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On the contrary, the MWMZ method maintains an acceptable level of the KLD even for the high shadow fading standard deviation.
The resulting method maintains an exact representation of the (prescribed) moving boundary at the discrete level, or an approximation of the appropriate order, yet is immune to large distortions of the mesh under large deformations of the domain.
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The queue created using such a method maintains a reverse ordering of a FIFO queue.
While doing this, the in-degree method maintains a very low false positive rate.
This method maintains a lower bound on α k (how to maintain this lower bound will be explained in Section 4.3).
The overall method maintains a smooth geometrical description of the interface and the implementation simplicity characteristic of the level set method.
The new method maintains a 3rd order error even with these additional terms and models the equation in all three spatial dimensions and time.
However, unlike in typical undrained experiments where pore pressure is allowed to vary, the modified method maintains a constant pore pressure, and instead relies on the simultaneous manipulation of the confining pressure and axial stress to maintain a constant pore fluid pressure.
The method maintains a smooth geometrical description of the interface for both two-dimensional and three-dimensional tests with accurate volume conservation even in very challenging situations where the fluid bodies progressively deform and stretch developing localized regions with very high curvature and thin fluid filaments.
The MD method maintains a very creditable performance level for all the α values.
In experiments on two other big pedigrees (size 22 and 23), our method maintains a locus-by-locus IBD inference error rate <1%.
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