorrect final shape of the aspheric mirror is obtained.
Moreover, it is necessary to calibrate and remove errors of the large-aperture null lens and trace errors to surfaces that are easy to obtain high accuracy.
The large-aperture null corrector for convex aspheric mirror is verified and calibrated by a wisely designed small aperture certifying null whose surfaces are either flat or spherical which are easy to be fabricated, measured and assembled.
The GABAergic input to DSGCs is two to ten times larger for null direction motion than for preferred direction motion [5], [6], [7], [8], suggesting that directional inhibition is a key mechanism generating directional responses.
First, inhibitory currents are larger during null motion than preferred motion.
