Although the simulated trend of circular polarization spectra is well matched to the laboratory data and suggests that our model correctly reproduces polarization trends, the magnitude of the modeled results is several orders smaller than measured in the lab.
The model correctly reproduces the nonlinear behavior observed for different resonator designs.
The model correctly reproduces the observed discharge at the basin outlet.
Our results show that the Gō model correctly reproduces the cooperative, two-state, folding mechanism of the WW-domain, while the SHG model predicts a transition occurring in two stages: a collapse, followed by a structural rearrangement.
The model correctly reproduces some observations concerning the mechanisms of attentional control, such as the coherence of spikes in the population of neurons included in the focus of attention, and the inhibition of neurons outside the focus of attention.
The analytical model correctly reproduces the stress strain curve in the presence of a debonding process although overestimating the size of the debonding cavity which is obtained by comparison between experiments and FEM simulations.
For the statistically stationary case, the mean and RMS progress variable are in very good agreement with experimental data, demonstrating that the model correctly reproduces the flame anchoring and the flame turbulence interactions in the recirculation zone.
It can be seen that the model correctly reproduces the change in conduction mechanism: whereas the hole current is much larger than the ion current inside the silicon, the opposite is true in the electrolyte.
The model correctly reproduces the polarimetric data, including a pronounced negative polarization at small phase angles and the positive polarization with the maximum value less than 30% at the phase angle around 95? and red polarimetric color.
In addition, the model correctly reproduces the switching-off of the UV lesion bypass signal at low UV doses.
