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The physical mechanisms of the grating can be shown clearly by using the simplified modal method with consideration of the corresponding accumulated average phase difference of two excited propagating grating modes, which illustrates that the grating structure depends mainly on the ratio of the average effective indices difference to the incident wavelength.
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In the locations of capitals towards the eastern and southern EMME the second mode dominates, which illustrates the long duration of the warm season (Fig. 7).
At the same time, the distributed locations of eigenvalue corresponding to normal mode and different fault modes are non-coincident which illustrates that these different eigenvalues can be discriminated by a clustering algorithm.
Which illustrates a more general point.
Which illustrates the difference between being great and being wearable.
Which illustrates the bigger issue.
Failure mode maps are constructed which illustrate the dominant failure mode for practical beam designs.
To further support the proposed binding mode, potent conjugates are described which illustrate the potential for development of chemical probes to enable further target evaluation.
Furthermore, the wavelengths of the first, second, third, and fourth modes of GNR (a = 30 nm) versus AR (4 to 8) for n = 1.25 are plotted in Figure 6, which illustrate that these modes are red-shifted as the AR of GNR increases.
Failure mechanism maps which illustrate the dominant initial failure mode for practical beam designs were constructed for different test temperatures based on the modified Gibson model.
In this paper we present the Monte Carlo ray-tracing simulations, the results of which illustrate the performance of the instrument in the inelastic-scattering mode.
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