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PMDL is a simple variant of perfectly matched layers (PML) that is also equivalent to rational approximation-based local ABCs (rational ABCs); it inherits the straightforward approximation properties of rational ABCs along with the versatility of PML.
The local ABC used here is the perfectly matched discrete layer (PMDL) which is a simple variant of perfectly matched layers (PMLs) that is also equivalent to rational approximation-based local ABCs (rational ABCs); it inherits the straightforward approximation properties of rational ABCs along with the versatility of PML.
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They derive a relatively straightforward analytic approximation for catastrophe frequency, consistent with the data in 36.
We show that straightforward discrete approximations to these problems yield approximate problems which are ill-posed.
This improves on the straightforward 2-approximation algorithms for these problems, and generalizes earlier results for 2-connectivity.
However, estimating ng from Ne is not straightforward and approximations used in the literature differ [ 9, 15- 17].
Numerical results for wave transmission through a rectangular connector with linearly tapered thickness and constant width are obtained in a straightforward manner without approximation errors and at a low computational cost, irrespective of frequency.
Also, it is straightforward to recover the approximation done in (24) by considering.
Even though the use of a point-charge approximation is straightforward and in most cases works quite well [108], it has shown some limitations, such as its tendency to overestimate short-range electrostatic (ES) interactions [114], as well as divergence problems during the SCF iterations [104].
With these parameters, we also obtain the Gaussian approximation that is straightforward to use and matches the exact results.
Using Gaussian approximation, it is straightforward to model the effect of PU transmitter's spectral leakage on the actual false alarm probability P ˜ FA as P ˜ FA k = Q λ − σ w 2 + I adj k 1 L t L f σ w 2 + I adj k (9).
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Justyna Jupowicz-Kozak
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