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Current differences between our simulation and our real physical setup are in the order of 1.45 K mean squared error for faces pointing toward the light source and 2.4 K mean squared errors for shadowed faces.
To facilitate the comparison between our simulation and the back-projection result, we compute the HF slip-rate power over a 10 s sliding windows and apply a spatial Gaussian smoothing with a half-width of 50 km, comparable to the main lobe width of the array response of the USArray and the European array (Fig. 4(b)).
Good agreement of first-order diffraction efficiency is shown, between our simulation and the experimental result offered by [15], as illustrated in Figure 2. So, SMM is verified as a suitable method to further analyze and investigate characters of IPPCs. Figure 2 Comparing experimental and numerical results.
The lack of environmental adaptation is similar to the simulation results of model B, demonstrating a lack of aftereffects in Experiment 3. The other difference between our simulation and patients with cerebellar disorder is the learning rate.
We built this parameter into our simulation, just as we had incorporated pH dependence with a measured pK into the dimer dissociation step and found better correlation between our simulation and the experimental yield at higher pH values (updated Figure 7B).
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Similarly, we compute the difference between our simulations and the fitted power law.
Figure 7 Comparison between our simulations and results from the literature.
It is important to point out that comparison between our simulations and in vivo experiments is qualitative.
One of the differences between our simulations and those in [9] is that we considered three populations rather than two populations.
Agreement between our simulations and the analytical solution is excellent.
The only two discrepancies found between our simulations and observed configurations concerns jkd in models A and B and mgp in models A and and
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