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From the dispersion analysis of the whistler doublets and triplets, it is found that the individual whistlers of the doublets and triplets simultaneously observed on the same day are one-hop whistlers having propagation path along higher and closely spaced L-values.
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We may assume that any element in ({mathcal F}) has propagation at most (R>0).
In the IC model, each edge has a propagation probability and influence is propagated by activated nodes independently activating their inactive neighbors based on the edge propagation probabilities.
The corresponding ModCod is determined by the terminal that is under the worst propagation conditions, assuming that all destination terminals (in a beam) have similar propagation conditions.
The edge flame has two propagation velocities.
Different paths may have different propagation delays due to its routing paths or network devices.
McKenzie et al. [35] have investigated propagation properties of IASWs in a bi-ion plasma.
On-chip buses in deep-submicron designs have large propagation delay due to dominant coupling capacitance.
The channel waveguides have shown propagation losses of about 0.1 0.2 dB/cm.
We consider the problem of designing optimal distributed controllers whose impulse response has limited propagation speed.
We have considered propagation of dopant within an environment that damps the motion.
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