"We are playing the role of the state" remarks Seida.
As stated in Remark 3.1, not every ordering covers completely.
Of course, if f is -concave, the above inequality is reversed, as stated in Remark 4.
For example, Theorem 1 stated in Remark 17 was obtained in [22].
As stated in Remark 1.2, the proof of our result is largely based on the Fourier localized methods.
However, as stated in Remark 3.1, our model has potential applications in robust stabilization of linear systems with nonlinear perturbation and chaotic control and synchronization.
In fact, as stated in Remark 5.1, there is a deep relationship between Artinian Gorenstein algebras for and tube hypersurfaces locally CR-equivalent to Levi non-degenerate hyperquadrics.
However, as stated in Remark 3, using a suitably large I (e.g., I=106 in this scenario) amplifies the effect of the virtual power queue sizes in (15a) and prevents continuous use of the peak powers.
Note that, as we stated in Remark 3, when U c is scaled with T c, it impacts the D2D coverage probability, but the decrease in the performance of D2D users is not significant.
We formulate an even more improved version of the Loéve-Young inequality in Remark 2. The inequality formulated in Remark 2, together with relation (18), yields (4), and this, together with (5), yields (3), but reasoning in opposite direction (derivation of (4) or inequality stated in Remark 2 from (3)) seems to be not possible.
