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BY 4.0 license Open Access Published by De Gruyter July 24, 2021

Nonuniform dichotomy spectrum and reducibility for nonautonomous difference equations

  • Jifeng Chu , Fang-Fang Liao , Stefan Siegmund EMAIL logo , Yonghui Xia and Hailong Zhu

Abstract

For nonautonomous linear difference equations, we introduce the notion of the so-called nonuniform dichotomy spectrum and prove a spectral theorem. As an application of the spectral theorem, we prove a reducibility result.

MSC 2010: 37D25; 37B55

1 Introduction

Let Ak ∈ ℝN × N, k ∈ ℤ, be a sequence of invertible matrices. In this paper, we consider the following nonautonomous linear difference equations

(1.1) xk+1=Akxk,

where xk ∈ ℝN, k ∈ ℤ. Let Φ:ℤ  ×  ℤ → ℝN × N, (k, l)↦Φ(k, l), denote the evolution operator of (1.1), i.e.,

Φ ( k , l ) = A k 1 A l , f o r k > l , I d , f o r k = l , A k 1 A l 1 1 , f o r k < l .

Obviously, Φ(k, m)Φ(m, l) = Φ(k, l), k, m, l ∈ ℤ, and Φ(·, l)ξ solves the initial value problem (1.1), x(l) = ξ, for l ∈ ℤ, ξ ∈ ℝN.

An invariant projector of (1.1) is defined to be a function P:ℤ → ℝN × N of projections Pk, k ∈ ℤ, such that for each Pk the following property holds

Pk+1Ak=AkPk,kZ.

We say that (1.1) admits an exponential dichotomy if there exist an invariant projector P and constants 0 < α < 1, K ≥ 1 such that

(1.2) Φ(k,l)PlKαkl,kl,

and

(1.3) Φ(k,l)QlK(1α)kl,kl,

where Ql = Id − Pl is the complementary projection.

The notion of exponential dichotomy was introduced by Perron in [25] and has attracted a lot of interest during the last few decades because it plays an important role in the study of hyperbolic dynamical behavior of differential equations and difference equations. For example, see [1, 19, 28] and the references therein. We also refer to the books [10, 16, 22] for details and further references related to exponential dichotomies. On the other hand, during the last decade, inspired both by the classical notion of exponential dichotomy and by the notion of nonuniformly hyperbolic trajectory introduced by Pesin (see [5]), Barreira and Valls have introduced the notion of nonuniform exponential dichotomies and have developed the corresponding theory in a systematic way (see [6] and the references therein). As explained by Barreira and Valls, in comparison to the notion of exponential dichotomies, nonuniform exponential dichotomy is a useful and weaker notion.

We say that (1.1) admits a nonuniform exponential dichotomy if there exist an invariant projector P and constants 0 < α < 1, K = 1, ε ≥ 1 such that αε2 < 1 and

(1.4) Φ(k,l)PlKαklε|l|,kl,

and

(1.5) Φ(k,l)QlK(1α)klε|l|,kl.

When ε = 1, (1.4)-(1.5) become (1.2)-(1.3), and therefore a nonuniform exponential dichotomy becomes an exponential dichotomy. Moreover, [5, Theorem 1.4.2]bp02 indicates that the condition αε2 < 1 is reasonable, which means that the nonuniform part is small.

For example, given ω>5a > 0, then the linear equation

(1.6) uk+1=eω+ak(1)ka(k1)(1)(k1)uk,vk+1=eωak(1)k+a(k1)(1)(k1)vk

admits a nonuniform exponential dichotomy, but does not admit an exponential dichotomy. In fact, we have

Φ(k,l)Pl=eω(kl1)a(kl1)(1)k1al(1)(k1)+al(1)l000

with Pl=1000 . Therefore (1.4) holds with

K=eωa>1,α=e(ω+a)(0,1),ε=e2a>1.

Analogous arguments applied to the second equation yield the estimate (1.5). Moreover, when both k and l are even, we obtain the equality

Φ(k,l)Pl=Kαklε|l|,kl,

which means that the nonuniform part εl = e2al cannot be removed.

Among the different topics on classical exponential dichotomies, the dichotomy spectrum (also called dynamical spectrum, or Sacker-Sell spectrum) is very important and many results have been obtained. As far as we know, dynamical spectrum defined with exponential dichotomies was first introduced by Sacker and Sell in [29] in which they studied the linear skew product flows with compact base. For more results on dichotomy spectrum, we refer the reader to [2, 3, 13, 18, 23, 26, 27, 29, 31, 32] and the references therein. The definition and investigation for finite-time hyperbolicity have also been studied in [9, 17]. The dynamical spectral theorem has some important applications. For example, based on the dichotomy spectral theorem, normal forms for nonautonomous systems were established in [20,21,33]. However, all the results mentioned above were established in the setting of classical exponential dichotomies. In this paper, we establish the corresponding spectral theory for difference equations (1.1) with a nonuniform exponential dichotomy. To the best of our knowledge the nonuniform dichotomy spectral theory for linear differential equations was first studied in [14] and [35]. We refer the reader to [7, 8, 11, 12, 34] for further results on nonuniform dichotomy spectrum.

This paper is organized as follows. In Section 2 we propose a definition of spectrum based on nonuniform exponential dichotomies, which is called nonuniform dichotomy spectrum. Such a spectrum can be seen as a generalization of Sacker-Sell spectrum. We prove a nonuniform dichotomy spectral theorem. In Section 3, as an application of the spectral theorem, we prove a reducibility result for (1.1). Recall that system (1.1) is called reducible if it is kinematically similar to a block diagonal system with blocks of dimension less than N.

