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It can be seen that the extinction coefficient also decreases with the increased wavelength.
In the 1020 2500-nm range, the transmittance increased with the increased wavelength.
Except for a decrease in the focal length introduced by the increased wavelength, the intensity of the focal spot for the wavelength of 681 nm is almost 100 times more than that of λ = 581 nm.
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Our result shows that the Kerr rotation angle increases with the increasing wavelength of the incident light, while the difference between the spectras of Fe and CoFeAl is attributed to plasma resonance.
The R of all the coatings increases slightly with the increasing wavelength.
From this figure, the refractive index decreases with the increasing wavelength (400 to 800 nm).
Unlike the increasing wavelength, the increase in power density led to more ordered and shaped nanostructures, presumably because of the increase in energy rate.
However, the R of all samples gradually increased with the increasing wavelength due to the maximum of the scattering and reflectance efficiencies at the high wavelength [1].
The UV Vis absorption spectra of aGQDs showed characteristic peak at around 230 nm and the absorption intensity decreased with the increasing wavelength, which was consistent with the previous report [6].
For the non-cross-linked films, the percentage of light transmission was gradually increased from 20% up to 60% along the increasing wavelength from 400 to 800 nm.
The increasing percentage of light transmission along the increasing wavelength was also observed for the genipin-cross-linked films; however, their light transmission percentages tended to drop at the wavelength around 520 680 nm.
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