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To check the light confinement therein, we calculated the Q-factor using the formula Q = λ/∆λ, where λ and ∆λ denote the mode position and the full width at half maximum (FWHM) of the mode, respectively[16], and the results are plotted in Figure 2b.
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The CNT films Raman G mode positions and widths exhibit two apparent regimes, a nonlinear temperature dependence at low temperatures (<270 K), which is explained by the phenomenon of optical phonon decay, and a linear temperature dependence above 270 K.
Figure 2 Evolution of mode positions and Q -factors with increasing coating layers.
To test the possible effects of other factors, dependencies of the c-BN transversal optical mode position on film thickness and c-BN content were investigated.
The first component has a center value close to the G mode position of pristine graphite and is assigned to block of not intercalated graphite layers, while the 1600 cm −1 mode is assigned to graphene layers next to an intercalant layer.
The thickness of grating and homogeneous absentee layers can significantly change the linewidth and resonant mode position in absorption spectrum.
The agreement between the theory and experiment is reasonable as far as the mode position is concerned.
Species with a mode position ≤ 0.69 form the cluster 3 (mean CpGo/e position is 0.45).
All the species have a CpGo/e mode position mode above 0.69 (the mean CpGo/e peak position is 1.00), a weak negative skewness (meanabsolute Q50 skewness = −0.0019) and a narrow standard deviation (meanSD = Da0.11).
As in the cluster 1, species present in the second cluster have a mode position > 0.69 with a mean mode position very close to the first cluster (mean CpGo/e position is 0.92) and a mean absolute Q50 skewness of 0.0012.
In this paper a sliding mode position control for high-performance real-time applications of induction motors is developed.
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