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HAL Id: hal-00258396https://hal.archives-ouvertes.fr/hal-00258396
Preprint submitted on 22 Feb 2008
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Center manifold and stability in critical cases for somepartial functional differential equations
Mostafa Adimy, Khalil Ezzinbi, Jianhong Wu
To cite this version:Mostafa Adimy, Khalil Ezzinbi, Jianhong Wu. Center manifold and stability in critical cases for somepartial functional differential equations. 2006. hal-00258396
Center manifold and stability in critical cases forsome partial functional differential equations 1.
Mostafa ADIMY ā, Khalil EZZINBI ā and Jianhong WU ā”
ā Universite de Pau et des Pays de lāAdourLaboratoire de Mathematiques Appliquees CNRS UMR 5142
Avenue de lāuniversite 64000Pau, France
ā Universite Cadi AyyadFaculte des Sciences Semlalia
Departement de Mathematiques, B.P. 2390Marrakesh, Morocco
ā” York UniversityDepartment of Mathematics and Statistics
Faculty of Pure and Applied Sciences4700 Keele Street North York, Ontario, Canada, M3J 1P3
Abstract. In this work, we prove the existence of a center manifold for some partialfunctional differential equations, whose linear part is not necessarily densely defined butsatisfies the Hille-Yosida condition. The attractiveness of the center manifold is alsoshown when the unstable space is reduced to zero. We prove that the flow on the centermanifold is completely determined by an ordinary differential equation in a finite dimen-sional space. In some critical cases, when the exponential stability is not possible, weprove that the uniform asymptotic stability of the equilibrium is completely determinedby the uniform asymptotic stability of the reduced system on the center manifold.Keys words: Hille-Yosida operator, integral solution, semigroup, variation of constantsformula, center manifold, attractiveness, reduced system, critical case, asymptotic stabil-ity, approximation.2000 Mathematical Subject Classification: 34K17, 34K19, 34K20, 34K30, 34G20,47D06.
1This research is supported by Grant from CNCPRST (Morocco) and CNRS(France) Ref. SPM17769, by TWAS Grant under contract Ref. 03-030 RG/MATHS/AF/AC, by the Canada ResearchChairs Program, by Natural Sciences and Engineering Research Council of Canada, and by Mathematicsfor Information Technology and Complex Systems.
ā[email protected]: to whom all correspondence should be sentā [email protected]ā” [email protected] appear in International Journal of Evolution Equations
1
2
1. Introduction
The aim of this paper is to study the existence of a center manifold and stability insome critical cases for the following partial functional differential equation
(1.1)
d
dtu(t) = Au(t) + L(ut) + g(ut), t ā„ 0
u0 = Ļ ā C := C ([ār, 0] ; E) ,
where A is not necessarily densely defined linear operator on a Banach space E and C
is the space of continuous functions from [ār, 0] to E endowed with the uniform normtopology. For every t ā„ 0 and for a continuous u : [ār, +ā) āā E, the function ut ā C
is defined byut(Īø) = u(t + Īø) for Īø ā [ār, 0] .
L is a bounded linear operator from C into E and g is a Lipschitz continuous functionfrom C to E with g(0) = 0.
In this work, we assume that A is a Hille-Yosida operator: there exist Ļ ā lR andM0 ā„ 1 such that (Ļ,ā) ā Ļ(A) and
ā£ā£(Ī»I ā A)ānā£ā£ ā¤ M0
(Ī» ā Ļ)nfor Ī» ā„ Ļ and n ā N,
where Ļ(A) is the resolvent set of A. In [21], the authors proved the existence, regularityand stability of solutions of (1.1) when A generates a strongly continuous semigroup, which
is equivalent by Hille-Yosida Theorem to that A is a Hille-Yosida operator and D(A) =E. In [3], the authors used the integrated semigroup approach to prove the existence andregularity of solutions of (1.1) when A is only a Hille-Yosida operator. Moreover, it wasshown that the phase space of equation (1.1) is given by
Y :=
Ļ ā C : Ļ(0) ā D(A)
.
Assume that the function g is differentiable at 0 with gā²(0) = 0. Then the linearizedequation of (1.1) around the equilibrium zero is given by
(1.2)
d
dtv(t) = Av(t) + L(vt), t ā„ 0
v0 = Ļ ā C.
If all characteristic values (see section 2) of equation (1.2) have negative real part, thenthe zero equilibrium of (1.1) is uniformly asymptotically stable. However, if there existsat least one characteristic value with a positive real part, then the zero solution of (1.1) isunstable. In the critical case, when exponential stability is not possible and there existsa characteristic value with zero real part, the situation is more complicated since eitherstability or instability may hold. The subject of the center manifold is to study the sta-bility in this critical case. For differential equations, the center manifold theory has beenextensively studied, we refer to [6], [7], [8], [12], [13], [14], [15], [16], [19], [20] and [24].
In [17] and [22], the authors proved the existence of a center manifold when D(A) = E.They established the attractiveness of this manifold when the unstable space is reduced tozero. In [11], the authors proved the existence of a center manifold for a given map. Theirapproach was applied to show the existence of a center manifold for partial functional dif-ferential equations in Banach spaces in the case when the linear part generates a compactstrongly continuous semigroup. Recently, in [18], the authors studied the existence of
3
invariant manifolds for an evolutionary process in Banach spaces and in particularly forsome partial functional differential equations. For more details about the center manifoldtheory and its applications in the context of partial functional differential equations, werefer to the monograph [27]. Here we consider equation (1.1) when the domain D(A) isnot necessarily dense in E. The nondensity occurs, in many situations, from restrictionsmade on the space where the equations are considered (for example, periodic continuoussolutions, H"older continuous functions) or from boundary conditions ( the spaceC1 with null value on the boundary is not dense in the space of continuous functions).For more details, we refer to [1], [2], [3], [4] and [5].
The organization of this work is as follows: in section 2, we recall some results of integralsolutions and the semigroup solution and we describe the variation of constants formulafor the associated non-homogeneous problem of (1.2). We also give some results on thespectral analysis of the linear equation (1.2). In section 3, we prove the existence of aglobal center manifold. In section 4, we prove that this center manifold is exponentiallyattractive when the unstable space is reduced to zero. In section 5, we prove that theflow on the center manifold is governed by an ordinary differential equation in a finitedimensional space. In section 6, we prove a result on the stability of the equilibrium in thecritical case. We also establish a new reduction principal for equation (1.1). In section 7,we study the existence of a local center manifold when g is only defined and C1-functionin a neighborhood of zero. In the last section, we propose a result on the stability whenzero is a simple characteristic value and no characteristic value lies on the imaginary axis.
2. Spectral analysis and variation of constants formula
In the following we assume
(H1) A is a Hille-Yosida operator.
Definition 2.1. A continuous function u : [ār, +ā) ā E is called an integral solutionof equation (1.1) if
i)
ā« t
0
u(s)ds ā D(A) for t ā„ 0,
ii) u(t) = Ļ(0) + A
(ā« t
0
u(s)ds
)+ L
(ā« t
0
usds
)+
ā« t
0
g(us)ds for t ā„ 0,
iii) u0 = Ļ.
We will call, without causing any confusion, the integral solution the function ut, fort ā„ 0.
Let A0 be the part of the operator A in D(A) which is defined by
D(A0) =
x ā D(A) : Ax ā D(A)
A0x = Ax for x ā D(A0).
The following result is well known (see [3]).
Lemma 2.2. A0 generates a strongly continuous semigroup (T0(t))tā„0 on D(A).
For the existence and uniqueness of an integral solution of (1.1), we need the followingcondition.
(H2) g : C āā E is Lipschitz continuous.
4
The following result can be found in [3].
Proposition 2.3. Assume that (H1) and (H2) hold. Then for Ļ ā Y, equation (1.1) hasa unique global integral solution on [ār,ā) which is given by the following formula
(2.1) u(t) =
T0(t)Ļ(0) + limĪ»āā
ā« t
0
T0(t ā s)BĪ» (L(us) + g(us)) ds, t ā„ 0
Ļ(t), t ā [ār, 0] ,
where BĪ» = Ī»(Ī»I ā A)ā1 for Ī» ā„ Ļ.
Assume that g is differentiable at zero with gā²(0) = 0. Then the linearized equation of(1.1) at zero is given by equation (1.2). Define the operator U(t) on Y by
U(t)Ļ = vt(., Ļ),
where v is the unique integral solution of equation (1.2) corresponding to the initial valueĻ. Then (U(t))tā„0 is a strongly continuous semigroup on Y . One has the followinglinearized principle.
