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Thus in our example in Figs. 5, 6 and 7, for a propagated distance of z < 3 mm, shearing has advantage of requiring less memory than the Radon transform.
At sufficiently low fluorescence concentrations, the original numerical phantom became obscured by the simulated noise (for example in Figs. 7m and 7q).
However, the example in Figs. 7b and 9 showed that all the 54 EEG electrodes were needed for recovering the deeper aspects of the source even in fusion.
This can be clearly seen, for example, in Figs. 2(c) and (e): In Fig. 2(c), granule cells (red) can be easily differentiated from myelin rich tissue (green), while Fig. 2 e) provides no further chemical information besides lipid contrast.
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For each ROI (example in Fig. 3, c1), we generated Minimum Spanning Tree graphs (Fig. 3, c2) (Supplementary Methods).
For example, in Fig. 1(c) there is \(b=1\) backbone, \(n=2\) chords, and \(r=1\) boundary (drawn in red).
As an example, in Fig. 3, we have provided the motifs of the two MRs, POU3F3 and SOX3.
Indeed, the behavioral time courses of rivalry and replay are quite close (see an example in Fig. 1d, and the relatively similar gamma distributions in Supplementary Fig. 1).
This can be seen for example in Fig. 3 of this web page that Gabe Vecchi and I have.
As an example in Fig 2a-3, we show a high magnification SEM image of two typical individual nanocubes (particles number P6 and P7).
Example: Consider the example in Fig. 7.
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CEO of Professional Science Editing for Scientists @ prosciediting.com