2 Nonuniform dichotomy spectrum

Consider the weighted system

(2.1) xk+1=1γAkxk,

where γ ∈ ℝ+ = (0, ∞). One can easily see that

Φγ(k,l):=(1γ)klΦ(k,l)

is its evolution operator. If for some γ ∈ ℝ+, (2.1) admits a nonuniform exponential dichotomy with projector Pk and constants K ≥ 1, 0 < α < 1 and ε ≥ 1, then Pk is also invariant for (1.1), that is

Pk+1Ak=AkPk,kZ,

and the dichotomy estimates of (2.1) are equivalent to

(2.2) Φ(k,l)PlK(γα)klε|l|,kl,

and

(2.3) Φ(k,l)QlK(γ1α)klε|l|,kl.

Definition 2.1

The nonuniform dichotomy spectrum of (1.1) is the set

ΣNED(A)={γR+:2.1admitsnononuniformexponentialdichotomy},

and the resolvent set ρNED(A) = ℝ+∖ΣNED(A) is its complement. The dichotomy spectrum of (1.1) is the set

ΣED(A)={γR+:2.1admitsnoexponentialdichotomy},

and ρED(A) = ℝ+∖ΣED(A).

Proposition 1

ΣNED(A) ⊂ ΣED(A).

Proof. For each γ ∈ ρED(A), the weighted system (2.1) admits an exponential dichotomy. Consequently, the weighted system (2.1) admits a nonuniform exponential dichotomy. Thus, γ ∈ ρNED(A), which implies that ρED(A) ⊂ ρNED(A), and therefore ΣNED(A) ⊂ ΣED(A). □

Let us define for γ ∈ ρNED(A)

Sγ:=(l,ξ)Z×RN:supklΦ(k,l)ξγkε|l|<,

and

Uγ:=(l,ξ)Z×RN:supklΦ(k,l)ξγkε|l|<,

where ε is the constant in (2.2)-(2.3). Note that 𝒮γ and 𝒰γ depend on ε=ε(γ) for each γ ∈ ρNED(A). If in addition γ ∈ ρED(A) then it is shown below that these sets do not depend on ε, more precisely, εcan be set to equal 1. One may readily verify that 𝒮γ and 𝒰γ are invariant vector bundles of (1.1), here we say that a nonempty set WZ×RN is an invariant vector bundle of (1.1) if (a) it is invariant, i.e., (l,ξ)W(k,Φ(k,l)ξ)W for all k ∈ ℤ; and (b) for every l ∈ ℤ the fiber W(l)={ξRN:(l,ξ)W} is a linear subspace of ℝN.

The next lemma gives the relationship between 𝒮γ, 𝒰γ and the projector P. In [16, Chapter 2]cop it is proved in the setting of exponential dichotomies that the invariant projector is unique. The proof for the invariant projectors for (1.1) and (2.1) in the setting of nonuniform exponential dichotomies is almost identical.

Lemma 2.2

Assume that (2.1) admits a nonuniform exponential dichotomy with invariant projector P for γ ∈ ℝ+. Then

Sγ=imP,Uγ=kerP and SγUγ=Z×RN.

Proof. We show only Sγ=imP . The fact 𝒰γ = ker P is analog and the fact SγUγ=Z×RN is clear.

First we show SγimP . Let l ∈ ℤ and ξ ∈ 𝒮γ(l). Then there exists a positive constant C such that

Φ(k,l)ξCγkε|l|,kl.

We write ξ = ξ1+ξ2 with ξ1 ∈ im Pl and ξ2 ∈ ker Pl. We show that ξ2 = 0. By invariance of P we have for k ∈ ℤ the identity

ξ2=Φγ(l,k)Φγ(k,l)Qlξ=Φγ(l,k)QkΦγ(k,l)ξ.

Using the fact that (2.1) admits a nonuniform exponential dichotomy, it follows that

Φγ(l,k)QkK(1α)lkε|k|.

Thus

ξ2K1αlkε|k|Φγ(k,l)ξ=K(αε)klεlk+|k|1γklΦ(k,l)ξCK(αε)klεl+|l|k+|k|1γklγk,kl,

which implies that when kl and k > 0, we have

ξ2CK(αε)klε2|l|γl,

and therefore ξ2 = 0 by letting k → ∞, since αε<1.

Next we show imPSγ . Let l ∈ ℤ and ξ ∈ im Pl, i.e., Plξ = ξ. Using the fact that α<1, the nonuniform exponential dichotomy estimate implies

Φγ(k,l)ξKαklε|l|ξKε|l|ξ,kl,

which yields

Φ(k,l)ξKγklε|l|ξ,

and thus ξ ∈ 𝒮γ(l).

Lemma 2.3

The resolvent set is open, i.e., for every γ ∈ ρNED(A), there exists a β = β(γ) ∈ (0, 1) with (βγ,1βγ)ρNED(A) . Furthermore,

Sζ=Sγanduζ=uγforζβγ,1βγ.

Proof. Let γ ∈ ρNED(A). Then (2.1) admits a nonuniform exponential dichotomy, i.e., the estimates (2.2)-(2.3) hold with an invariant projector P and constants K ≥ 0, 0<α <1 and ε ≥ 1. For β:=α(0,1) and ζ(βγ,1βγ) we have

Φζ(k,l)=(γζ)klΦγ(k,l).

Note that P is also an invariant projector for the equation

xk+1=1ζAkxk.

Moreover, we have the estimates

Φζ(k,l)PlK(γζα)klε|l|Kβklε|l|,kl,

and

Φζ(k,l)QlK(γζ1α)klε|l|K(1β)klε|l|,kl.

Hence ζ ∈ ρNED(A). Therefore, ρNED(A) is an open set. Using Lemma 2.2, we know that 𝒮ζ = 𝒮γ and 𝒰ζ = 𝒰γ.

