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METHODS FOR DETERMINATION AND APPROXIMATION OF THE DOMAIN OF ATTRACTION IN THE CASE OF AUTONOMOUS DISCRETE DYNAMICAL SYSTEMS

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METHODS FOR DETERMINATION AND APPROXIMATION OF THE DOMAIN OF ATTRACTION IN THE CASE OF AUTONOMOUS DISCRETE DYNAMICAL SYSTEMS

ST. BALINT, E. KASLIK, A. M. BALINT, AND A. GRIGIS Received 15 October 2004; Accepted 18 October 2004

A method for determination and two methods for approximation of the domain of attrac- tionDa(0) of the asymptotically stable zero steady state of an autonomous,R-analytical, discrete dynamical system are presented. The method of determination is based on the construction of a Lyapunov functionV, whose domain of analyticity isDa(0). The first method of approximation uses a sequence of Lyapunov functionsVp, which converge to the Lyapunov functionVonDa(0). EachVpdefines an estimateNpofDa(0). For anyx Da(0), there exists an estimateNpxwhich containsx. The second method of approxima- tion uses a ballB(R)Da(0) which generates the sequence of estimatesMp=fp(B(R)).

For anyxDa(0), there exists an estimateMpxwhich containsx. The cases0f<1 and ρ(∂0f)<10fare treated separately because significant differences occur.

Copyright © 2006 Hindawi Publishing Corporation. All rights reserved.

1. Introduction

Let be the following discrete dynamical system:

xk+1=fxk

k=0, 1, 2,..., (1.1)

where fΩis an R-analytic function defined on a domain ΩRn, 0Ωand f(0)=0, that is,x=0 is a steady state (fixed point) of (1.1).

Forr >0, denote byB(r)= {xRn:x< r}the ball of radiusr.

The steady statex=0 of (1.1) is “stable” provided that given any ballB(ε), there is a ballB(δ) such that ifxB(δ) then fk(x)B(ε), fork=0, 1, 2,...[4].

If in addition there is a ballB(r) such thatfk(x)0 ask→ ∞for allxB(r) then the steady statex=0 is “asymptotically stable” [4].

The domain of attractionDa(0) of the asymptotically stable steady statex=0 is the set of initial statesxΩfrom which the system converges to the steady state itself, that is,

Da(0)=

xΩ|fk(x)−−−→k→∞ 0. (1.2)

Hindawi Publishing Corporation Advances in Dierence Equations Volume 2006, Article ID 23939, Pages1–15 DOI10.1155/ADE/2006/23939

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Theoretical research shows that theDa(0) and its boundary are complicated sets [5–9].

In most cases, they do not admit an explicit elementary representation. The domain of attraction of an asymptotically stable steady state of a discrete dynamical system is not necessarily connected (which is the case for continuous dynamical systems). This fact is shown by the following example.

Example 1.1. Let be the functionf :R→Rdefined byf(x)=(1/2)x(1/4)x2+ (1/2)x3+ (1/4)x4. The domain of attraction of the asymptotically stable steady statex=0 isDa(0)= (2.79,2.46)(1, 1) which is not connected.

Different procedures are used for the approximation of theDa(0) with domains hav- ing a simpler shape. For example, in the case of [4, Theorem 4.20, page 170] the domain which approximates theDa(0) is defined by a Lyapunov functionV built with the ma- trix0f of the linearized system in 0, under the assumption0f<1. In [2], a Lya- punov function V is presented in the case when the matrix0f is a contraction, that is,0f<1. The Lyapunov functionV is built using the whole nonlinear system, not only the matrix0f.V is defined on the wholeDa(0), and more, theDa(0) is the nat- ural domain of analyticity ofV. In [3], this result is extended for the more general case whenρ(∂0f)<1 (whereρ(∂0f) denotes the spectral radius of0f.) This last result is the following.

Theorem 1.2 (see [3]). If the function f satisfies the following conditions:

f(0)=0,

ρ0f<1, (1.3)

then 0 is an asymptotically stable steady state.Da(0) is an open subset ofΩand coincides with the natural domain of analyticity of the unique solutionV of the iterative first-order functional equation

Vf(x)V(x)= −x2,

V(0)=0. (1.4)

The functionV is positive onDa(0) andV(x)xx0+, for anyx0∂Da(0), (∂Da(0) de- notes the boundary ofDa(0)) or forx → ∞.

