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The presence of sGNRs can be seen by a strong absorption band at around 1,060 cm-1.
The ultra-low reflectance of SiNSs is caused by a strong absorption due to the strong light-trapping property of the dense SiNSs.
The FT-IR spectra of as-synthesized hollow magnetite microspheres (Figure 9a) and SiO2@hollow magnetite microspheres (Figure 9b) are characterized by a strong absorption band at ca. 560 cm-1 attributed to the typical band of Fe3O4, corresponding to the stretching vibration modes of Fe-O [42, 45].
The FT-IR spectra of IOMNPs are dominated by a strong absorption band around 540 cm−1, which can be ascribed to Fe-O bond in Fe3O4 nanoparticles [27, 47], indicating that the main phase of the as-synthesized IOMNPs is Fe3O4.
Osseous tissues had the strongest attenuation coefficient which may be explained by a strong absorption from red blood cell precursors in the bone marrow.
(Scheme 3) The electronic absorption spectra of all PPAs are characterized by a strong absorption in the visible region, except for those of 6 c and the Au2 complex 8, which feature additional absorptions at higher energy.
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Reflectivity is indeed reduced from 45 to around 5%, revealing a strong absorption of light by the nanostructured surface of the sample.
When resonance conditions are matched, a strong absorption of the electromagnetic field energy is brought about by metallic NPs [2].
The eGNR spectrum exhibits a strong absorption in the UV and visible region and an absorption edge in NIR.
These compounds exhibit a strong absorption around 520 nm.
In contrast, the interaction of infrared radiation (1 11 μm) with materials is characterized by a strong energy absorption by plasma itself, which completely changes conditions of nanostructuring.
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