Corollary 2.4

ΣNED(A) is a closed set.

Using the facts proved above, we can obtain the following result, whose proof is similar as [4, Lemma 2.2], and therefore we omit the proof here.

Lemma 2.5

Let γ1, γ2 ∈ ρNED(A) with γ1 < γ2. Then F=Uγ1Sγ2 is an invariant vector bundle which satisfies exactly one of the following two alternatives and the statements given in each alternative are equivalent:

Alternative I Alternative II
(A)F=Z×{0}. AFZ×{0}.
(B)γ1,γ2ρNED(A). (B')Thereisaζγ1,γ2ΣNED(A).
(C)Sγ1=Sγ2andUγ1=Uγ2. CdimSγ1<dimSγ2.
(D)Sγ=Sγ2anduγ=Uγ2forγγ1,γ2. DdimCγ1>dimUγ2.

Now we are in a position to state and prove the nonuniform dichotomy spectral theorem which will be essential to prove the result on reducibility in Section 3. The proof follows the idea and technique of the classical dichotomy spectrum proposed in [30], we present the details for the reader’s convenience.

Theorem 2.6

The nonuniform dichotomy spectrum NED(A) of (1.1) is the disjoint union of n closed intervals (called spectral intervals) where 0nN,i.e.,ΣNED(A)=orΣNED(A)=R+ or one of the four cases

ΣNED(A)=a1,b1or0,b1a2,b2an1,bn1an,bnoran,

where 0 < a1b1 < a2b2 < ··· < anbn. Choose a

(2.4) γ0ρNED(A)with0,γ0ρNED(A)ifpossible,

otherwise define Uγ0:=Z×RN,Sγ0:=Z×{0} . Choose a

(2.5) γnρNED(A)withγn,+ρNED(A)ifpossible,

otherwise define Uγn:=Z×{0},Sγ0:=Z×RN . Then the sets

W0=Sγ0 and Wn+1=Sγn

are invariant vector bundles of (1.1). For n = 2, choose γi ∈ ρNED(A) with

(2.6) b i < γ i < a i + 1 f o r i = 1 , , n 1 ,

then for every i = 1, …, n  −  1 the intersection

Wi=Uγi1Sγi

is an invariant vector bundle of (1.1) with dim 𝒲i ≥ 1. The invariant vector bundles 𝒲i, i = 0, …, n + 1, are called spectral bundles and they are independent of the choice of γ0, …, γn in (2.4), (2.5) and (2.6). Moreover

W0Wn+1=Z×RN

is a direct sum, i.e., WiWj=Z×{0} for ij and W0++Wn+1=Z×RN .

Proof. Recall that the resolvent set ρNED(A) is open and therefore ΣNED(A) is the disjoint union of closed intervals. Next we will show that ΣNED(A) consists of at most N intervals. Indeed, if ΣNED(A) contains N + 1 components, then one can choose a collection of points ζ1, …, ζN in ρNED(A) such that ζ1<··· < ζN and each of the intervals (0, ζ1), (ζ1, ζ2), …, (ζN − 1, ζN), (ζN, ∞) has nonempty intersection with the spectrum ΣNED(A). Now alternative II of Lemma 2.5 implies

0dimsζ1<<dimSζNN

and therefore either dimSζ1=0ordimSζN=N or both. Without loss of generality, dimSζN=N , i.e., SζN=Z×RN . Assume that

xk+1=1ζNAkxk

admits a nonuniform exponential dichotomy with invariant projector P ≡ Id, then

xk+1=1ζAkxk

also admits for every ζ>ζN a nonuniform exponential dichotomy with the same projector. We conclude (ζN, ∞) ⊂ ρNED(A), which is a contradiction. This proves the alternatives for ΣNED(A).

Due to Lemma 2.5, the sets 𝒲0, …, 𝒲n+1 are invariant vector bundles. To prove now that dim 𝒲1 ≥ 1, …, dim 𝒲n ≥ 1 for n ≥ 1, let us assume that dim 𝒲1 = 0, i.e., Uγ0Sγ1=Z×{0} . If (0, b1] is a spectral interval this implies that Sγ1=Z×{0} . Then the projector of the nonuniform exponential dichotomy of

xk+1=1γ1Akxk

is 0 and then we get the contradiction (0, γ1) ⊂ ρNED(A). If [a1, b1] is a spectral interval then [γ0, γ1]∩ΣNED(A)≠∅ and by alternative II of Lemma 2.5 we get a contradiction. Therefore dim 𝒲1 ≥ 1 and analogously dim𝒲n ≥ 1. Furthermore for n ≥ 3 and i = 2, …, n  −  1 one has [γi − 1, γi]∩ΣNED(A)≠∅ and again alternative II of Lemma 2.5 yields dim𝒲i ≥ 1.

For i < j we have WiSγi and WjUγj1Uγi and with Lemma 2.5 this gives WiWjSγiUγi=Z×{0} , so WiWj=Z×{0} for ij.

To show that W0Wn+1=Z×RN , recall the monotonicity relations Sγ0Sγn , Uγ0Uγn , and the identity SγUγ=Z×RN for γ ∈ ℝ+. Therefore Z×RN=W0+Uγ0 . Now we have

Z × R N = W 0 + U γ 0 [ S γ 1 + U γ 1 ] = W 0 + [ U γ 0 S γ 1 ] + U γ 1 = W 0 + W 1 + U γ 1 .