The functionV is given by V(x)=

k=0

fk(x)2 for anyxDa(0). (1.5)

The Lyapunov functionV can be found theoretically using relation (1.5). In the fol- lowings, we will shortly present the procedure of determination and approximation of the domain of attraction using the functionV presented in [2,3].

The region of convergenceD0of the power series development ofVin 0 is a part of the domain of attractionDa(0). IfD0is strictly contained inDa(0), then there exists a point x0∂D0such that the functionVis bounded on a neighborhood ofx0. Let be the power

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series development ofVinx0. The domain of convergenceD1of the series centered inx0 gives a new partD1\(D0D1) of the domain of attractionDa(0). At this step, the part D0 D1ofDa(0) is obtained.

If there exists a pointx1∂(D0 D1) such that the functionVis bounded on a neigh- borhood ofx1, then the domainD0 D1is strictly included in the domain of attraction Da(0). In this case, the procedure described above is repeated inx1.

The procedure cannot be continued in the case when it is found that on the boundary of the domainD0 D1 ··· Dp obtained at stepp, there are no points having neigh- borhoods on whichV is bounded.

This procedure gives an open connected estimateDof the domain of attractionDa(0).

Note that fk(D),kNis also an estimate ofDa(0), which is not necessarily connected.

The procedure described above is illustrated by the following examples.

Example 1.3. Let be the f :RRdefined by f(x)=x2. Due to the equalityfk(x)=x2k the domain of attraction of the asymptotically stable steady statex=0 isDa(0)=(1, 1).

The Lyapunov function isV(x)=

k=0x2k+1. The domain of convergence of the series is D0=(1, 1) which coincides withDa(0).

Example 1.4. Let be the function f=(−∞, 1)Ωdefined by f(x)=x/(e+ (1e)x).

Due to the equality fk(x)=x/(ek+ (1ek)x) the domain of attraction of the asymp- totically stable steady statex=0 isDa(0)=(−∞, 1). The power series expansion of the Lyapunov functionV(x)=

k=0|fk(x)|2in 0 is V(x)=

m=2

(m1) k=0

e2k1ekm2xm. (1.6)

The radius of convergence of the series (1.6) is

r0=mlim

→∞m

(m1)

k=0

e2k1ekm2=1, (1.7)

therefore the domain of convergence of the series (1.6) isD0=(1, 1)Da(0). More, V(x)→ ∞asx1 andV(1)<. The radius of convergence of the power series ex- pansion ofV in1 is

r1=mlim

→∞m

k=1

ekek1m2(m3)ek+ 2

2ek1m+2 =1, (1.8)

therefore the domain of convergence of the power series development ofVin1 isD1= (2, 0) which gives a new part ofDa(0).

Numerical results for more complex examples are given in [2,3].

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2. Theoretical results when the matrixA=0f is a contraction (i.e.,A<1) The function f can be written as

f(x)=Ax+g(x) for anyxΩ, (2.1)

whereA=0f andgΩis anR-analytic function such thatg(0)=0 and limx0(g(x) /x)=0.

Proposition 2.1. IfA<1, then there existsr >0 such thatB(r)Ωandf(x)<x for anyxB(r)\ {0}.

Proof. Due to the fact that limx0(g(x)/x)=0 there existsr >0 such thatB(r)Ω and

g(x)<1A

x for anyxB(r)\ {0}. (2.2) Let bexB(r)\ {0}. Inequality (2.2) provides that

f(x)=Ax+g(x)Ax+g(x)<A+ 1A

x = x (2.3)

therefore,f(x)<x.

Definition 2.2. LetR >0 be the largest number such thatB(R)Ωandf(x)<xfor anyxB(R)\ {0}.

If for anyr >0,B(r)Ωandf(x)<xfor anyxB(r)\ {0}, thenR=+and B(R)=Ω=Rn.

Lemma 2.3. (a)B(R) is invariant to the flow of system (1.1).

(b) For anyxB(R), the sequence (fk(x))k∈Nis decreasing.

(c) For anyp0 andxB(R)\ {0},ΔVp(x)=Vp(f(x))Vp(x)<0, where Vp(x)=

p k=0

fk(x)2 for xΩ. (2.4)

Proof. (a) Ifx=0, then fk(0)=0, for anykN. ForxB(R)\ {0}, we havef(x)<

x, which implies thatf(x)B(R), that is,B(R) is invariant to the flow of system (1.1).

(b) By induction, it results that forxB(R) we have fk(x)B(R) andfk+1(x) fk(x), which means that the sequence (fk(x))k∈Nis decreasing.

