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The pigment vermilion is orange-red at maximum intensity; the brown earth pigment burnt sienna is grayer and has a lower degree of orange-red saturation.
Here we considered the following metrics: duration (the time between the start and end dates), mean intensity and maximum intensity (the average and maximum temperature anomaly over the duration of the event) and cumulative intensity (the integrated temperature anomaly over the duration of the event).
Before the PL intensity decaying to 1/e of the maximum intensity, the carrier density in active region is close to the carrier density in TDPL experiments.
In order to compare the emission spectra, we used data collected with the Leica LCS software to determine the position of maximum intensity, the spectrum intensities at 430 and 520 nm, and the full width at the half-maximum intensity (FWHM) of the intensity-wavelength curves.
Considering the mean wavelength at half maximum intensity, the excitation and emission peaks are shifted by 13 and 13.5 nm, respectively.
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On the other hand, the separation of beta particles and gamma photons is difficult due to the maximum intensity of the spots because the intensity levels of these two types of radiation were similar.
The average maximum intensity for the alpha particles, the beta particles, and the gamma photons is shown in Fig. 10(A).
Therefore, the distance between the point of minimum and maximum intensity represents the width of the projected skyrmion in the plane normal to the beam propagation direction.
Similarly in the spectrogram the intensities were scaled by finding the maximum intensity on the time-frequency distribution and calculating relative intensities in the decibel scale.
The position of the maximum intensity of the electric field was also determined.
Thresholds (TS) were determined as a percentage of the maximum intensity in the cross section area of the spheres.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com