Doing the same for Uγ1 , we get

Z × R N = W 0 + W 1 + U γ 1 [ S γ 2 + U γ 2 ] = W 0 + W 1 + [ U γ 1 S γ 2 ] + U γ 2 = W 0 + W 1 + W 2 + U γ 2 ,

and mathematical induction yields Z×RN=W0++Wn+1 . To finish the proof, let γ˜0,,γ˜nρNED(A) be given with the properties (2.4), (2.5) and (2.6). Then alternative I of Lemma 2.5 implies

Sγi=Sγ˜iandUγi=Uγ˜ifori=0,,n

and therefore the invariant vector bundles 𝒲0, …, 𝒲n+1 are independent of the choice of γ0, …, γn in (2.4), (2.5) and (2.6).

Definition 2.7

We say that the evolution operator of (1.1) is nonuniformly exponentially bounded if there exist K > 0, ε ≥ 1 and a ≥ 1 with

(2.7) Φ(k,l)Ka|kl|ε|l|,k,lZ.

Lemma 2.8

Assume the evolution operator of (1.1) is nonuniformly exponentially bounded. Then ΣNED(A) is a bounded closed set and ΣNED(A)[1a,a] .

Proof. Assume that (2.7) holds. Let γ > a and 0<α:=aγ<1 , then estimate (2.7) implies

Φγ(k,l)Kαklε|l|,kl.

Therefore (1.1) admits a nonuniform exponential dichotomy with invariant projector P = Id. It follows that γ ∈ ρNED(A) and also similarly for 0<γ<1a , hence ΣNED(A)[1a,a] .

Lemma 2.9

The evolution operator of (1.1) is nonuniformly exponentially bounded if and only if the nonuniform dichotomy spectrum ΣNED(A) of (1.1) is the disjoint union of n closed intervals where 0 ≤ n ≤ N, i.e.,

ΣNED(A)=[a1,b1][a2,b2][an1,bn1][an,bn],

where 0 < a1b1 < a2b2 < ··· < anbn < ∞. In addition, W1Wn=Z×RN , W0=Wn+1=Z×{0} , where the sets 𝒲0, …, 𝒲n+1 are invariant vector bundles defined in Theorem 2.6.

Proof. Necessity. It is easy to know that ΣNED(A) is bounded from Lemma 2.8. Now we prove that ΣNED(A)≠∅. It is easy to verify that Sγ=imP=Z×RN and Uγ=kerP=Z×{0} for γ>a. Set

γ = inf γ ρ N E D ( A ) : S γ = Z × R N .

Clearly, γ[1a,a] . In addition, we have γ* ∈ ΣNED(A). Otherwise, by using Lemma 2.3, there exists a neighborhood J of γ* such that JρNED(A) and for any γ<γ* of J we have Sγ=Sγ=Z×RN , which is a contradiction to the definition of γ*. So ΣNED(A)≠∅, which means that

ΣNED(A)=[a1,b1][a2,b2][an1,bn1][an,bn].

Let γ0 ∈ (0, a1), γi ∈ (bi, ai+1) for i = 1, …, n  −  1 and γn ∈ (bn, ∞). Clearly, from the proof of Lemma 2.8, we have Uγn=Z×{0} for γn>bn and Sγ0=Z×{0} for 0<γ0<a1. Therefore, W0=Wn+1=Z×{0} , and then it follows from Theorem 2.6 that W1Wn=Z×RN .

Sufficiency. Let γ0 ∈ (0, a1), γi ∈ (bi, ai+1) for i = 1, …, n  −  1 and γn ∈ (bn, ∞). Clearly, from the proof of Lemma 2.8, we have Sγn=Z×RN for γn>bn and Uγ0=Z×RN for 0 <γ0<a1. This means that the invariant projectors associated to γ0 and γn are Pl = 0 and Pl = Id respectively.

Hence, there exist K0 > 1, 0<α0 < 1 and ε0 > 1 such that

Φγ0(k,l)K0(1α0)klε0|l|,kl,

and there exist Kn > 1, 0 < αn < 1 and εn > 1 such that

Φγn(k,l)Knαnklεn|l|,kl.

Now taking K = max{K0, Kn}, ε = max{ε0, εn} and a=max{a0γ0,anγn} , then we have

Φ(k,l)Kα|kl|ε|l|,fork,lZ,

which shows that the evolution operator of (1.1) is nonuniformly exponentially bounded.

From Proposition 1, we know ΣNED(A) ⊂ ΣED(A). Finally in this section, we present an example to illustrate that ΣNED(A)≠ΣED(A) can occur.

Example 2.10

Given ω>5a > 0. Consider the scalar equation

(2.8) uk+1=Akuk

with

Ak=eω+ak(1)ka(k1)(1)(k1).

Then ΣNED(A) = [eω − 5a, eω+5a] and ΣED(A) = ℝ+.

Proof. The evolution operator of (2.8) is given by

Φ ( k , l ) = e ω ( k l 1 ) a ( k l 1 ) ( 1 ) k 1 a l ( 1 ) ( k 1 ) + a l ( 1 ) l .

For each γ ∈ ℝ+ the evolution operator of

(2.9) ukuk+1=1γAkuk

is given by

(2.10) Φ γ ( k , l ) = ( 1 γ ) ( k l ) e ω ( k l 1 ) a ( k l 1 ) ( 1 ) k 1 a l ( 1 ) ( k 1 ) + a l ( 1 ) l .

For any γ ∈ (e( − ω+5a), +∞), it follows from (2.10) that

(2.11) Φ γ ( k , l ) e ω a e ω + a γ k l e 2 a | l | , k l ,

which implies that the equation (2.9) admits a nonuniform exponential dichotomy with invariant projector P = Id, by setting

K=eωa,α=eω+aγ<1,ε=e2a>0.

Thus,

(2.12) (eω+5a,+)ρNED(A).

