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Using their results, Draief and Ganesh [7] derived the upper bound for the expected time that all particles are infected for complete graphs and regular graphs.
Park et al. derived the upper bound of the achievable throughput for the EH SUs under the energy causality and collision constraints [25].
Recently, Payne and Schaefer [9, 10] studied the blowup phenomena and derived the upper and lower bounds of blowup time for some semilinear equations under certain assumptions on reactions and initial boundary data.
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We now derive the upper bound of Pr ( E ).
from which we derive the upper bound on the quantization error as.
Thus, to derive the upper bound, we use specific assignment of channel gains.
We next leverage a technique first used in [11, 22] to derive the upper bound.
We first derive the upper bound of (f_{n,varphi}'(0)).
When deriving the upper bound, we will consider all possible sequences of.
We first derive the upper bound on the probability that the individual completion times of all receivers meet the deadline.
A proof of the Lyapunov stability of the system with integral control is presented, and a method for deriving the upper bound for the regulating gain is shown.
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