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We calculated the band gap structures of TE and TM waves, and found the TE (TM) wave band gaps of function photonic crystals are wider (narrower) than the conventional photonic crystals.
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A photonic band gap structure of (SiO2/TiO2 5 with Ag system for energy efficient film was proposed theoretically and experimentally.
Doping of fluorine in C3N4 could adjust the band gap structure of C3N4, resulting in altering the emission peak position and increasing the fluorescent intensity.
The doping of fluorine resulted in the partial transformation of the band gap structure of SrTiO3 to Sr(Ti4+1−xTi3+x O3−xFx, by reducing Ti4+ to Ti3+ to compensate for the charge balance in the host lattice.
This indicates that the distribution of the nanopore arrays is another key factor of the band gap structure of nanonets.
In order to confirm our arguments, the band gap structure of 100D nanonets with different passivation conditions is studied here.
First-principles calculation based on density functional theory with the generalized gradient approximation (GGA) were carried out to investigate the energy band gap structure of this special structure.
It is also proved that Si O Si is an effective passivation bond which can change the band gap structure of the nanonets.
Si O Si bond has more effective influence on the band edge region of the nanonets than –H or –OH bonds and is expected to change the band gap structure of silicon nanonets.
Dynamics of nanocones formation by laser radiation in intrinsic semiconductors is shown in Figure 4. Figure 1 Schematic image of a nanocone and a calculated band gap structure of Si.
A calculated band gap structure of Si as a function of the nanowire's diameter using the formula from the paper [14]ΔE g = (2Ћ 2 ζ 2 ) / (m*d 2 ), where 1 / (m*) =1 / (m e *) + 1 / (m h *), (m e * and m h * are electron and hole effective masses, respectively) and d is the diameter, is shown in Figure 1b.
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