Theorem 2.4. Assume that (H1) and (H2) hold. If the zero equilibrium of (U(t))tā„0 isexponentially stable, in the sense that there exist N0 ā„ 1 and Ē« ā„ 0 such that
|U(t)| ā¤ N0eāĒ«t for t ā„ 0,
then the zero equilibrium of equation (1.1) is locally exponentially stable, in the sense thatthere exist Ī“ ā„ 0, Āµ ā„ 0 and k ā„ 1 such that
|xt(., Ļ)| ā¤ keāĀµt |Ļ| for Ļ ā Y with |Ļ| ā¤ Ī“ and t ā„ 0,
where xt(., Ļ) is the integral solution of equation (1.1) corresponding to initial value Ļ.Moreover, if Y can be decomposed as Y = Y1 ā Y2 where Yi are U-invariant subspaces of
Y , Y1 is a finite-dimensional space and with Ļ0 = limhāā
1
hlog |U(h)|Y2| we have
inf |Ī»| : Ī» ā Ļ (U(t)|Y1) ā„ eĻ0t for t ā„ 0,
where Ļ (U(t)|Y1) is the spectrum of U(t)|Y1, then the zero equilibrium of equation (1.1)is unstable, in the sense that there exist Īµ ā„ 0 and sequences (Ļn)n converging to 0 and(tn)n of positive real numbers such that |xtn(., Ļn)| ā„ Īµ.
The above theorem is a consequence of the following result. For more details on theproof, we refer to [3].
Theorem 2.5. [9] Let (V (t))tā„0 be a nonlinear strongly continuous semigroup on a sub-set Ī© of a Banach space Z and assume that x0 ā Ī© is an equilibrium of (V (t))tā„0 suchthat V (t) is differentiable at x0, with W (t) the derivative at x0 of V (t) for each t ā„ 0.Then, (W (t))tā„0 is a strongly continuous semigroup of bounded linear operators on Z.
If the zero equilibrium of (W (t))tā„0 is exponentially stable, then x0 is locally exponen-tially stable equilibrium of (V (t))tā„0. Moreover, if Z can be decomposed as Z = Z1 ā Z2
where Zi are W -invariant subspaces of Z, Z1 is a finite-dimensional space and with
Ļ1 = limhāā
1
hlog |W (h)|Z2| we have
inf |Ī»| : Ī» ā Ļ (W (t)|Z1) ā„ eĻ1t for t ā„ 0,
then the equilibrium x0 is unstable in the sense that there exist Īµ ā„ 0 and sequences (yn)n
converging to x0 and (tn)n of positive real numbers such that |V (tn)yn ā x0| ā„ Īµ.
5
Some informations of the infinitesimal generator of (U(t))tā„0 can be found in [5]. Forexample, we know that
Theorem 2.6. The infinitesimal generator AU of (U(t))tā„0 on Y is given by
D(AU) =
Ļ ā C1 ([ār, 0] ; E) : Ļ(0) ā D(A), Ļā²(0) ā D(A) andĻā²(0) = AĻ(0) + L(Ļ)
AUĻ = Ļā² for Ļ ā D(AU).
We now make the next assumption about the operator A.
(H3) The semigroup (T0(t))tā„0 is compact on D(A) for t ā„ 0.
Theorem 2.7. Assume that (H3) holds. Then, U(t) is a compact operator on Y fort ā„ r.
Proof. Let t ā„ r and D be a bounded subset of Y . We use Ascoli-Arzelaās theorem to
show that
U(t)Ļ : Ļ ā D
is relatively compact in Y . Let Ļ ā D, Īø ā [ār, 0] and Īµ ā„ 0
such that t + Īø ā Īµ ā„ 0. Then
(U(t)Ļ) (Īø) = T0(t + Īø)Ļ(0) + limĪ»ā+ā
ā« t+Īø
0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds.
Note that
ā« t+Īø
0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds
=
ā« t+ĪøāĪµ
0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds +
ā« t+Īø
t+ĪøāĪµ
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds
and
limĪ»ā+ā
ā« t+ĪøāĪµ
0
T0(t+Īøās)BĪ»L(U(s)Ļ)ds = T0(Īµ) limĪ»ā+ā
ā« t+ĪøāĪµ
0
T0(t+ĪøāĪµās)BĪ»L(U(s)Ļ)ds.
The assumption (H3) implies that
T0(Īµ)
lim
Ī»ā+ā
ā« t+ĪøāĪµ
0
T0(t + Īø ā Īµ ā s)BĪ»L(U(s)Ļ)ds : Ļ ā D
is relatively compact in E. As the semigroup (U(t))tā„0 is exponentially bounded, thenthere exists a positive constant b1 such that
ā£ā£ā£ā£ limĪ»ā+ā
ā« t+Īø
t+ĪøāĪµ
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds
ā£ā£ā£ā£ ā¤ b1Īµ for Ļ ā D.
Consequently, the set
limĪ»ā+ā
ā« t+Īø
t+ĪøāĪµ
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds : Ļ ā D
is totally bounded in E. We deduce that
(U(t)Ļ) (Īø) : Ļ ā D
is relatively compact in E,
for each Īø ā [ār, 0]. For the completeness of the proof, we need to show the equicontinuityproperty. Let Īø, Īø0 ā [ār, 0] such that Īø ā„ Īø0. Then
6
(U(t)Ļ) (Īø) ā (U(t)Ļ) (Īø0) = (T0(t + Īø) ā T0(t + Īø0)) Ļ(0)
+ limĪ»ā+ā
ā« t+Īø
0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds
ā limĪ»ā+ā
ā« t+Īø0
0
T0(t + Īø0 ā s)BĪ»L(U(s)Ļ)ds.
Furthermore,ā« t+Īø
0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds =
ā« t+Īø0
0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds
+
ā« t+Īø
t+Īø0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds.
Consequently,
|(U(t)Ļ) (Īø) ā (U(t)Ļ) (Īø0)| ā¤ |T0(t + Īø) ā T0(t + Īø0)| |Ļ(0)|
+
ā£ā£ā£ā£ limĪ»ā+ā
ā« t+Īø0
0
(T0(t + Īø ā s) ā T0(t + Īø0 ā s)) BĪ»L(U(s)Ļ)ds
ā£ā£ā£ā£
+
ā£ā£ā£ā£ limĪ»ā+ā
ā« t+Īø
t+Īø0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds
ā£ā£ā£ā£ .
Assumption (H3) implies that the semigroup (T0(t))tā„0 is uniformly continuous for t ā„ 0.Then
limĪøāĪø0
|T0(t + Īø) ā T0(t + Īø0)| = 0.
The semigroup (U(t))tā„0 is exponentially bounded. Consequently, there exists a positiveconstant b2 such that
ā£ā£ā£ā£ limĪ»ā+ā
ā« t+Īø
t+Īø0
T0(t + Īø ā s)BĪ»L(U(s)Ļ)ds
ā£ā£ā£ā£ ā¤ b2 (Īø ā Īø0)
and
limĪ»ā+ā
ā« t+Īø0
0
(T0(t + Īø ā s) ā T0(t + Īø0 ā s)) BĪ»L(U(s)Ļ)ds
= (T0(Īø ā Īø0) ā I) limĪ»ā+ā
ā« t+Īø0
0
T0(t + Īø0 ā s)BĪ»L(U(s)Ļ)ds.
We have proved that there exists a compact set K0 in E such that
limĪ»ā+ā
ā« t+Īø0
0
T0(t + Īø0 ā s)BĪ»L(U(s)Ļ)ds ā K0 for Ļ ā D.
Using Banach-Steinhausās theorem, we obtain
limĪøāĪø0
(T0(Īø ā Īø0) ā I)x = 0 uniformly in x ā K0.
This implies that
limĪøāĪø+
0
(U(t)Ļ) (Īø) ā (U(t)Ļ) (Īø0) = 0 uniformly in Ļ ā D.
7
We can prove in similar way that
limĪøāĪøā
0
(U(t)Ļ) (Īø) ā (U(t)Ļ) (Īø0) = 0 uniformly in Ļ ā D.
By Ascoli-Arzelaās theorem, we conclude that
U(t)Ļ : Ļ ā D
is compact for t ā„ r.
