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Models in Fig. 4f, g are used to simulate the cases that the self-connecting occurs between the neighboring pyramids at different sites on the Si (001) faceted sidewall.
To demonstrate this, we have considered several sets (combinations) of the parameters σ si 2 and k for the model (1) to simulate the cases of dominant additive noise and dominant signal-dependent noise with different intensities.
A continuum mixed-mode damage model is developed in order to better simulate the cases where adhesive thickness plays an important role.
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The semi-permeable crack-face magnetoelectric boundary conditions are utilized to simulate the case of an opening dielectric crack.
We simulate the case that ε ˆ ≠ ε and β ˆ ≠ β.
By not adding any noise on the pilot symbols we can also simulate the case of perfect CSIR.
We simulate the case where the same RNS-FH pattern used in the cell of interest is assigned to adjacent interfering cells.
As we simulate the case where (R 2sel) n = (R 1sel) n, (del2lini,j) n will be superior than (dellini,j) n because it includes deli,j.
We used the same material as in the first experiment, but to simulate the case in which the spoken utterance is not present in the list, we also generated language models in which the correct utterance is left out.
In Figure 3 we simulate the case of a persistent inflammatory response which corresponds to an increased exposure of the host response to the inflammatory stimulus (LPS).
By doing so, we simulate the case in which only the first 3 (2 for GLY) MS peaks were measured, and had not been normalized.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com