(c) In particular, for p0 and xB(R), we have fp+1(x)f(x)<x and

therefore,ΔVp(x)= fp+1(x)2x2<0.

Corollary 2.4. For any p0, there exists a maximal domainGpΩsuch that 0Gp

and forxGp\ {0}, the (positive definite) functionVpverifiesΔVp(x)<0. In other words, for any p0, the functionVp defined by (2.4) is a Lyapunov function for (1.1) onGp. Moreover,B(R)Gpfor anyp0.

Theorem 2.5. B(R) is an invariant set included in the domain of attractionDa(0).

Proof. Let bexB(R)\ {0}. We have to prove that limk→∞fk(x)=0.

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The sequence (fk(x))k∈Nis bounded: fk(x) belongs toB(R). Let be (fkj(x))j∈Na con- vergent subsequence and let be limj→∞fkj(x)=y0. It is clear thaty0B(R).

It can be shown that

fk(x)y0 for anykN. (2.5)

For this, observe first that fkj(x)y0 and (fkj(x))k∈N is decreasing (Lemma 2.3).

These imply thatfkj(x)y0for anykj. On the other hand, for anykN, there exists kjN such that kjk. Therefore, as the sequence (fk(x))k∈N is decreasing (Lemma 2.3), we obtain thatfk(x)fkj(x)y0.

We show now thaty0=0. Suppose the contrary, that is,y0=0.

Inequality (2.5) becomes

fk(x)y0>0 for anykN. (2.6) By means ofLemma 2.3, we have thatf(y0)<y0.

Therefore, there exists a neighborhoodUf(y0)B(R) of f(y0) such that for anyz Uf(y0) we havez<y0. On the other hand, for the neighborhoodUf(y0) there ex- ists a neighborhoodUy0B(R) of y0such that for any yUy0, we have f(y)Uf(y0). Therefore:

f(y)<y0 for anyyUy0. (2.7) As fkj(x)y0, there exists ¯jsuch that fkj(x)Uy0, for any jj. Making¯ y= fkj(x) in (2.7), it results that

fkj+1(x)=ffkj(x)<y0 for jj¯ (2.8) which contradicts (2.6). This means thaty0=0, consequently, every convergent subse- quence of (fk(x))k∈Nconverges to 0. This provides that the sequence (fk(x))k∈Nis con- vergent to 0, andxDa(0).

Therefore, the ballB(R) is contained in the domain of attraction ofDa(0).

Forp0 andc >0 let beNpcthe set Npc=

xΩ:Vp(x)< c. (2.9) Ifc=+, thenNcp=Ω.

Theorem 2.6. Let bep0. For anyc(0, (p+ 1)R2], the setNcpis included in the domain of attractionDa(0).

Proof. Let bec(0, (p+ 1)R2] andxNpc. ThenVp(x)=p

k=0fk(x)2< c(p+ 1)R2, therefore, there exists k∈ {0, 1,...,p}such thatfk(x)2< R2. It results that fk(x)

B(R)Da(0), therefore,xDa(0).

Remark 2.7. It is obvious that forp0 and 0< c< cone hasNpcNpc. Therefore, for a givenp0, the largest part ofDa(0) which can be found by this method isNpcp, where

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cp=(p+ 1)R2. In the followings, we will use the notation Np instead ofNpcp. Shortly, Np= {xΩ:Vp(x)<(p+ 1)R2}is a part ofDa(0). Let us note thatN0=B(R).

Remark 2.8. IfR=+(i.e.,Ω=Rnandf(x)<x, for anyxR\ {0}), thenNp= Rnfor anyp0 andDa(0)=Rn.

Theorem 2.9. For the sets (Np)p∈N, the following properties hold:

(a) for anyp0, one hasNpNp+1; (b) for anyp0, the setNpis invariant to f;

(c) for anyxDa(0), there existspx0 such thatxNpx. Proof. (a) Let bep0 andxNp. ThenVp(x)=p

k=0fk(x)2<(p+ 1)R2, therefore, there exists k∈ {0, 1,...,p}such that fk(x)2< R2. It results that fk(x)B(R) and therefore fm(x)B(R), for anymk. Form=p+ 1 we obtainfp+1(x)< R, hence Vp+1(x)=Vp(x) +fp+1(x)2<(p+ 1)R2+R2=(p+ 2)R2. Therefore,xNp+1.

