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In fact, in both fluorescence and reflectance modes the absorption properties of a specimen have a negative impact on image contrast by attenuating the illuminated beam and backscattered or fluorescence signal.
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In comparison, NWs with larger diameters provide more supported modes; hence, the absorption is greatly increased when these modes are well coupled and concentrated within the NWs.
Newton's method is used to find the complex wavenumbers of radial modes for the absorption boundary condition.
Considering the arrays of multilayer hollow nanopillars (crystalline-Si/Ag/air) with the appropriate geometrical sizes, three kinds of optical modes at the absorption profile in the wide range of the spectrum are reported.
This gives the distribution of the resonant modes in the absorption region.
Finally, strong fields at interfaces can also lead to leaky modes enhancing the absorption in the vicinity similarly to the near fields.
The band located at 417 cm−1 is a typical ZnO absorption attributed to the bending vibration absorption of Zn-O bond, which corresponds to the E1 symmetry transverse optical phonon mode, and the absorption intensity is increased obviously.
Sweatlock and coworkers performed theoretical calculations with the objective of establishing the contribution of the longitudinal plasmon mode to the absorption spectrum of one-dimensional arrays of 4, 8, and 12 spherical silver nanoparticles [18].
Most prominent are IR bands in the 620 660 cm−1 range corresponding to bending Si H2 mode and the absorption band located at 1100 cm−1 that can be related to valence Si O Si vibrations [29, 30].
Since these modes strongly affect the absorption spectra, the knowledge of the existence of two different modes and their interaction is essential to designing light trapping plasmonic grating structures for photovoltaic devices.
Only when the resonant modes lie within the absorption region, they can contribute to the photocurrent.
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