Using numerical simulations, the cavity resonances and their effects on the reflection of the gratings are identified and further analyzed.
Auxiliary experiments at constant irradiation energy and at different tilt sample angles were carried out to confirm the effect of the reflection of the incoming ions on the resilience of FLG.
Since the mimicked free surface is bounded, we also assume an absorbing boundary condition (e.g., Cerjan et al. 1985) along the perimeter of the free surface to reduce the effect of the reflection by artificially attenuating waves.
In contrast, using the hue of the as-acquired images to monitor complete degradation is limited due to the interfering effect of the reflection of the broad light source spectrum from the porous silicon, silicon substrate, and other surfaces within the light path.
In the four transmitter case, the RMSDS at position 1 is comparable to that at position 9 for the circular emission since the effect of the reflections is almost the same near the corner (position 1) and near the wall (position 9), regardless of the shape of the emission cross-section.
Effects of the acoustic reflection coefficient on self-sustained combustion oscillations are investigated and a passive control solution is proposed, using perforated plates with bias flow.
Except when (theta_{0}=0) or (pmpi /2), this would have the effect of breaking the reflection symmetry of θ, because applying the new reflection would not preserve the lattice.
If all the models of the network component are available, it is possible to analyze the network behavior in real operation conditions, verifying the effects of the network reflections, timings, and so forth.
The λ/4 P2 layer introduces a π phase shift in the reflections from the interfaces either side of the P2 layer, suppressing the effect of these reflections in the transmitted beam (similar to an antireflection coating).