(b) Let be xNp. If x< R then fm(x)< R for any m0 (by means of Lemma 2.3). This implies that Vp(f(x))=p

k=0fk(f(x))2=p+1

k=1fk(x)2<(p+ 1)R2, meaning that f(x)Np.

Let us suppose thatxR. AsxNp, we have thatVp(x)=p

k=0fk(x)2<(p+ 1)R2, therefore, there existsk∈ {0, 1,...,p}such thatfk(x)< R. It results that fk(x) B(R) and thereforefm(x)B(R), for anymk. Form=p+ 1 we obtainfp+1(x)< R.

This implies that Vp

f(x)=Vp(x) +fp+1(x)2x2<(p+ 1)R2+R2R2=(p+ 1)R2 (2.10)

therefore f(x)Np.

(c) Suppose the contrary, that is, there existxDa(0) such that for any p0,x / Np. Therefore,Vp(x)(p+ 1)R2 for any p0. Passing to the limit for p→ ∞in this inequality, provides thatV(x)= ∞. This means x∂Da(0) which contradicts the fact that x belongs to the open setDa(0). In conclusion, there exists px0 such that x

Npx.

Forp0 let beMp= fp(B(R))= {xΩ: fp(x)B(R)}, obtained by the trajectory reversing method.

Theorem 2.10. The following properties hold:

(a)MpDa(0) for anyp0;

(b) for anyp0,Mpis invariant to f; (c)MpMp+1for anyp0;

(d) for anyxDa(0), there existspx0 such thatxMpx.

Proof. (a) AsMp=fp(B(R)) andB(R)Da(0) (seeTheorem 2.5) it is clear thatMp Da(0).

(b) and (c) follow easily by induction, usingLemma 2.3.

(d)xDa(0) provides that fp(x)0 asp→ ∞. Therefore, there existspxNsuch that fp(x)B(R), for anyppx. This provides thatxMpfor anyppx.

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Both sequences of sets (Mp)p∈Nand (Np)p∈Nare increasing, and are made up of esti- mates ofDa(0). From the practical point of view, it is important to know which sequence converges more quickly. The next theorem provides that the sequence (Mp)p∈Nconverges more quickly than (Np)p∈N, meaning that for p0, the setMp is a larger estimate of Da(0) thenNp.

Theorem 2.11. For anyp0, one hasNpMp.

Proof. Let bep0 andxNp. We have thatVp(x)=p

k=0fk(x)2<(p+ 1)R2, there- fore, there existsk∈ {0, 1,...,p}such thatfk(x)< R. This implies that fm(x)B(R), for anymk. Form=pwe obtain fp(x)B(R), meaning thatxMp. 3. Theoretical results whenA=0f is a convergent noncontractive matrix

(i.e.,ρ(A)<1A)

Proposition 3.1. Ifρ(A)<1A, then there existp2 andrp>0 such thatB(rp)Ω andfp(x)<xfor anyp∈ {p,p+ 1,..., 2p1}andxB(rp)\ {0}.

Proof. We have thatρ(A)<1 if and only if limp→∞Ap=0 (see [1]), which provides (to- gether withA1) that there exists p2 such thatAp<1 for any pp. Let be p2 fixed with this property.

The formula of variation of constants for anypgives:

fp(x)=Apx+

p1 k=0

Apk1gfk(x) xΩ, pN. (3.1)

Due to the fact that for anykNwe have limx0(g(fk(x))/x)=0, there existsrp>0 such that for anyp∈ {p, p+ 1,..., 2p1}the following inequality holds:

p1 k=0

Apk1gfk(x)<1Apx for xBrp

\ {0}. (3.2) Let bexB(rp)\ {0}andp∈ {p,p+ 1,..., 2p1}. Using (3.1) and (3.2) we have

fp(x)= Apx+

p1 k=0

Apk1gfk(x)

Apx+

p1 k=0

Apk1gfk(x)

<Ap+ 1Apx = x.

(3.3)

Therefore,fp(x)<xforp∈ {p, p+ 1,..., 2p1}andxB(rp)\ {0}. Definition 3.2. Let p2 be the smallest number such thatAp<1 for anypp(see the proof ofProposition 3.1). LetR > 0 the largest number be such thatB(R) Ωand fp(x)<xforp∈ {p, p+ 1,..., 2p1}andxB(R) \ {0}.

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If for anyr >0, we have thatB(r)Ωandfp(x)<xfor any p∈ {p, p+ 1,..., 2p1}andxB(r)\ {0}, thenR=+andB(R) =Ω=Rn.