Now, we consider the spectral properties of the infinitesimal generator AU . We denoteby E, without causing confusion, the complexication of E. For each complex number Ī»,
we define the linear operator ā(Ī») : D(A) ā E by
(2.2) ā(Ī») = Ī»I ā A ā L(eĪ»Ā·I),
where eĪ»Ā·I : E ā C is defined by(eĪ»Ā·x
)(Īø) = eĪ»Īøx, x ā E and Īø ā [ār, 0] .
Definition 2.8. We say that Ī» is a characteristic value of equation (1.2) if there existsx ā D(A)\0 solving the characteristic equation ā(Ī»)x = 0.
Since the operator U(t) is compact for t ā„ r, the spectrum Ļ(AU) of AU is the pointspectrum Ļp(AU). More precisely, we have
Theorem 2.9. The spectrum Ļ(AU) = Ļp(AU) = Ī» ā C : ker ā(Ī») 6= 0 .
Proof. Let Ī» ā Ļp(AU). Then there exists Ļ ā D(AU)\0 such that AUĻ = Ī»Ļ, whichis equivalent to
Ļ(Īø) = eĪ»ĪøĻ(0), for Īø ā [ār, 0] and Ļā²(0) = AĻ(0) ā L(Ļ) with Ļ(0) 6= 0.
Consequently ā(Ī»)Ļ(0) = 0. Conversely, let Ī» ā C such that ker ā(Ī») 6= 0 . Then thereexists x ā D(A)\0 such that ā(Ī»)x = 0. If we define the function Ļ by
Ļ(Īø) = eĪ»Īøx for Īø ā [ār, 0] ,
then Ļ ā D(AU) and AUĻ = Ī»Ļ, which implies that Ī» ā Ļp(AU).The growth bound Ļ0(U) of the semigroup (U(t))tā„0 is defined by
Ļ0(U) = inf
Īŗ ā„ 0 : sup
tā„0eāĪŗt |U(t)| < ā
.
The spectral bound s(AU) of AU is defined by
s(AU) = sup Re(Ī») : Ī» ā Ļp(AU) .
Since U(t) is compact for t ā„ r, then it is well known that Ļ0(U) = s(AU). Consequently,the asymptotic behavior of the solutions of the linear equation (1.2) is completely obtainedby s(AU). More precisely, we have the following result.
Corollary 2.10. Assume that (H1), (H2) and (H3) hold. Then, the following propertieshold,i) if s(AU) < 0, then (U(t))tā„0 is exponentially stable and zero is locally exponentiallystable for equation (1.1);ii) if s(AU) = 0, then there exists Ļ ā Y such that |U(t)Ļ| = |Ļ| for t ā„ 0 and eitherstability or instability may hold;iii) if s(AU) ā„ 0, then there exists Ļ ā Y such that |U(t)Ļ| ā ā as t ā ā and zero isunstable for equation (1.1).
8
As a consequence of the compactness of the semigroup U(t) for t ā„ r and by Theorem2.11, p.100, in [10], we get the following general spectral decomposition of the phase spaceY .
Theorem 2.11. There exist linear subspaces of Y denoted by Yā, Y0 and Y+ respectivelywith
Y = Yā ā Y0 ā Y+
such thati) AU(Yā) ā Yā, AU(Y0) ā Y0, and AU(Y+) ā Y+;ii) Y0 and Y+ are finite dimensional;iii) Ļ(AU |Y0) = Ī» ā Ļ(AU) : Re Ī» = 0 , Ļ(AU |Y+) = Ī» ā Ļ(AU) : Re Ī» ā„ 0;iv) U(t)Yā ā Yā for t ā„ 0, U(t) can be extended for t ā¤ 0 when restricted to Y0 āŖY+ andU(t)Y0 ā Y0, U(t)Y+ ā Y+ for t ā lR;v) for any 0 < Ī³ < inf |Re Ī»| : Ī» ā Ļ(AU) and Re Ī» 6= 0 , there exists K ā„ 0 such that
|U(t)PāĻ| ā¤ KeāĪ³t |PāĻ| for t ā„ 0,|U(t)P0Ļ| ā¤ Ke
Ī³
3|t| |P0Ļ| for t ā lR,
|U(t)P+Ļ| ā¤ KeĪ³t |P+Ļ| for t ā¤ 0,
where Pā, P0 and P+ are projections of Y into Yā, Y0 and Y+ respectively.Yā, Y0 and Y+ are called stable, center and unstable subspaces of the semigroup (U(t))tā„0 .
The following result deals with the variation of constants formula for equation (1.1)which are taken from [5]. Let ćX0ć be defined by
ćX0ć = X0c : c ā E ,
where the function X0c is defined by
(X0c) (Īø) =
0 if Īø ā [ār, 0) ,
c if Īø = 0.
We introduce the space Y ā ćX0ć , endowed with the following norm
|Ļ + X0c| = |Ļ| + |c| .
The following result is taken from [5].
Theorem 2.12. The continuous extension AU of the operator AU defined on Y ā ćX0ćby:
D(AU) =
Ļ ā C1 ([ār, 0] ; E) : Ļ(0) ā D(A) and Ļā²(0) ā D(A)
AUĻ = Ļā² + X0(AĻ(0) + L(Ļ) ā Ļā²(0)),
is a Hille-Yosida operator on Y āćX0ć: there exist Ļ ā lR and M0 ā„ 1 such that (Ļ,ā) ā
Ļ(AU) andā£ā£ā£(Ī»I ā AU)ān
ā£ā£ā£ ā¤ M0
(Ī» ā Ļ)nfor Ī» ā„ Ļ and n ā N,
with Ļ(AU) the resolvent set of AU .Moreover, the integral solution u of equation (1.1) is given for Ļ ā Y, by the followingvariation of constants formula
(2.3) ut = U(t)Ļ + limĪ»āā
ā« t
0
U(t ā s)BĪ» (X0g(us)) ds for t ā„ 0,
9
where BĪ» = Ī»(Ī»I ā AU)ā1 for Ī» ā„ Ļ.
Remarks. i) Without loss of generality, we assume that M0 = 1. Otherwise, we can
renorm the space Y ā ćX0ć in order to get an equivalent norm for which M0 = 1.ii) For any locally integrable function : lR ā E, one can see that the following limitexists:
limĪ»āā
ā« t
s
U(t ā Ļ)BĪ»X0(Ļ)dĻ for t ā„ s.
3. Global existence of the center manifold
Theorem 3.1. Assume that (H1) and (H3) hold. Then, there exists Īµ ā„ 0 such that if
Lip(g) = supĻ1 6=Ļ2
|g(Ļ1) ā g(Ļ2)|
|Ļ1 ā Ļ2|< Īµ,
then, there exists a bounded Lipschitz map hg : Y0 ā YāāY+ such that hg(0) = 0 and theLipschitz manifold
Mg := Ļ + hg(Ļ) : Ļ ā Y0
is globally invariant under the flow of equation (1.1) on Y .
Proof. Let B = B(Y0, Yā ā Y+) denote the Banach space of bounded maps h : Y0 āYā ā Y+ endowed with the uniform norm topology. We define
F = h ā B : h is Lipschitz, h(0) = 0 and Lip(h) ā¤ 1 .
Let h ā F and Ļ ā Y0. Using the strict contraction principle, one can prove the existenceof v
Ļt solution of the following equation
(3.1) vĻt = U(t)Ļ + lim
Ī»āā
ā« t
0
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + h(vĻĻ ))
)0
dĻ, t ā lR.
We now introduce the mapping Tg : F ā B by
Tg(h)Ļ = limĪ»āā
ā« 0
āā
U(āĻ)(BĪ»X0g(vĻ
Ļ + h(vĻĻ ))
)ā
dĻ
+ limĪ»āā
ā« 0
+ā
U(āĻ)(BĪ»X0g(vĻ
Ļ + h(vĻĻ ))
)+
dĻ.
The first step is to prove that Tg maps F into itself. Let Ļ1, Ļ2 ā Y0 and t ā lR. Supposethat Lip(g) < Īµ. Then
|vĻ1
t ā vĻ2
t | ā¤ KeĪ³
3|t| |Ļ1 ā Ļ2| + 2K |P0| Īµ
ā£ā£ā£ā£ā« t
0
eĪ³
3|tāĻ | |vĻ1
Ļ ā vĻ2
Ļ | dĻ
ā£ā£ā£ā£ .
