Download Almost periodic solutions of differential equations in by Yoshiyuki Hino, Toshiki Naito, Nguyen VanMinh, Jong Son Shin PDF

By Yoshiyuki Hino, Toshiki Naito, Nguyen VanMinh, Jong Son Shin

This monograph offers contemporary advancements in spectral stipulations for the life of periodic and nearly periodic recommendations of inhomogenous equations in Banach areas. a number of the effects characterize major advances during this sector. specifically, the authors systematically current a brand new strategy in keeping with the so-called evolution semigroups with an unique decomposition method. The ebook additionally extends classical thoughts, comparable to fastened issues and balance tools, to summary practical differential equations with functions to partial practical differential equations. virtually Periodic suggestions of Differential Equations in Banach areas will entice someone operating in mathematical research.

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Extra info for Almost periodic solutions of differential equations in Banach spaces

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We shall denote by A M the op­ erator f E M � AfO with D( AM ) = {! E M I Vt E R, f (t) E D(A) , Af(·) E M } . When M = B UC(R, X ) we shall use the notation A : = AM . Throughout the paragraph we always assume that A is a given operator on X with p(A) :I 0 , ( so it is closed) . In this paragraph we will use the notion of translation-invariance of a function space, which we recall in the following definition, and additional conditions on it. e. , S(r)M e M for all r E R , is said to satisfy i) condition H1 if the following condition is fulfilled: VC E L(X) , Vf E M :::} Cf E M , ii) condition H2 if the following condition is fulfilled: For every closed linear operator A, if f E M such that f(t) E D (A) , Vt, Af E B UC(R, X) , then A f E M , iii) condition H3 if the following condition is fulfilled: For every bounded linear operator B E L(BUC(R, X)) which commutes with the translation group (S( t ) ) t E R one has B M C M .

We now show that 1 E pCP) . For every x E X put f(t) = U(t, O)g(t)x for t E [ 0, 1] ' where get) is any continuous function of t such that g(O) = g( l ) = 0, and 1 1 g(t)dt = 1. Thus f (t) can be continued to a I-periodic function on the real line which we denote also by f (t) for short. Put Sx = [L -1 ( - 1 )] (0) . Obviously, S is a bounded operator. We have [£ - 1 ( - 1 )] (1) = U ( 1 , O) [£ - l ( _ 1 ) ) (O) + Sx = PSx + Px. 1 1 U ( l, �) U(�, O)g( �)xd� Thus (1 - P) (Sx + x) = Px + x - Px = x.

To this end, we show that u(T1 Ip( » \ {0} C o-(P) \{O} . To see this, 1 we note that A T 1 Ip( l ) = Pp( l ) . p(T1 Ip( 1 » . By Example 2 . 4 1 E also true. Conversely, we suppose that Eq. 4) is uniquely solvable in P ( l ) . We now show that 1 E pCP) . For every x E X put f(t) = U(t, O)g(t)x for t E [ 0, 1] ' where get) is any continuous function of t such that g(O) = g( l ) = 0, and 1 1 g(t)dt = 1. Thus f (t) can be continued to a I-periodic function on the real line which we denote also by f (t) for short.

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