Lemma 3.3. (a) For anyxB(R) and p∈{p,p+ 1,..., 2p1}, the sequence (fkp(x))k∈N

is decreasing.

(b) For anyppandxB(R) \ {0},fp(x)<x.

(c) For any ppandxB(R) \ {0},ΔVp(x)=Vp(f(x))Vp(x)<0, where Vp is defined by (2.4).

Proof. (a) Ifx=0, then fp(0)=0, for anyp0.

Let bexB(R) \ {0}. We know thatfp(x)<xfor anyp∈ {p,p+ 1,..., 2p1}. It results that fp(x)B(R) for any p∈ {p, p+ 1,..., 2p1}. This implies that for any kNwe havefkp(x)<xandf(k+1)p(x)fkp(x), meaning that the sequence (fkp(x))k∈Nis decreasing.

(b) Let bexB(R) \ {0}. Inequalityfp(x)<xis true for any p∈ {p, p+ 1,..., 2p1}.

Let bep2p. There exists qNand p∈ {p, p+ 1,..., 2p1}such thatp=qp+ p. Using (a), we have that fp(x)B(R) and fqp(y)y, for anyyB(R), therefore

fp(x)=fqpfp(x)fp(x)<x (3.4)

(c) results directly from (b).

Corollary 3.4. For anypp, there exists a maximal domain GpΩsuch that 0Gp

and for anyxGp\ {0}, the (positive definite) functionVp verifiesΔVp(x)<0. In other words, for anypp, the function Vpis a Lyapunov function for (1.1) onGp. More,B(R) Gpfor anypp.

Lemma 3.5. For anykp, there exists qkNsuch that

f(qk+3)p(x)fk(x)fqkp(x) for anyxB R. (3.5)

Proof. Let bekp. There exists a unique qkNand a uniquepk∈ {p, p+ 1,..., 2p1} such thatk=qkp+pk.Lemma 3.3provides that for anyxB(R) we have that fqkp(x) B(R) and fpk(x)x. It results that

fk(x)=fpkfqkp(x)fqkp(x) for anyxBR¯. (3.6)

On the other hand, we have (qk+ 3)p=k+ (3ppk). As (3ppk)∈ {p+ 1,p+ 2,..., 2p} andkp, Lemma 3.3 provides that for anyxB(R) we have that fk(x)B(R) and

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f3ppk(x)x. Therefore

f(qk+3)p(x)=f3ppkfk(x)fk(x) for anyxB R. (3.7)

Combining the two inequalities, we get that

f(qk+3)p(x)fk(x)fqkp(x) for anyxB R (3.8)

which concludes the proof.

Theorem 3.6. B(R) is included in the domain of attraction Da(0).

Proof. Let bexB(R) \ {0}. We have to prove that limk→∞fk(x)=0.

The sequence (fk(x))k∈Nis bounded (seeLemma 3.3). Let be (fkj(x))j∈Na convergent subsequence and let be limj→∞fkj(x)=y0.

We suppose, without loss of generality, thatkjpfor any jN.Lemma 3.5provides that for anyjNthere existsqjNsuch that

f(qj+3)p(x)fkj(x)fqjp(x). (3.9)

As (fqjp(x))j∈Nand (f(qj+3)p(x))j∈N are subsequences of the convergent sequence (fqp(x))q∈N(decreasing, according toLemma 3.3), it results that they are convergent.

The double inequality (3.9) provides that limj→∞fqjp(x) = y0. Therefore, limq→∞

fqp(x) = y0. It can be shown that

fk(x)y0 for anykp. (3.10)

For this, remark that limq→∞fqp(x) = y0and (fqp(x))q∈Nis decreasing (Lemma 3.3), which implies thatfqp(x)y0for anyqN. On the other hand,Lemma 3.5 provides that for anykpthere existsqksuch thatf(qk+3)p(x)fk(x). Therefore, fk(x)f(qk+3)p(x)y0, for anykp.

We show now thaty0=0. Suppose the contrary, that is,y0=0.

Inequality (3.10) becomes

fk(x)y0>0 for anykp. (3.11)

By means ofLemma 3.3, we have thatfp(y0)<y0.

There exists a neighborhoodUfp(y0)B(R) of fp(y0) such that for anyzUfp(y0)we havez<y0. On the other hand, for the neighborhoodUfp(y0)there exists a neigh- borhoodUy0B(R) of y0such that for anyyUy0, we havefp(y)Ufp(y0). Therefore:

fp(y)<y0 for anyyUy0. (3.12)

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