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Additionally, by increasing the defect thickness, it is also possible to have a filter with multiple resonant peaks, leading to a multichannel filter.
Finally, by increasing the defect thickness leads to the presence of multiple defect modes which can be used to design a multichanneled filter.
It is found that the positions and the number of defect modes can be significantly changed due to the change in the defect thickness.
It is found that, within the photonic band gap, the number of defect modes (transmission peaks) will decrease as the defect thickness increases, in sharp contrast to the case of using usual dielectric defect.
For the same dielectric constituents and the same (or closest to same) number of layers, pre-fractal structures are remarkably better than the periodic ones, both in terms of filter bandwidth and transmittance peak, and are less sensitive to variations in the defect thickness.
A solution is also provided for the energetics of the relaxation of misfit strain in a linear isotropic elastic half-space by means of twin-like defects in which the defect thickness is allowed to vary continuously, allowing for the determination of effective average twin thicknesses and spacings which themselves vary continuously during the relaxation process.
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Imperfections due to the manufacturing process are taken into account including material imperfections (elastic modulus variability) and geometrical defects (thickness variability).
Table 1 Description of the five different treatment groups and the empty chondral- and osteochondral control groups Treatment Type n Details Empty full-thickness chondral defect Full thickness chondral 3 Ø 6 mm full thickness chondral defect left untreated.
Also, simultaneous enhancement of the transmission magnitude and Faraday rotation of the structure can be obtained by optimizing the optical contrast ratio-magnetic defect layer thickness product.
The graphene defects and thickness of 2-10 layers can be controlled by variation in the argon flow rate and pressure during graphene growth step.
The type, intensity of the structural defects, and thickness of the electrodeposited e-RGO layers were studied by collecting the Raman spectrum (as illustrated in Fig. 4b).
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