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Figure 6 shows that the reflection coefficient is larger for the case of larger wave propagation angle.
Figure 1a shows that the reflection peaks of (100), (002), and (101) correspond to hexagonal ZnO with a wurtzite structure, but a preferred orientation along the (002) plane is intense.
Comprehensive analysis considering Figs. 2, 3, and 4 shows that the reflection heights of both characteristic waves increase and the distance between them decreases with decreasing latitude (the black circles in Figs. 3a, c and 4a, c above).
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On the other hand, Fig. 3a, b shows that the reflections remained the same, corresponding to the 0002 and ( 10overline{1}3 ) peaks, for the GZO films with different thicknesses prepared by IP with dc arc discharge.
The results show that the reflection loss could be reduced owing to the lower reflectivity of this structure.
It is shown that the reflection at the corners is correctly eliminated.
Simulations show that the reflection coefficient for the ridge gap waveguide is below −15 dB between 240 and 340 GHz.
The analytical investigations show that the reflection characteristics of a slotted seawall depend mainly on the porosity of the slotted plate and the incident wave height.
Well-posedness is investigated and it is shown that the reflection properties of the second-order equation are superior to those of the first-order equation.
The results show that the reflection coefficient and the chemomechanical coupling parameter are correlated with each other and with both the Cation Exchange Capacity (CEC) and the Specific Surface Area (SSA).
We show that the reflection coefficient is exponentially small with respect to the damping parameter and the width of the PML and this independently of the advection and of the viscosity.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com