Exact(19)
Plots are presented to facilitate the design of filter parameters matching the physics requirements on the maximal error.
A 2016 paper the two published together in Linear and Multilinear Algebra ("On the Maximal Error of Spectral Approximation of Graph Bisection") evaluates how precisely such work can be performed.
It creates filters that are optimal in the L-infinity sense – that is, it minimizes the maximal error present within the pass and stop bands regions of the filter.
The simulation results show that the arrival angle and drift velocity will be underestimated in all the conditions and the maximal error will be about −0.87° and −121 m/s, respectively.
The galvano-charge current also leads to the error due to the semi-conductive character of LiMn2O4, and the maximal error may reach as much as one order of magnitude.
We now consider a random design matrix Xn and the case n→∞ and study the probability P0(max1⩽i⩽n |xi′β̂n|⩾γn) with γn=F−1(1−1/n), a population analog of the maximal error.
Similar(41)
The maximal errors of the numerical solutions under various mesh steps (h=tau) at (t=10) are listed on Table 2.
In Example 2, the maximal errors of the numerical solutions at different time t for Scheme III are listed on Table 3.
The maximal errors were 5.35 mm and 4.58 mm for the right carotid bifurcation LM, respectively.
The maximal errors were 2.63 Gy and 2.74 Gy for the right PG LM, for each of the method, respectively.
In this sense, the reported errors correspond to the mean and maximal error in the computational domain.
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