For any γ˜(0,eω5a) , it follows from (2.10) that

(2.13) Φγ(k,l)eω+aeωaγkle2a|l|,kl,

which implies that (2.9) admits a nonuniform exponential dichotomy with P = 0, by taking

K=eω+a,α=γeωa<1,ε=e2a>0.

Thus,

(2.14) (0,eω5a)ρNED(A).

It follows from (2.12) and (2.14) that

(0,eω5a)(eω+5a,+)ρNED(A),

which implies that

ΣNED(A)[eω5a,eω+5a].

Next we show that

[eω5a,eω+5a]ΣNED(A).

To do this, we first prove that γ1 = eω+5a ∈ ΣNED(A). The evolution operator of the system

uk+1=1γ1Akuk

is given as

Φ γ 1 ( k , l ) = e ω a e a ( k l 1 ) ( 1 + ( 1 ) k 1 ) a l ( 1 ) ( k 1 ) + a l ( 1 ) l .

It is easy to see that there do not exist K, α>0 and ε>0 such that

Φγ1(k,l)Kαklε|l|,forkl,

or

Φγ1(k,l)K(1α)klε|l|,forkl.

Therefore γ1 = eω+5a ∈ ΣNED(A). In a similar manner, we can prove γ2 = eω − 5a ∈ ΣNED(A). We can see from Theorem 2.6 that (2.8) has at most one nonuniform dichotomy spectral interval, which means that [eω − 5a, eω+5a] ⊂ ΣNED(A) and therefore [eω − 5a, eω+5a] = ΣNED(A).

On the other hand, using a similar argument as in equations (1.6), we know that the nonuniform part εl cannot be removed in the estimates (2.11) and (2.13). Therefore, (2.8) does not admit an exponential dichotomy, which means that ΣED(A) = ℝ+.

3 Reducibility

In this section we utilize Theorem 2.6 to show a reducibility result. For the reducibility results in the setting of an exponential dichotomy, we refer the reader to [15, 24, 32] and the references therein. First we recall the definition of kinematic similarity given in Coppel [16] and Aulbach et al. [2].

Definition 3.1

Equation (1.1) is said to be kinematically similar to another equation

(3.1) yk+1=Bkyk

with k ∈ ℤ, if there exists an invertible matrix Sk withSk∣ ≤ M and Sk1M (M > 0), which satisfies the difference equation

Sk+1Bk=AkSk.

The change of variables xk = Skyk then transforms (1.1) into (3.1).

The next lemma is important to establish the reducibility results and its proof follows along the lines of the proof of Siegmund [32]. See also Coppel [16] and Aulbach et al. [2]

Lemma 3.2

[16, Chapter 5] Let P be an orthogonal projection (PT = P) and let X be an invertible matrix function. Then there exists an invertible matrix function S:ZRN×N such that

SkPSk1=XkPXk1,SkQSk1=XkQXk1,

and

Sk2,
Sk1[XkPXk12+Xk(IP)Xk12]12,

where k ∈ ℤ and Q = Id − P. Define

R˜:ZRN×N,kPXkTXkP+[IdP]XkTXk[IdP].

Then the mapping is a positive definite, symmetric matrix for every kZ . Moreover, there is a unique function

R:ZRN×N

of positive definite symmetric matrices Rk, kZ , with

Rk2=R˜k,PRk=RkP.

We remark that in the setting of an exponential dichotomy the function kSk1 in Lemma 3.2 is bounded. However, in the setting of a nonuniform exponential dichotomy, Sk1 can be unbounded, because ∣Φ(k, k)Pk∣ ≤ Kεk for k = 0. In fact, we can see that

(3.2) Sk12Kε|k|.

To overcome the difficulty, we introduce a new version of non-degeneracy, so-called weak non-degeneracy and define the concept of weak kinematical similarity, which is a very natural notion if we note the fact (3.2).

Definition 3.3

S:ZRN×N is called weakly non-degenerate if there exists an M = M(ε)>0 such that

SkMε|k|andSk1Mε|k|,forallkZ,

where ε is the same constant in (1.4)-(1.5).

Definition 3.4

If there exists a weakly non-degenerate matrix Sk such that

Sk+1Bk=AkSk,

then equation (1.1) is weakly kinematically similar to equation (3.1). For short, we denote (1.1) w (3.1) or AkwBk .

We analogously denote kinematical similarity by (1.1)(3.1) or AkBk.

Definition 3.5

Equation (1.1) is called reducible, if it is weakly kinematically similar to equation (3.1) whose coefficient matrix Bk has the block diagonal form

(3.3) Bk100Bk2,

where Bk1 and Bk2 are matrices of smaller size than Bk.

Before stating the main results of this section, we prove several preliminary lemmas.

Lemma 3.6

Assume that (1.1) admits a nonuniform exponential dichotomy. Then the projector of equation (1.1) can be chosen as P˜=IN1000N2 with N1=dimimP˜ and N2=dimkerP˜ , and the fundamental matrix Xk can be chosen suitably such that the estimates (1.4)-(1.5) can be rewritten as

(3.4) XkP˜Xl1Kαklε|l|,kl,

and

(3.5) XkQ˜Xl1K(1α)klε|l|,kl,

where Q˜=IdP˜ .

Proof. Let nZ be arbitrary but fixed. Note that the rank of the projector Pn is independent of nZ (see [9, page 1100]), then there exists a nondegenerate matrix T ∈ ℝN × N such that

P˜:=IN1000N2=TPnT1

with N1=dimimP˜ and N2=dimkerP˜ . Define

Xk:=Φ(k,n)T1forkZandP˜:=IN1000N2=TPnT1.

