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The four smallest spheres were filled with a target-to-background ratio (TBR) of 4 1.
The two smallest spheres were underestimated for all three methods (RC = 0.40 0.82).
The data for the 7.5 1 contrast ratio scan and the five smallest spheres are presented therein.
are (approximations for) the radii of the smallest spheres centred on z and s and containing all sources and sinks, respectively.
The four smallest spheres were filled with a target-to-background ratio (TBR) of 8 1 (first set of scans) and 4 1 (second set of scans).
The influence of varying reconstruction parameters is demonstrated for the four smallest spheres in Table 3 and plotted in Fig. 5.
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Conventionally, the length a is defined as the radius of the smallest sphere which completely encapsulates the antenna7,8.
RCs lie in the range 0.2 0.86 for the smallest sphere and largest sphere, respectively.
The smallest sphere possible to segment using a threshold-based method was 13 mm.
However, for the smallest sphere, a small increase in recovery could still be noted even after six iterations.
RCs range from 0.2 for the smallest sphere to 0.86, approximately, for the largest sphere (Fig. 1e).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com