on, then has proper orbits [15, 19]; consequently, we obtain the following generalization of the corresponding result of Kirk [20].
then, consequently, we obtain for the instantaneous capacity in underlay approach C U (resp. interweave approach C I ) C^{U} = max_{1,..,N}{C_{k}^{U}} = varepsilon log_{2}left(1+frac{P}{N_{0}}W^{U}right) (15).
and, consequently, we obtain ( p − 1 ) ξ ( t 1 ) + X p ( t 1 ) p + Y q ( t 1 ) q = 0. We consider T, α as sufficiently large numbers for which (4.4) and (4.5) are satisfied.
Hence, the computation imposes the relation ( Γ ( 1 + m β ) Γ ( 1 + m β − β ) + 4 m ) μ m + 1 2 μ m − 1 = 0. with μ ( 0 ) = 1, and consequently we obtain μ m : = ( B m ) m Γ ( 1 + m β ), where B m in terms of a gamma function.
Consequently, we obtain (5.42).
Consequently, we obtain on.
Consequently, we obtain that (3.11).
Consequently, we obtain for (3.14).
Consequently, we obtain that for all.
Consequently, we obtain the following theorem.
Consequently, we obtain that (2.2). which contradicts.
