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The first column of Figure 5 is the initial LSFs for all the methods.
Here, we draw the red contours to represent their initial contours in the first column of Figure 1.
The original slices and zoomed view of their ROIs are illustrated in the first column of Figure 16.
In the first column of Figure 3, we initialize piecewise constant function (0 and 1) for all methods except GDEWRM, which is initialized with a SDF.
Accordingly, the four charge distributions shown in the first column of Figure 13 possess net dipole moment where (a) and (d) are x-dipoles and (b) and (e) are y-dipoles.
In the first column of Figure 13, we show the charge distribution of the two lowest energy E1u modes in an unstressed gold heptamer structure composed of seven identical gold spheres where the sphere diameter is 150 nm and gap between the spheres is 25 nm.
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Numerical data are presented in the first column of Figures 11, 12, and 13.
A comparison of the non-normalized data from the first columns of Figure 8a and Figure 2a revealed that caMEKK1 increased Sox9 activity by 3.7 ± 0.7 fold (mean ± standard deviation; P < 0.01; data are from the same series of experiments).
The images from the joint correction are given in the third column of Figure 7.
RD images obtained by MERA and MEPA are shown in the second column of Figure 7 corresponding to different SNRs.
The result is the truncated output membership functions as shown in the third column of Figure 4. 3.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com