By Gronwallās lemma, we get that
eāĪ³
3|t| |vĻ1
t ā vĻ2
t | ā¤ K |Ļ1 ā Ļ2| e2K|P0|Īµ|t|
and|vĻ1
t ā vĻ2
t | ā¤ K |Ļ1 ā Ļ2| e[ Ī³
3+2K|P0|Īµ]|t| for t ā lR.
If we choose Īµ such that
(3.2) 2K |P0| Īµ <Ī³
6,
10
then
(3.3) |vĻ1
t ā vĻ2
t | ā¤ K |Ļ1 ā Ļ2| eĪ³
2|t| for t ā lR.
Moreover,
|Tg(h)Ļ1 ā Tg(h)Ļ2| ā¤
ā« 0
āā
|U(āĻ)Pā| |g(vĻ1
Ļ + h(vĻ1
Ļ )) ā g(vĻ2
Ļ + h(vĻ2
Ļ ))| dĻ
+
ā« +ā
0
|U(āĻ)P+| |g(vĻ1
Ļ + h(vĻ1
Ļ )) ā g(vĻ2
Ļ + h(vĻ2
Ļ ))| dĻ.
Consequently,
|Tg(h)Ļ1 ā Tg(h)Ļ2| ā¤ 2
ā« 0
āā
KeĪ³Ļ |Pā| Īµ |vĻ1
Ļ ā vĻ2
Ļ | dĻ+2
ā« +ā
0
KeāĪ³Ļ |P+| Īµ |vĻ1
Ļ ā vĻ2
Ļ | dĻ.
Using inequality (3.3), we obtain
|Tg(h)Ļ1 ā Tg(h)Ļ2| ā¤ 2K2 |Pā| Īµ |Ļ1 ā Ļ2|
ā« 0
āā
eĪ³
2ĻdĻ+2K2 |P+| Īµ |Ļ1 ā Ļ2|
ā« +ā
0
eāĪ³
2ĻdĻ.
It follows that
|Tg(h)Ļ1 ā Tg(h)Ļ2| ā¤4Īµ
Ī³K2 (|Pā| + |P+|) |Ļ1 ā Ļ2| .
If we choose Īµ such that4Īµ
Ī³K2 (|Pā| + |P+|) < 1,
then Tg maps F into itself.The next step is to show that Tg is a strict contraction on F . Let h1, h2 ā F . For Ļ ā Y0
and for i = 1, 2, let vit denote the solution of the following equation
vit = U(t)Ļ + lim
Ī»āā
ā« t
0
U(t ā Ļ)(BĪ»X0g(vi
Ļ + hi(viĻ ))
)0
dĻ for t ā lR.
Then,
ā£ā£v1t ā v2
t
ā£ā£ ā¤ ĪµK |P0|
ā£ā£ā£ā£ā« t
0
eĪ³
3|tāĻ |
(ā£ā£v1Ļ ā v2
Ļ
ā£ā£ +ā£ā£h1(v
1Ļ ) ā h1(v
2Ļ )
ā£ā£ +ā£ā£h1(v
2Ļ ) ā h2(v
2Ļ )
ā£ā£) dĻ
ā£ā£ā£ā£ ,
and
ā£ā£v1t ā v2
t
ā£ā£ ā¤ 2ĪµK |P0|
ā£ā£ā£ā£ā« t
0
eĪ³
3|tāĻ |
ā£ā£v1Ļ ā v2
Ļ
ā£ā£ dĻ
ā£ā£ā£ā£ + ĪµK |P0| |h1 ā h2|
ā£ā£ā£ā£ā« t
0
eĪ³
3|tāĻ |dĻ
ā£ā£ā£ā£ .
By Gronwallās lemma, we obtain that
ā£ā£v1t ā v2
t
ā£ā£ ā¤ 3ĪµK
Ī³|P0| |h1 ā h2| e
[ Ī³
3+2K|P0|Īµ]|t| for t ā lR.
By (3.2), we obtain
ā£ā£v1t ā v2
t
ā£ā£ ā¤ 3ĪµK
Ī³|P0| |h1 ā h2| e
Ī³
2|t| for all t ā lR.
11
For i = 1, 2, we have
Tg(hi)Ļ = limĪ»āā
ā« 0
āā
U(āĻ)(BĪ»X0g(vi
Ļ + hi(viĻ ))
)ā
dĻ
+ limĪ»āā
ā« 0
+ā
U(āĻ)(BĪ»X0g(vi
Ļ + hi(viĻ ))
)+
dĻ.
It follows that
|Tg(h1)Ļ ā Tg(h2)Ļ| ā¤ 2K |Pā|6Īµ2K
Ī³2|P0| |h1 ā h2| +
K |Pā| Īµ
Ī³|h1 ā h2|
+ 2K |P+|6Īµ2K
Ī³2|P0| |h1 ā h2| +
K |P+| Īµ
Ī³|h1 ā h2| .
Consequently,
|Tg(h1) ā Tg(h2)| ā¤ (|Pā| + |P+|)KĪµ
Ī³
[|P0|
12ĪµK
Ī³+ 1
]|h1 ā h2| .
We choose Īµ such that
(|Pā| + |P+|)KĪµ
Ī³
[|P0|
12ĪµK
Ī³+ 1
]< 1.
Then Tg is a strict contraction on F , and consequently it has a unique fixed point hg inF : Tg(hg) = hg.Finally, we show that
Mg := Ļ + hg(Ļ) : Ļ ā Y0
is globally invariant under the flow on Y . Let Ļ ā Y0 and v be the solution of equation(3.1). We claim that t ā v
Ļt + hg(v
Ļt ) is an integral solution of equation (1.1) with initial
value Ļ + hg(Ļ). In fact, we have Tg(hg)(vĻt ) = hg(v
Ļt ), t ā lR. Moreover, for t ā lR, one
has
Tg(h)(vĻt ) = lim
Ī»āā
ā« 0
āā
U(āĻ)(BĪ»X0g(vĻ
t+Ļ + hg(vĻt+Ļ ))
)ā
dĻ
+ limĪ»āā
ā« 0
+ā
U(āĻ)(BĪ»X0g(vĻ
t+Ļ + hg(vĻt+Ļ ))
)+
dĻ,
which implies that
hg(vĻt ) = lim
Ī»āā
ā« t
āā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ
+ limĪ»āā
ā« t
+ā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ.
12
Then, for t ā lR, we have
vĻt + hg(v
Ļt ) = U(t)Ļ + lim
Ī»āā
ā« t
0
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)0
dĻ
+ limĪ»āā
ā« t
āā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ
+ limĪ»āā
ā« t
+ā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ.
For any t ā„ a, we have
limĪ»āā
ā« t
āā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ
= limĪ»āā
ā« a
āā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ
+ limĪ»āā
ā« t
a
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ,
and
limĪ»āā
ā« a
āā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ
= U(t ā a)
(lim
Ī»āā
ā« a
āā
U(a ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ
).
By the same argument as above, we obtain
limĪ»āā
ā« t
+ā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ
= limĪ»āā
ā« a
+ā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ
+ limĪ»āā
ā« t
a
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ,
and
limĪ»āā
ā« a
+ā
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ
= U(t ā a)
(lim
Ī»āā
ā« a
+ā
U(a ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ
).
Note that
hg(vĻa ) = lim
Ī»āā
ā« a
+ā
U(a ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ
+ limĪ»āā
ā« a
āā
U(a ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ,
and in particular
vĻt = U(t ā a)vĻ
a + limĪ»āā
ā« t
a
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)0
dĻ.
13
Consequently, for any t ā„ a, we obtain
vĻt + hg(v
Ļt ) = U(t ā a) (vĻ
a + hg(vĻa )) + lim
Ī»āā
ā« t
a
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)0
dĻ
+ limĪ»āā
ā« t
a
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)+
dĻ
+ limĪ»āā
ā« t
a
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)ā
dĻ,
which implies that for any t ā„ a,
vĻt + hg(v
Ļt ) = U(t ā a) (vĻ
a + hg(vĻa )) + lim
Ī»āā
ā« t
a
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)dĻ.
Finally, we conclude that vĻt
+ hg(vĻt) is an integral solution of equation (1.1) on lR with
initial value Ļ + hg(Ļ).
Theorem 3.2. Let vĻ be the solution of equation (3.1) on lR. Then, for t ā lR
|vĻt | ā¤ K |Ļ| e
Ī³
2|t| and |vĻ
t + hg(vĻt )| ā¤ 2K |Ļ| e
Ī³
2|t|.
