Exact(8)
In this paper, we improve the concept of (C^{m} -almost periodiC^{m} -almostdic time scales.
Thus, by the definition and the property of (S_{tau_{t}}), we can obtain the local almost periodicity on the periodic sub-timescale (mathbb{T}_{tau_{t}}) from Definition 3.1 (see Figure 5).
Figure 5 The local-almost periodicity of the function f occurs on the periodic sub-timescale (pmb{mathbb{T}_{2}}) through ε -local translation number (pmb{tau_{0}}), but the function f is without almost periodicity on the periodic sub-timescale (pmb{mathbb{T}_{1}}). Now we give another definition which in view of Theorem 2.21 is equivalent to Definition 3.1.
From these one-dimensional and two-dimensional analyses, the influence of the finite-length periodicity on the wave transmission characteristics is discussed.
These layers form a c(2x2) periodicity on the Pt (100) substrate.
The latter is well known and relatively cheap method that allows to form a planar periodicity on large areas.
The second modification to the structure was carried out by imposing a partial periodicity on the structure.
Figure 6 Dependence of grating periodicity on the angle of incidence of laser beam measured from surface normal.
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