Then

(3.6) XkP˜Xl1=Φ(k,n)T1P˜TΦ1(l,n)=Φ(k,n)PnΦ1(l,n).

On the other hand, we have

(3.7) Φ ( k , l ) P l = Φ ( k , n ) Φ ( n , l ) P l = Φ ( k , n ) P n Φ ( n , l ) = Φ ( k , n ) P n Φ 1 ( l , n ) .

It follows from (3.6) and (3.7) that (1.4)-(1.5) can be rewritten in the form (3.4)-(3.5).

Lemma 3.7

Assume that (1.1) admits a nonuniform exponential dichotomy with the form of estimates (3.4)-(3.5) and rank(P˜)=N1,(0<N1<N) , and there exists a weakly non-degenerate transformation Sk such that AkwBk . Then system (3.1) also admits a nonuniform exponential dichotomy, and the projector has the same rank.

Proof. Suppose that Sk is weakly non-degenerate, which means that there exists M = M(ε) > 0 such that ∣Sk∣ ≤ Mεk and Sk1Mε|k| and such that AkwBk . Let Xk = SkYk. It is easy to see that Yk is the fundamental matrix of system (3.1). To prove that system (3.1) admits a nonuniform exponential dichotomy, we first consider the case kl and obtain

(3.8) YkP˜Yl1=Sk1XkP˜Xl1SlSk1XkP˜Xl1SlKM2ε|k|αklε2|l|=KM2(αε2)klε2l2k+|k|+2|l|KM2(αε2)klεlk+3|l|KM2(αε2)klε3|l|,kl.

A similar argument shows that

(3.9) YkQ˜Yl1KM2(1αε2)klε3|l|,kl.

Form (3.8) and (3.9), it is easy to see that system (3.1) admits a nonuniform exponential dichotomy. Clearly, the rank of the projector is N1.

Lemma 3.8

Assume that the systems (1.1) and (3.1) are weakly kinematically similar via Sk. If for a constant γ ∈ ℝ+ the system (2.1) admits a nonuniform exponential dichotomy with constants K > 0, 0 < α < 1, ε ≥ 1 and invariant projector P, then the system

(3.10) yk+1=1γBkyk

also admits a nonuniform exponential dichotomy.

Proof. Obviously, P is also an invariant projector for (1.1). The dichotomy estimates are equivalent to

XkPXl1Kαklε|l|,kl,

and

XkPXl1K(1α)klε|l|,kl.

Using Lemma 3.7, it is easy to see that

YkPYl1Kγ(εα)klε|l|,kl,

and

YkPYl1Kγ(1εα)klε|l|,kl,

for some constant Kγ ≥ 1. Therefore, (3.10) admits a nonuniform exponential dichotomy.

The following result follows directly from Lemma 3.8.

Corollary 3.9

Assume that there exists a weakly non-degenerate transformation Sk such that AkwBk . Then ΣNED(A) = ΣNED(B), i.e.,

ΣNED(A)=a1,b1 or 0,b1a2,b2an1,bn1an,bn or an,=ΣNED(B).

The following theorem states that if (1.1) admits a nonuniform exponential dichotomy, then there exists a weakly non-degenerate transformation such that AkwBk and Bk has the block form (3.3), i.e., system (1.1) is reducible.

Theorem 3.10

Assume that (1.1) admits a nonuniform exponential dichotomy (not necessary ) of the form (3.4)-(3.5) with the invariant projector satisfying Pk≠0, Id. Then (1.1) is reducible. More precisely, it is weakly kinematically similar to a decoupled system

(3.11) xk+1=Bk100Bk2xk

for some matrix functions

B1:ZRN1×N1andB2:ZRN2×N2

where N 1 := dim im P ~ and N2:=dimkerP˜ .

Proof. Since equation (1.1) admits a nonuniform exponential dichotomy of the form (1.4)-(1.5) with the invariant projector satisfying Pk≠0, Id, by Lemma 3.6, one can choose a suitable fundamental matrix Xk and the projector P˜=IN1000 , (0 < N1<N) such that the estimates (3.4)-(3.5) hold. By Lemma 3.2 and the estimates (3.4)-(3.5), there exists an M = M(ε)>0 large enough such that

Sk2Mε|k|,Sk1XkP˜Xk12+Xk(IdP˜)Xk12122Kε|k|.

Thus, S is weakly non-degenerate. Setting

Bk=Rk+1Rk1,

where Rk is defined in Lemma 3.2 and Xk = SkRk. Obviously, Rk is the fundamental matrix of the linear system

yk+1=Bkyk.

Now we need to show that AkwBk and Bk has the block diagonal form

Bk=Bk100Bk2,forkZ.

First, we show that AkwBk . In fact,

Sk+1Bk=Xk+1Rk+11Bk=AkXkRk1Bk1Bk=AkSk,

which implies that AkwBk .

Now we show that system (1.1) is weakly kinematically similar to (3.11). By Lemma 3.2, Rk+1 and Rk1 commute with the matrix P˜ for every kZ . It follows that

(3.12) P˜Bk=BkP˜

for all kZ . Now we decompose B k : Z R N × N into four functions

Bk1:ZRN1×N1,Bk2:ZRN2×N2,Bk3:ZRN1×N2,Bk4:ZRN2×N1,

with

Bk=Bk1Bk3Bk4Bk2,kZ.

Identity (3.12) implies that

Bk1Bk300=Bk10Bk40,kZ.

Therefore Bk30 and Bk40 . Thus Bk has the block form

Bk=Bk100Bk2,kZ.

Now the proof is finished.

From Theorem 3.10, we know that if (1.1) admits a nonuniform exponential dichotomy, then there exists a weakly non-degenerate transformation Sk such that AkwBk and Bk has two blocks of the form (3.3). Now we are in a position to prove the reducibility result.

