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We repeated this volume calculation until we attained the x, y axis boundaries of the field.
The weight phenotype (rightmost straw plot) is the same as that described in Figures 3 and 4 and is marked by the effect of NZO escaping the ±2 SD axis boundaries.
The OAK produces a good ranking of the innermost 50 compounds (right x-axis boundary in Figure 3) yielding an AUROC of nearly 0.8 for the One-Class AD (Figure 3), whereas the FlexOAK leads to an almost arbitrary ranking on the right AD score boundary (Figure 4).
Previous our original 3-D computational region (the first quadrant) is extended to the second quadrant and axis symmetry boundary conditions are used.
Specifically, for symmetric tilt grain boundaries about the [0 0 1] axis, grain boundaries composed of both B and C structural units show a lower segregation susceptibility than other grain boundaries.
In the first part of the paper, under the hypotheses of axis-symmetrical boundary conditions, elasticity and perfect bond between the phases, new analytical solutions for self-equilibrated axial forces applied at the extremities of the object are derived.
We establish the topological equivalence between the single-axis grain boundary space and the 3-sphere, which in turn enables the use of hyperspherical harmonics as basis functions to construct continuous functions.
Gray lines on the horizontal axis represent boundaries between assembled contigs.
For instance, FGFRs 1,3,4 spans the entire DV axis of boundaries (excluding the floor plate), whereas FGFR2 is more dorsally restricted.
All the physical boundaries along with the axis are adiabatic boundaries.
The grain boundaries consist of twin boundaries when two adjacent grains are oriented close to the [110]c-BN zone axis and the boundary plane is parallel to the {111}c-BN close-packed planes of both grains.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com