Conversely, if we choose Īµ such that
2KĪµ
Ī³(|Pā| + |P+| + 3 |P0|) < 1,
then for any integral solution u of equation (1.1) on lR with ut = O(eĪ³
2|t|), we have ut ā Mg
for all t ā lR.
Proof. Let vĻ be the solution of equation (3.1). Then, using the estimate (3.3), we obtainthat
|vĻt | ā¤ K |Ļ| e
Ī³
2|t| for t ā lR
and from the fact that Lip(h) ā¤ 1 and hg(0) = 0, we obtain
|vĻt + hg(v
Ļt )| ā¤ 2K |Ļ| e
Ī³
2|t| for t ā lR.
Let u be an integral solution of equation (1.1) such that ut = O(eĪ³
2|t|). Then there exists
a positive constant k0 such that |ut| ā¤ k0eĪ³
2|t| for all t ā lR. Note that
ut = U(t ā s)us + limĪ»āā
ā« t
s
U(t ā Ļ)BĪ»X0g(uĻ )dĻ for t ā„ s.
On the other hand,
u+t = U(t ā s)u+
s + limĪ»āā
ā« t
s
U(t ā Ļ)(BĪ»X0g(uĻ )
)+
dĻ for s ā„ t.
Moreover, for s ā„ t and s ā„ 0, we haveā£ā£U(t ā s)u+
s
ā£ā£ ā¤ KeĪ³(tās) |P+us| ā¤ k0K |P+| eĪ³(tās)e
Ī³
2|s| = k0K |P+| e
Ī³teāĪ³
2s.
Therefore,limsāā
ā£ā£U(t ā s)u+s
ā£ā£ = 0.
It follows that
u+t = lim
Ī»āā
ā« t
+ā
U(t ā Ļ)(BĪ»X0g(uĻ )
)+
dĻ.
14
Similarly, we can prove that
uāt = lim
Ī»āā
ā« t
āā
U(t ā Ļ)(BĪ»X0g(uĻ )
)ā
dĻ.
We conclude that
ut = u+t + uā
t + U(t)u00 + lim
Ī»āā
ā« t
0
U(t ā Ļ)(BĪ»X0g(uĻ )
)0
dĻ for t ā lR.
Let Ļ ā Y0 such that Ļ = u0. By Theorem 3.1, there exists an integral solution w ofequation (1.1) on lR with initial value Ļ + hg(Ļ) such that wt ā Mg for all t ā lR and
wt = U(t)Ļ + limĪ»āā
ā« t
0
U(t ā Ļ)(BĪ»X0g(wĻ )
)0
dĻ
+ limĪ»āā
ā« t
āā
U(t ā Ļ)(BĪ»X0g(wĻ )
)+
dĻ
+ limĪ»āā
ā« t
+ā
U(t ā Ļ)(BĪ»X0g(wĻ )
)ā
dĻ.
Then, for all t ā lR, we have
|ut ā wt| ā¤
ā£ā£ā£ā£ limĪ»āā
ā« t
0
U(t ā Ļ)(BĪ»X0 (g(uĻ ) ā g(wĻ ))
)0
dĻ
ā£ā£ā£ā£
+
ā£ā£ā£ā£ limĪ»āā
ā« t
āā
U(t ā Ļ)(BĪ»X0 (g(uĻ ) ā g(wĻ ))
)+
dĻ
ā£ā£ā£ā£
+
ā£ā£ā£ā£ limĪ»āā
ā« t
+ā
U(t ā Ļ)(BĪ»X0 (g(uĻ ) ā g(wĻ ))
)ā
dĻ
ā£ā£ā£ā£ .
This implies that
|ut ā wt| ā¤ KĪµ
(|P0|
ā£ā£ā£ā£ā« t
0
eĪ³
3|tāĻ | |uĻ ā wĻ | dĻ
ā£ā£ā£ā£
+ |Pā|
ā« t
āā
eāĪ³(tāĻ) |uĻ ā wĻ | dĻ + |P+|
ā« ā
t
eĪ³(tāĻ) |uĻ ā wĻ | dĻ
).
Let N(t) = eāĪ³
2|t| |ut ā wt| for all t ā lR. Then, N = sup
tālRN(t) < ā. On the other hand,
we have
N(t) ā¤ KĪµN
(|P0|
ā£ā£ā£ā£ā« t
0
eāĪ³
6|tāĻ |dĻ
ā£ā£ā£ā£ + |Pā|
ā« t
āā
eāĪ³
2(tāĻ)dĻ + |P+|
ā« ā
t
eĪ³
2(tāĻ)dĻ
).
Finally we arrive at
N ā¤2KĪµ
Ī³(3 |P0| + |Pā| + |P+|) N .
Consequently, N = 0 and ut = wt for t ā lR.
15
4. Attractiveness of the center manifold
In this section, we assume that there exists no characteristic value with a positive realpart and hence the unstable space Y+ is reduced to zero. We establish the following resulton the attractiveness of the center manifold.
Theorem 4.1. There exist Īµ ā„ 0, K1 ā„ 0 and Ī± ā(
Ī³
3, Ī³
)such that if Lip(g) < Īµ, then
any integral solution ut(Ļ) of equation (1.1) on R+ satisfies
(4.1)ā£ā£uā
t (Ļ) ā hg(u0t (Ļ))
ā£ā£ ā¤ K1eāĪ±t
ā£ā£Ļā ā hg(Ļ0)
ā£ā£ for t ā„ 0.
Proof. The proof of this theorem is based on the following technically lemma.
Lemma 4.2. There exist Īµ ā„ 0, K0 ā„ 0 and Ī± ā(
Ī³
3, Ī³
)such that if Lip(g) < Īµ, then
there is a continuous bounded mapping p : lR+ Ć Y0 Ć Yā ā Yā such that any integralsolution ut(Ļ) of equation (1.1) satisfies
(4.2) uāt (Ļ) = p(t, u0
t (Ļ), Ļā) for t ā„ 0.
Moreover,
(4.3) |p(t, Ļ1, Ļ1) ā p(t, Ļ2, Ļ2)| ā¤ K0
(|Ļ1 ā Ļ2| + eāĪ±t |Ļ1 ā Ļ2|
)
for all Ļ1, Ļ2 ā Y0, Ļ1, Ļ2 ā Yā and t ā„ 0.
Idea of the proof of Lemma 4.2. The proof is similar to the one given in [22]. LetĻ ā Y0 and Ļ ā Yā. For t ā„ 0 and 0 ā¤ Ļ ā¤ t, we consider the system
q(Ļ, t, Ļ, Ļ) = U(Ļāt)Ļā limĪ»āā
ā« t
Ļ
U(Ļās)(BĪ»X0g (q(s, t, Ļ, Ļ) + p(s, q(s, t, Ļ, Ļ), Ļ))
)0
ds,
and
p(t, Ļ, Ļ) = U(t)Ļ + limĪ»āā
ā« t
0
U(t ā s)(BĪ»X0g(q(s, t, Ļ, Ļ) + p(s, q(s, t, Ļ, Ļ), Ļ))
)ā
ds.
Using the contraction principle, we can prove the existence of q and p. The expression(4.2) and the estimate (4.3) are obtained in a completely similar fashion to that in [22].
Proof of Theorem 4.1. Let Mg be the center manifold of equation (1.1). Then anyintegral solution lying in Mg must satisfy (4.2). Let ut = ut(Ļ
ā+Ļ0) be an integral solutionof equation (1.1) on R
+ with initial value Ļā + Ļ0. Let Ļ ā„ 0. Then, u0Ļ + hg(u
0Ļ ) ā Mg
and the corresponding integral solution exists on R and lies on Mg. This solution canbe considered as an integral solution of equation (1.1) starting from Ļā + Ļ0 at 0. Letvt = vt(Ļ
ā + Ļ0) be the integral solution corresponding to Ļā + Ļ0. Using Lemma 4.2,we conclude that
uāĻ ā hg(u
0Ļ ) = p(Ļ, u0
Ļ , Ļā) ā p(Ļ, u0
Ļ , Ļā),
which implies that
(4.4)ā£ā£uā
Ļ ā hg(u0Ļ )
ā£ā£ ā¤ K0eāĪ±Ļ
ā£ā£Ļā ā Ļāā£ā£ .