Theorem 3.11

Assume that (1.1) admits a nonuniform exponential dichotomy. Due to Theorem 2.6, the dichotomy spectrum is either empty or the disjoint union of n closed spectral intervals J1, ⋅, Jn with 1 ≤ N ≤ N, i.e.,

ΣNED(A)=(n=0) or ΣNED(A)=J1Jn.

Then there exists a weakly kinematic similarity action S : Z R N × N between (1.1) and a block diagonal system

xk+1=Bk0Bkn+1xk

with B i : Z R N i × N i , Ni = dim𝒲i, and

ΣNEDB0=,ΣNEDB1=J1,,ΣNEDBn=Jn,ΣNEDBn+1=.

Proof. If for any γ ∈ ℝ+, system (2.1) admits a nonuniform exponential dichotomy, then ΣNED(A) = ∅. Conversely, for any γ ∈ ℝ+, system (2.1) does not admit a nonuniform exponential dichotomy, then ΣNED(A) = ℝ+. Now, we prove the theorem for the nontrivial case (ΣNED(A)≠∅ and ΣNED(A)≠ℝ+).

Recall that the resolvent set ρNED(A) is open and therefore the dichotomy spectrum ΣNED(A) is the disjoint union of closed intervals. Using Theorem 2.6, we can assume

J1=a1,b1 or 0,b1,J2=a2,b2,,Jn1=an1,bn1,Jn=an,bn or an,

with 0 < a1b1 < a2b2 < … < anbn.

If J1 = [a1, b1] is a spectral interval, then (0, γ0) ⊂ ρNED(A) and W 0 = S γ 0 for some γ0 < a1 due to Theorem 2.6, which implies that

xk+1=1γ0Akxk

admits a nonuniform exponential dichotomy, let its invariant projector be denoted by P˜0 . By Theorem 3.10 and Corollary 3.9, there exists a weakly non-degenerate transformation xk=Sk0xk(0) with Sk0M0ε|k| and (Sk0)1M0ε|k| for some positive constant M0 = M0(ε) and such that AkwAk0 and Ak0 has two blocks of the form Ak0=Bk000Bk0, with dim B k 0 = d i m i m P ~ 0 = dim S γ 0 = dim W 0 =: N 0 due to Theorem 3.10, Lemma 2.5 and Theorem 2.6. If J1 = (0, b1] is a spectral interval, a block Bk0 is omitted.

Now we consider the following system

xk+1(0)=Ak0xk(0)=Bk000Bk0,xk(0).

By using Lemma 2.5, we take γ1 ∈ (b1, a2). In view of (b1,a2)ρNED(Bk0,) , γ1ρNED(Bk0,) , which implies that

xk+1(0)=1γ1Bk000Bk0,xk(0)

admits a nonuniform exponential dichotomy. Its invariant projector P˜1 satisfies P˜10,I . Similarly, by Theorem 3.10 and Corollary 3.9, there exists a weakly non-degenerate transformation

xk(0)=Sk1xk(1)=IN000S˜k1xk(1)

with S˜k1M1ε|k| and (S˜k1)1M1ε|k| for some positive constant M1 = M1(ε) and such that Bk0,wB˜k0, and B˜k0, has two blocks of the form B˜k0,=Bk100Bk1, with dim B k 1 = dim im P ~ 1 = dim S γ 1 dim ( U γ 0 S γ 1 ) = dim W 1 =: N 1 due to Theorem 3.10, Lemma 2.5 and Theorem 2.6. In addition, using Theorem 3.10 and Corollary 3.9, we have

ΣNEDBk1=a1,b1 or 0,b1,ΣNEDBk1,=a2,b2an1,bn1an,bn or an,.

Now we can construct a weakly non-degenerate transformation xk=S˜kxk(1) with S˜k=Sk0Sk1=Sk0IN000S˜k1 , where S˜kM0M1ε2|k| and S˜k1M0M1ε2|k| . Then AkwAk1 and Ak1 has three blocks of the form

Ak1=Bk0Bk1Bk1,.

Applying similar procedures to γ2 ∈ (b2, a3), γ3 ∈ (b3, a4), …, we can construct a weakly non-degenerate transformation xk=Skxk(n+1) with

Sk=Sk0IN000S˜k1IN0+N100S˜k2IN0++Nn100S˜kn

such that ∣ Sk∣ ≤ Mε εnk and Sk1Mεεn|k| with Mε = M0  ×  ···  ×  Mn. Now we can prove

AkwAkn:=Bk=Bk0Bkn+1

with locally integrable functions B i : Z R N i × N i and

ΣNEDB0=,ΣNEDB1=J1,,ΣNEDBn=Jn,ΣNEDBn+1=.

Finally, we show that Ni = dim𝒲i. From the claim above, we note that dim B k 0 = dim W 0 , dim B k 1 dim W 1 , , dim B k n dim W n , dim B k n + 1 = dim W n + 1 and using Theorem 2.6 this yields dim𝒲0 +···+dim𝒲n+1 = N, so dim B k i = dim W i for i = 0, …, n + 1. Now the proof is finished.

