The anisotropic hyperfine splitting due to nitrogen nucleus observed at −196°C, which is a good measure of the magnitude of the PS-silica interaction, is larger for the adsorbed PS from the CCl4 solution and the PS on the silica with the larger pore diameter.
Since the energy gained from the double exchange interaction is larger than that from the super-exchange interaction due to the existence of large exchange splitting ε dd, the FM states are favored in the Cr-doped ZnO nanowire, which is also true for the Fe doped in ZnO nanowire.
This may overestimate the sample size requirement, especially if the effect of the interaction is larger than the main effects, but it illustrates the general requirement for a larger sample size when interactions are introduced into hypothesis testing.
With equal interstitial and intracellular longitudinal conductivities and close coupling, the interaction was large enough (induced Vm approximately 20 mV peak-to-peak) that action potentials from one fiber initiated excitation in the other, for the 40-microns radius evaluated.
The values of the Interaction Contrast Ratios indicate that the excess risk due to the interaction was large relative to the risk without either exposure.
The excess risk due to BMI was small compared with that due to alcohol, but the relative excess risk due to interaction was large (5.58, 95% CI 1.09 to 10.1).
Since the number of interactions is large, we only analyze the top twenty interactions, the others could be analyzed similarly.
According to Fig. 8b, for quite a few gene pairs with high function similarity (>0.9) in terms of cellular component, their genomic distance varies a lot when the number of interactions are small, however, when the number of interactions is large, their genomic distance is short.
Nitrogen dioxide effects were consistently modified, but p-values for interaction were larger (0.09 and 0.19, respectively).
In all studies, the proportion attributable to the interaction was larger than the individual effect of physical inactivity.
