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The impacts of the surface stiffness, stiction, and engery barrier are normalized by their maximum values in Fig. 4. The result domain can be clearly divided into two regions, one for the nanoscale grooves (left) and the other for the microscale textures (right).
To display signals of different amplitudes in one time-distance plot, the fluctuations of Doppler shifts and v z are normalized by their maximum values.
We subtracted the minimum values from the weighted residual norm and the roughness norm, and we normalized them by their maximum values, respectively.
Fig. 2. The distribution of the eigenvectors for the first 8 modes during period A. Note that the eigenvectors for each mode are normalized by their maximum values.
In Eq. (4), the modes are arranged in descending order, and eigenvectors for each mode are normalized by their maximum values.
Open image in new window Fig. 1 a c The contour maps of the dark photon probability densities, normalized by their maximum values are mapped as functions of x and t. d f The probability distributions of the incident (φi), reflected (φr), and transmitted (φt) pulses.
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The ratios of the maximum stiction length (// over ⊥) are normalized by their maximum value among all textured surfaces and shown as squares in Fig. 4.
The surface stiffness ratios are normalized by their maximum value among all textured surfaces and shown as circles in Fig. 4. The same trend is observed for other samples although that for the nanoscale textured Si surfaces follows a different line.
The amplitudes of the PSDs in each diagram are normalized by their maximum value.
In these figures, the determinant of the FIMs are first normalized (the value of σ 2 becomes irrelevant) by their maximum value and depicted in the dB scale.
All indices were divided by their maximum value, in order to normalize them and to use the same scale for all.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com