Since Lip(h) ā¤ 1, we haveā£ā£uā
Ļ ā hg(u0Ļ )
ā£ā£ ā¤ K0eāĪ±Ļ
(ā£ā£Ļā ā hg(Ļ0)
ā£ā£ +ā£ā£Ļ0 ā Ļ0
ā£ā£) .
16
The initial values Ļ0 and Ļ0 correspond to the solutions of the following equations for0 ā¤ s ā¤ Ļ
vs = U(s ā Ļ)vĻ + limĪ»āā
ā« s
Ļ
U(s ā Ļ)(BĪ»X0g(vĻ + p(Ļ, vĻ, Ļ
ā)))0
dĻ,
vās = U(s ā Ļ)vā
Ļ + limĪ»āā
ā« s
Ļ
U(s ā Ļ)(BĪ»X0g(vā
Ļ + p(Ļ, vāĻ, Ļ
ā)))0
dĻ.
Note that vĻ = vāĻ . It follows, for 0 ā¤ s ā¤ Ļ , that
|vs ā vās | ā¤ K(1+K0)Īµ |P0|
ā« Ļ
s
eĪ³
3(Ļās) |vĻ ā vā
Ļ| dĻ+KK0Īµ |P0|
ā« Ļ
s
eĪ³
3(Ļās)eāĪ±ĻdĻ
ā£ā£Ļā ā Ļāā£ā£ .
Then by Gronwallās lemma, we deduce that there exists a positive constant Ī½ whichdepends only on constants Ī³, K, K0 and Īµ such that, for 0 ā¤ s ā¤ Ļ , we have
|vs ā vās | ā¤ Ī½
ā£ā£Ļā ā Ļāā£ā£ .
If we assume that Lip(g) is small enough such that Ī½ < 1, thenā£ā£Ļ0 ā Ļ0
ā£ā£ ā¤ Ī½ā£ā£Ļā ā Ļā
ā£ā£ ā¤ Ī½(ā£ā£Ļā ā hg(Ļ
0)ā£ā£ +
ā£ā£hg(Ļ0) ā hg(Ļ
0)ā£ā£) ,
which gives thatā£ā£Ļ0 ā Ļ0
ā£ā£ ā¤ Ī½
1 ā Ī½
ā£ā£Ļā ā hg(Ļ0)
ā£ā£ .
We conclude that
ā£ā£uāt ā hg(u
0t )
ā£ā£ ā¤ 1
1 ā Ī½K0e
āĪ±tā£ā£Ļā ā hg(Ļ
0)ā£ā£ for t ā„ 0.
As an immediate consequence, we obtain the following result on the attractiveness of thecenter manifold.
Corollary 4.3. Assume that Lip(g) is small enough and the unstable space Y+ is reducedto zero. Then the center manifold Mg is exponentially attractive.
We also obtain.
Proposition 4.4. Assume that Lip(g) is small enough and the unstable space Y+ isreduced to zero. Let w be an integral solution of equation (1.1) that is bounded on R.Then wt ā Mg for all t ā R.
Proof. Let w be a bounded integral solution of equation (1.1). Since, the equation (1.1)is autonomous, then for Ļ ā¤ 0, wtā²+Ļ is also an integral solution of equation (1.1) fortā² ā„ 0 with initial value wĻ at 0. It follows by the estimation (4.1) that
ā£ā£wātā²+Ļ(Ļ) ā hg(w
0tā²+Ļ(Ļ))
ā£ā£ ā¤ K1eāĪ±tā²
ā£ā£wāĻ ā hg(w
0Ļ)
ā£ā£ for tā² ā„ 0.
Let t ā„ Ļ. Then
(4.5)ā£ā£wā
t ā hg(w0t )
ā£ā£ ā¤ K1eāĪ±(tāĻ)
ā£ā£wāĻ ā hg(w
0Ļ)
ā£ā£ for t ā„ Ļ.
Since w is bounded on R, letting Ļ ā āā, we obtain that wāt = hg(w
0t ) for all t ā R.
17
5. Flow on the center manifold
In this section, we establish that the flow on the center manifold is governed by anordinary differential equation in a finite dimensional space. In the sequel, we assumethat the function g satisfies the conditions of Theorem 4.1. We also assume that theunstable space Y+ is reduced to zero. Let d be the dimension of the center space Y0 andĪ¦ = (Ļ1, ...., Ļd) be a basis of Y0. Then there exists d-elements Ī¦ = (Ļā
1, ...., Ļād) in Y ā, the
dual space of Y, such that
ćĻāi , Ļjć := Ļā
i (Ļj) = Ī“ij, 1 ā¤ i, j ā¤ d,
and Ļāi = 0 on Yā. Denote by ĪØ the transpose of (Ļā
1, ...., Ļād). Then the projection
operator P0 is given by
P0Ļ = Ī¦ ćĪØ, Ļć .
Since (U0(t))tā„0 is a strongly continuous group on the finite dimensional space Y0, byTheorem 2.15, p. 102 in [10], we get that there exists a d Ć d matrix G such that
U0(t)Ī¦ = Ī¦eGt for t ā„ 0.
Let n ā N, n ā„ n0 ā„ Ļ and i ā 1, ...., d . We define the function xāni on E by
xāni(y) =
āØĻā
i , Bn (X0y)ā©
.
Then xāni is a bounded linear operator on E. Let xā
n be the transpose of (xān1, ..., x
ānd), then
ćxān, yć =
āØĪØ, Bn (X0y)
ā©.
Consequently,
supnā„n0
|xān| < ā,
which implies that (xān)nā„n0
is a bounded sequence in L(E, Rd). Then, we get the followingimportant result.
Theorem 5.1. There exists xā ā L(E, Rd) such that (xān)nā„n0
converges weakly to xā inthe sense that
ćxān, yć ā ćxā, yć as n ā ā for y ā E.
For the proof, we need the following fundamental theorem [25, pp. 776]
Theorem 5.2. Let X be a separable Banach space and (zān)nā„0 be a bounded sequence in
Xā. Then there exists a subsequence(zānk
)kā„0
of (zān)nā„0 which converges weakly in Xā in
the sense that there exists zā ā Xā such thatāØzānk
, yā©ā ćzā, yć as k ā ā for x ā X.
Proof of Theorem 5.1. Let Z0 be a closed separable subspace of E. Since (xān)nā„n0
is
a bounded sequence, by Theorem 5.2 there is a subsequence(xā
nk
)kāN
which converges
weakly to some xāZ0
in Z0. We claim that all the sequence (xān)nā„n0
converges weakly toxā
Z0in Z0. This can be done by way of contradiction. Namely, suppose that there exists
18
a subsequence(xā
np
)pāN
of (xān)nā„n0
which converges weakly to some xāZ0
with xāZ0
6= xāZ0
.
Let ut(., Ļ, Ļ, f) denote the integral solution of the following equation
d
dtu(t) = Au(t) + L(ut) + f(t), t ā„ Ļ
uĻ = Ļ ā C,
where f is a continuous function from R to E. Then by using the variation of constantsformula and the spectral decomposition of solutions, we obtain
P0ut(., Ļ, 0, f) = limnā+ā
ā« t
Ļ
U (t ā Ī¾)(BnX0f(Ī¾)
)0
dĪ¾,
and
P0
(BnX0f(Ī¾)
)= Ī¦
āØĪØ, BnX0f(Ī¾)
ā©= Ī¦ ćxā
n, f(Ī¾)ć .
It follows that
P0ut(., Ļ, 0, f) = limnā+ā
Ī¦
ā« t
Ļ
e(tāĪ¾)GāØĪØ, BnX0f(Ī¾)
ā©dĪ¾,
= limnā+ā
Ī¦
ā« t
Ļ
e(tāĪ¾)G ćxān, f(Ī¾)ć dĪ¾.
For a fixed a ā Z0, set f = a to be a constant function. Then
limkā+ā
ā« t
Ļ
e(tāĪ¾)GāØxā
nk, a
ā©dĪ¾ = lim
pā+ā
ā« t
Ļ
e(tāĪ¾)GāØxā
np, a
ā©dĪ¾ for a ā Z0,
which implies thatā« t
Ļ
e(tāĪ¾)GāØxā
Z0, a
ā©dĪ¾ =
ā« t
Ļ
e(tāĪ¾)GāØxā
Z0, a
ā©dĪ¾ for a ā Z0.
