Exact(4)
Suppose that (phi_{i}inmathcal{B}_{v}) ((i=1,2)) are arbitrary functions and that (y_{1}), (y_{2}) are the corresponding mild solutions of the problem (1.1 - 1.2 1.1 - 1.2
In view of Theorem 3.1, for each (uin U_{ad}), and (yin C [0,c],X)) is the corresponding mild solution of system (1.1), one has biglVert y(t bigrVert leq Vert y_{0}Vert +N+MVert eta Vert _{L^{1}([0,c])}+M int_{0}^{t} eta (tau biglVert y tau bigrVert,mathrm{d}tau +MM_{B}tilde{M}c.
It turns out that the sequence ({v_{n}}) defined by the IMR v_{n+1}=alpha_{n} f v_{n})+ 1- alpha_{n}) T biggl(frac{v_{n}+v_{n+1}}{2} biggr) (4.9) with ({alpha_{n}}) satisfying the conditions (C1 - C3) of Theorem 3.1, converges weakly to a fixed point v of T, and then the corresponding mild solution u of (4.7) with initial value (u(0)=xi) is a periodic solution of (4.7).
As a matter of fact, if v and (v_{1}) are two elements of B, (u(t)) and (u_{1}(t)) are the corresponding mild solutions, we have begin{aligned} frac{1}{2}{dt}bigl{t}bigl| bigl| u(t -u_{1}(t -u_{r| ^{2}bigr} =&-operatorname{Re}bigllangle A(t) bigl(u(t)-u_{1}(t)bigr), u(t)-u_{1}(t)bigrrangle &+operatorname{Re}bigllangle fbigl(t,u(t)bigr)-fbigl(t,u_{1}(t) bigr), u(t)-u_{1}(t)bigrrangle le&0.
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