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From the analysis, it is clarified that the coupled Bragg-resonance band gap is much wider than the narrow-banded local resonance and the corresponding effective material properties at band gap could be either positive or negative.
Well-dispersed BiFeO3 nanoparticles with tunable size and band gap could be synthesized at 500 °C.
Therefore, tuning of the graphene band gap could be achieved by surface modification using organic molecule which is required in electronic device applications.
All copolymers show broad absorption bands, and the energy level and band gap could be well fine-tuned by the introduction of thiophene/furan bridges to polymer backbone.
Varying structural characteristics of the PCs by choosing different butterfly wings, the slow photon region of the photonic band gap could be purposely tuned to overlap with strong localized surface plasmon resonance (SPR) region of the Au NPs.
The dispersion relation of the single resonance system, i.e., periodic spring mass system with sub-structure, could be derived based on lattice dynamics and the band gap could be easily identified.
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The optical band gaps could be determined from the curves of (αhυ) n versus hυ, α being the optical absorption coefficient.
That gap could be tough to close.
The width of band gaps could also be enlarged by decreasing dielectric cylinder's radius.
With the working power of ion source in 150 W, the atom percent of N, mean absorbency in visible range, and band gap could reach at the optimal value, which was 22.9 at.%, 44.6%, and 2.81 eV, respectively.
The band gap engineering could be readily realized in the ZnO system using mist-CVD.
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