Consequently xāZ0
= xāZ0
, which yields a contradiction.We now conclude that the whole sequence (xā
n)nā„n0converges weakly to xā
Z0in Z0. Let
Z1 be another closed separable subspace of X. By using the same argument as above, weobtain that (xā
n)nā„n0converges weakly to xā
Z1in Z1. Since Z0 ā© Z1 is a closed separable
subspace of E, we get that xāZ1
= xāZ0
in Z0 ā© Z1. For any y ā E, we define xā by
ćxā, yć = ćxāZ , yć ,
where Z is an arbitrary given closed separable subspace of E such that y ā Z. Then xā
is well defined on E and xā is a bounded linear operator from E to Rd such that
|xā| ā¤ supnā„n0
|xān| < ā,
and (xān)nā„n0
converges weakly to xā in E.
As a consequence, we conclude that
Corollary 5.3. For any continuous function f : R ā E, we have
limnā+ā
ā« t
Ļ
U (t ā Ī¾)(BnX0f(Ī¾)
)0
dĪ¾ = Ī¦
ā« t
Ļ
e(tāĪ¾)G ćxā, f(Ī¾)ć dĪ¾ for t, Ļ ā R.
19
Let Ļ ā Y0 such that Ļ + hg(Ļ) ā Mg. From the properties of the center manifold, weknow that the integral solution starting from Ļ + h(Ļ) is given by v
Ļt + hg(v
Ļt ), where v
Ļt
is the solution of
vĻt = U(t)Ļ + lim
Ī»āā
ā« t
0
U(t ā Ļ)(BĪ»X0g(vĻ
Ļ + hg(vĻĻ ))
)0
dĻ for t ā lR.
Let z(t) be the component of vĻt . Then Ī¦z(t) = v
Ļt for t ā lR. By Theorem 5.1 and
Corollary 5.3, we have
Ī¦z(t) = vĻt = Ī¦eGtz(0) + Ī¦
ā« t
0
e(tāĻ)G ćxā, g(vĻĻ + hg(v
ĻĻ ))ć dĻ for t ā lR.
We conclude that z satisfies
z(t) = eGtz(0) + limnāā
ā« t
0
eG(tāĻ) ćxān, g(vĻ
Ļ + hg(vĻĻ ))ć dĻ for t ā lR.
Finally we arrive at the following ordinary differential equation, which determines theflow on the center manifold
(5.1) zā²(t) = Gz(t) + ćxā, g(Ī¦z(t) + hg(Ī¦z(t)))ć for t ā lR.
6. Stability in critical cases
In this section, we suppose that Lip(g) < Īµ, where Īµ is given by Theorem 4.1. Here westudy the critical case where the unstable space Y+ is reduced to zero and the exponentialstability is not possible, which implies that there exists at least one characteristic valuewith a real part equals zero.
Theorem 6.1. Assume that Lip(g) is small enough. Then there exists a positive constantK2 such that for each Ļ ā Y, there exists z0 ā R
d such that
(6.1)ā£ā£u0
t ā Ī¦z(t)ā£ā£ +
ā£ā£uāt ā hg(Ī¦z(t))
ā£ā£ ā¤ K2eāĪ±t
ā£ā£Ļā ā hg(Ļ0)
ā£ā£ for t ā„ 0,
where z is the solution of the reduced system (5.1) with initial value z0 and u is the integralsolution of equation (1.1) with initial value Ļ.
Proof. Let Ļ ā Y and u be the corresponding integral solution of equation (1.1). Then
u0s = U(s ā t)u0
t + limĪ»āā
ā« s
t
U(s ā Ļ)(BĪ»X0g(uā
Ļ + u0Ļ )
)0
dĻ for 0 ā¤ s ā¤ t.
Also let s ā ws,t be the solution of the following equation
ws,t = U(s ā t)u0t + lim
Ī»āā
ā« s
t
U(s ā Ļ)(BĪ»X0g(wĻ,t + hg(wĻ,t))
)0
dĻ for 0 ā¤ s ā¤ t.
Then, for 0 ā¤ s ā¤ t, we have
ā£ā£u0s ā ws,t
ā£ā£ ā¤ 2KĪµ |P0|
ā« t
s
eĪ³
3(Ļās)
ā£ā£u0Ļ ā wĻ,t
ā£ā£ dĻ + KĪµ |P0|
ā« t
s
eĪ³
3(Ļās)
ā£ā£uāĻ ā hg(u
0Ļ )
ā£ā£ dĻ.
It follows that
eĪ³
3sā£ā£u0
s ā ws,t
ā£ā£ ā¤ 2KĪµ |P0|
ā« t
s
eĪ³
3Ļā£ā£u0
Ļ ā wĻ,t
ā£ā£ dĻ + KĪµ |P0|
ā« t
s
eĪ³
3Ļā£ā£uā
Ļ ā hg(u0Ļ )
ā£ā£ dĻ.
20
Using Gronwallās lemma, we obtain that
ā£ā£u0s ā ws,t
ā£ā£ ā¤ 2KĪµ |P0|
ā« t
s
eĀµ(Ļās)ā£ā£uā
Ļ ā hg(u0Ļ )
ā£ā£ dĻ for 0 ā¤ s ā¤ t,
where Āµ = 2KĪµ |P0| +Ī³
3. By Theorem 4.1, we obtain
ā£ā£u0s ā ws,t
ā£ā£ ā¤(
2KK1Īµ |P0|
ā« t
s
e(ĀµāĪ±)(Ļās)dĻ
) ā£ā£uās ā hg(u
0s)
ā£ā£ for 0 ā¤ s ā¤ t.
Let us recall that Ī± ā(
Ī³
3, Ī³
). Then we can choose Īµ small enough such that Āµ ā Ī± < 0.
Consequently,
(6.2)ā£ā£u0
s ā ws,t
ā£ā£ ā¤ 2KK1Īµ |P0|
Ī± ā Āµ
ā£ā£uās ā hg(u
0s)
ā£ā£ for 0 ā¤ s ā¤ t,
and for s = 0, we have
ā£ā£u00 ā w0,t
ā£ā£ ā¤ 2KK1Īµ |P0|
Ī± ā Āµ
ā£ā£uā0 ā hg(u
00)
ā£ā£ for t ā„ 0.
We deduce that w0,t : t ā„ 0 is bounded in Y0 and then there exists a sequence tn ā āas n ā ā and Ļ ā Y0 such that
w0,tn ā Ļ as n ā ā.
Let w(., Ļ) be the solution of the following equation
wt(., Ļ) = U(t)Ļ + limĪ»āā
ā« t
0
U(t ā Ļ)(BĪ»X0g(wĻ (., Ļ) + hg(wĻ (., Ļ)))
)0
dĻ for t ā„ 0.
By the continuous dependence on the initial data, we obtain, for all s ā„ 0
ws(0, Ļ) = limnāā
ws(0, w0,tn) = limnāā
ws(0, wātn(0, utn)),
= limnāā
wsātn(0, utn) = limnāā
ws,tn .
By (4.4) and (6.2), there exists a positive constant K2 such thatā£ā£u0
s ā ws(0, Ļ)ā£ā£ ā¤ K2e
āĪ±sā£ā£uā
0 ā hg(u00)
ā£ā£ for all s ā„ 0.
If we put
Ī¦z(t) = wt(0, Ļ) for t ā lR,
then
z(t) = eGtz(0) +
ā« t
0
e(tāĻ)G ćxā, g(Ī¦z(Ļ) + hg(Ī¦z(Ļ)))ć dĻ for t ā lR.
Finally, the estimation (6.1) follows from (4.4).
Now, we can state the following result on the stability by using the reduction to thecenter manifold.
Theorem 6.2. If the zero solution of equation (5.1) is uniformly asymptotically stable(unstable), then the zero solution of equation (1.1) is uniformly asymptotically stable(unstable).
21
Proof. Assume that 0 is uniformly asymptotically stable for equation (5.1). For Ļ ā„ 0,let
BĻ =Ļā + Ļ0 ā Yā ā Y0 :
ā£ā£Ļāā£ā£ +
ā£ā£Ļ0ā£ā£ < Ļ
,
and Mg ā© BĻ for some Ļ ā„ 0, be the region of attraction of 0 for equation (5.1). First,we prove that 0 is stable for equation (1.1). Let Īµ ā„ 0. Then there exists Ī“ < Ļ suchthat |z(t)| < Īµ for t ā„ 0, provided that |z(0)| < Ī“, where z is a solution of (5.1). As 0 isassumed to be uniformly asymptotically stable for equation (5.1), there exists t0 = t0(Ī“)such that |z(t)| < Ī“
2, for t ā„ t0. Without loss of generality, we can choose Ī“ and t0 so that
max(K1, K2)eāĪ±t0 < 1
2.
By the continuous dependence on the initial value for equation (1.1), there exists Ī“1 < Ī“2
such that if
Ļā + Ļ0 ā VĪ“1 :=
Ļā + Ļ0 ā Yā ā Y0 :
ā£ā£Ļ0ā£ā£ <
Ī“1
2,
ā£ā£Ļā ā hg(Ļ0)
ā£ā£ <Ī“1
2
,
then the corresponding integral solution ut = ut(Ļā + Ļ0) of equation (1.1) satisfies
ut ā BĪµ for t ā [0, t0] .
Moreover,ā£ā£uā
t0ā hg(u
0t0)ā£ā£ <
Ī“1
2.
Furthermore, by Theorem 6.1, there exists z0 ā Rd such that
(6.3)ā£ā£u0
t ā Ī¦z(t)ā£ā£ ā¤ K2e
āĪ±tā£ā£Ļā ā hg(Ļ
0)ā£ā£ for t ā„ 0,
where z is a solution of the reduced system (5.1) with initial value z0 such that |z0| < Ī“.It follows that ā£ā£u0
t0
ā£ā£ < Ī“.
Consequently, ut0 ā BĪµ and ut must be in BĪµ for all t ā„ 0. This completes the proof ofthe stability.
Now we deal with the local attractiveness of the zero solution. For a given integralsolution u(., Ļ) of equation (1.1) which is assumed to be bounded for t ā„ 0, it is wellknown that the Ļ-limit set Ļ(Ļ) is nonempty, compact, invariant and connected since themap Ļ ā ut(Ā·, Ļ) is compact for t ā„ r.
For the attractiveness of 0, let VĪ“ be chosen as above and Ļ ā VĪ“. Then the integralsolution u of equation (1.1) starting from Ļ lies in BĪµ. The Ļ-limit set Ļ(Ļ) of u isnonempty and invariant and must be in Mg ā© BĪµ. Since the equilibrium 0 of (1.1) is uni-formly asymptotically stable, we deduce by Theorem 11.4, p. 111 [23] and by the LaSalleinvariance principle that the only invariant set in Mg ā© BĪµ must be zero. Consequently,the Ļ-limit set Ļ(Ļ) is zero and
ut(., Ļ) ā 0 as t ā 0.
Assume now that the zero solution of the reduced system (5.1) is unstable. Then thereexist Ļ1 ā„ 0, a sequence (tn)n of positive real numbers and a sequence (zn)n convergingto 0 such that |z(tn, zn)| ā„ Ļ1, where z(., zn) is a solution of (5.1). On the other handĪ¦z(., zn) + hg(Ī¦z(., zn)) is an integral solution of equation (1.1) and
|Ī¦z(tn, zn) + hg(Ī¦z(tn, zn))| ā„ (1 ā Lip(hg)) |Ī¦z(tn, zn)| .
22
Moreover, Lip(hg) can be chosen such that 1 ā Lip(hg) ā„ 0. It follows that
|Ī¦z(tn, zn) + hg(Ī¦z(tn, zn))| ā„ (1 ā Lip(hg)) Ļ2,
for some Ļ2 ā„ 0. Consequently, the zero solution of equation (1.1) is unstable.
7. Local existence of the center manifold
In this section we prove the existence of the local center manifold when g is only definedin a neighborhood of zero. We assume that
(H4) There exists Ļ1 ā„ 0 such that g : B(0, Ļ1) ā E is C1-function, g(0) = 0 andgā²(0) = 0, where B(0, Ļ1) = Ļ ā C : |Ļ| < Ļ1 .
For Ļ < Ļ1, we define the cut-off function gĻ : C ā E by
gĻ(Ļ) =
g(Ļ) if |Ļ| ā¤ Ļ,
g( Ļ
|Ļ|Ļ) if |Ļ| ā„ Ļ.
We consider the following partial functional differential equation
(7.1)
d
dtu(t) = Au(t) + L(ut) + gĻ(ut) for t ā„ 0
u0 = Ļ ā C.
Theorem 7.1. Assume that (H1), (H3) and (H4) hold. Then there exist 0 < Ļ < Ļ1
and Lipschitz continuous mapping hgĻ: Y0 ā Yā ā Y+ such that hgĻ
(0) = 0 and the localLipschitz manifold
MgĻ=
Ļ + hgĻ
(Ļ) : Ļ ā Y0
is globally invariant under the flow associated to equation (7.1).
Proof. Using the same arguments as in [26], Proposition 3.10, p.95, one can show thatgĻ is Lipschitz continuous with
Lip(gĻ) ā¤ 2 sup|Ļ|<Ļ
|gā²(Ļ)| .
It follows that Lip(gĻ) goes to zero when Ļ goes to zero. According to Theorem 3.1, wededuce that there exist Ļ ā„ 0 and mapping hgĻ
: Y0 ā Yā ā Y+ with hgĻ(0) = 0 such that
the Lipschitz manifoldMgĻ
=Ļ + hgĻ
(Ļ) : Ļ ā Y0
is globally invariant under the flow of equation (7.1).
Definition 7.2. The local center manifold associated to equation (1.1) is defined by
MgĻ=
Ļ + hgĻ
(Ļ) : Ļ ā Y0
ā© B(0, Ļ).
We deduce that the local center manifold contains all bounded integral solutions ofequation (1.1) which are bounded by Ļ. Moreover, the following interesting results hold.
Theorem 7.3. (Attractiveness). Assume that (H1), (H3), (H4) hold and the unstablespace Y+ is reduced to zero. Then there exist 0 < Ļ < Ļ1, K3 ā„ 0 and Ī± ā
(Ī³
3, Ī³
)such
that any integral solution ut(Ļ) of equation (1.1) with initial data Ļ ā B(0, Ļ1), exists onR
+ and satisfies
(7.2)ā£ā£uā
t (Ļ) ā hgĻ(u0
t (Ļ))ā£ā£ ā¤ K3e
āĪ±tā£ā£Ļā ā hgĻ
(Ļ0)ā£ā£ for t ā„ 0.
23
Theorem 7.4. (Reduction principle and stability). Assume that (H1), (H3), (H4)hold and the unstable space Y+ is reduced to zero. If the zero solution of equation (5.1)is uniformly asymptotically stable (unstable), then the zero solution of equation (1.1) isuniformly asymptotically stable (unstable).
8. Application
In this section, we assume that
(H5) Ļ(AU) ā© Ī» ā C : Re(Ī») ā„ 0 = 0 and 0 is a simple eigenvalue of AU .
In this case, the reduced system (5.1) on the center manifold becomes
zā²(t) = Ļ (z(t)),
where Ļ is the scalar function given by
Ļ (z) =āØxā, g(Ī¦z + hgĻ
(Ī¦z))ā©
for z ā R.
Theorem 8.1. Assume that (H1), (H3), (H4), (H5) hold and Ļ satisfies
(8.1) Ļ (z) = amzm + am+1zm+1 + ....
If m is odd and am < 0, then the zero solution of equation (1.1) is uniformly asymptoticallystable. If am > 0 then the zero solution of equation (1.1) is unstable.
Proof. The proof is based on Theorem 6.2 and on the following known stability result.
Theorem 8.2. [6] Consider the scalar differential equation
(8.2) zā²(t) = amzm + am+1zm+1 + ....
If m is odd and am < 0, then the zero solution of equation (8.2) is uniformly asymptoticallystable. If am > 0, then the zero solution of equation (8.2) is unstable.
Concluding remark. Assumption (8.1) is natural and it is a consequence of the smooth-ness of the center manifold, which states that if g is a Ck-function, for k ā„ 1, then hgĻ
is also a Ck-function. Consequently if g is a Cā-function, then the center manifold hgĻ
is also a Cā-function. Assumption (8.1) can be obtained by using the approximation ofthe center manifold hgĻ
. The proof of the smoothness result is omitted here and it can bedone in similar way as in [11].
Acknowledgements: A part of this work has been done when the second author wasvisiting the Abdus Salam International Centre for Theoretical Physics, ICTP, Trieste-Italy. He would like to acknowledge the centre for the support.
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