References

[1] B. Aulbach, The fundamental existence theorem on invariant fiber bundles, J. Difference Equ. Appl. 3 (1998), 267-312.10.1080/10236199708808118Search in Google Scholar

[2] B. Aulbach, N. V. Minh, P. P. Zabreiko, The concept of spectral dichotomy for linear difference equations, J. Math. Anal. Appl. 185 (1994), 275-287.10.1006/jmaa.1994.1248Search in Google Scholar

[3] B. Aulbach, N. V. Minh, The concept of spectral dichotomy for linear difference equations II, J. Difference Equ. Appl. 2 (1996), 251-262.10.1080/10236199608808060Search in Google Scholar

[4] B. Aulbach, S. Siegmund, A spectral theory for nonautonomous difference equations, New trends in difference equations (Temuco, 2000), 45-55, Taylor & Francis, London, 2002.Search in Google Scholar

[5] L. Barreira, Ya. Pesin, Lyapunov Exponents and Smooth Ergodic Theory, University Lecture Series 23, Amer. Math. Soc. 2002.10.1090/ulect/023Search in Google Scholar

[6] L. Barreira, C. Valls, Stability of Nonautonomous Differential Equations, Lecture Notes in Mathematics, vol. 1926, Springer, 2008.Search in Google Scholar

[7] L. Barreira, D. Dragičević, C. Valls, Nonuniform spectrum on Banach spaces, Adv. Math. 321 (2017), 547-591.10.1016/j.aim.2017.10.006Search in Google Scholar

[8] L. Barreira, C. Valls, Spectral theory for invertible cocycles under nonuniform hyperbolicity, São Paulo J. Math. Sci. 12 (2018), 6-17.10.1007/s40863-017-0070-zSearch in Google Scholar

[9] A. Berger, T.S. Doan, S. Siegmund, A definition of spectrum for differential equations on finite time, J. Differential Equations, 246 (2009), 1098-1118.10.1016/j.jde.2008.06.036Search in Google Scholar

[10] A. Carvalho, J. Langa, J. Robinson, Attractors for infinite-dimensional non-autonomous dynamical systems, Springer, 2013.10.1007/978-1-4614-4581-4Search in Google Scholar

[11] A. Castañeda, I. Huerta, Nonuniform almost reducibility of nonautonomous linear differential equations, J. Math. Anal. Appl. 485 (2020), 123822, 22 pp.10.1016/j.jmaa.2019.123822Search in Google Scholar

[12] A. Castañeda, G. Robledo, Dichotomy spectrum and almost topological conjugacy on nonautonomus unbounded difference systems, Discrete Contin. Dyn. Syst. 38 (2018), 2287-2304.10.3934/dcds.2018094Search in Google Scholar

[13] S. N. Chow, H. Leiva, Dynamical spectrum for time dependent linear systems in Banach spaces, Japan J. Indust. Appl. Math. 11 (1994), 379-415.10.1007/BF03167229Search in Google Scholar

[14] J. Chu, F. Liao, S. Siegmund, Y. Xia, W. Zhang, Nonuniform dichotomy spectrum and reducibility for nonautonomous equations, Bull. Sci. Math. 139 (2015), 538-557.10.1016/j.bulsci.2014.11.002Search in Google Scholar

[15] W. A. Coppel, Dichotomies and reducibility, J. Differential Equations, 3 (1967), 500-521.10.1007/BFb0067785Search in Google Scholar

[16] W. A. Coppel, Dichotomy in stability theory, Lecture Notes in Mathematics, Vol. 629, Springer-Verlag, New York/Berlin, 1978.10.1007/BFb0067780Search in Google Scholar

[17] T. S. Doan, D. Karrasch, T. Y. Nguyen, S. Siegmund, A unified approach to finite-time hyperbolicity which extends finite-time Lyapunov exponents, J. Differential Equations, 252 (2012), 5535-5554.10.1016/j.jde.2012.02.002Search in Google Scholar

[18] T. S. Doan, K. J. Palmer, M. Rasmussen, The Bohl spectrum for linear nonautonomous differential equations, J. Dynam. Differential Equations 29 (2017), 1459-1485.10.1007/s10884-016-9530-xSearch in Google Scholar PubMed PubMed Central

[19] I. Gohberg, M. A. Kaashoek, J. Kos, Classification of linear time-varying difference equations under kinematic similarity, Integral Equations Operator Theory, 25 (1996), 445-480.10.1007/BF01203027Search in Google Scholar

[20] W. Li, J. Llibre, H. Wu, Polynomial and linearized normal forms for almost periodic difference systems, J. Difference Equ. Appl. 15 (2009), 927-948.10.1080/10236190802284848Search in Google Scholar

[21] W. Li, J. Llibre, H. Wu, Normal forms for almost periodic differential systems, Ergodic Theory Dynam. Systems 29 (2009), 637-656.10.1017/S0143385708080401Search in Google Scholar

[22] J. Massera, J. Schäffer, Linear differential equations and function spaces, in: Pure and Applied Mathematics, vol. 21, Academic Press, 1966.Search in Google Scholar

[23] D. C. Nguyen, S. Siegmund, Dichotomy spectrum of nonautonomous linear stochastic differential equations, Stoch. Dyn. 2 (2002), 175-201.10.1142/S0219493702000364Search in Google Scholar

[24] K. J. Palmer, On the reducibility of almost periodic systems of linear differential equations, J. Differential Equations, 36 (1980), 374-390.10.1016/0022-0396(80)90056-XSearch in Google Scholar

[25] O. Perron, Die Stabilitätsfrage bei Differentialgleichungen, Math. Z. 32 (1930), 703-728.10.1007/BF01194662Search in Google Scholar

[26] C. Pötzsche, A note on the dichotomy spectrum, J. Difference Equ. Appl. 15 (2009), 1021-1025.10.1080/10236190802320147Search in Google Scholar

[27] C. Pötzsche, Fine structure of the dichotomy spectrum, Integral Equations Operator Theory, 73 (2012), 107-151.10.1007/s00020-012-1959-7Search in Google Scholar

[28] R. Sacker, G. Sell, Existence of dichotomies and invariant splitting for linear differential systems I [II, III], J. Differential Equations, 15 (1974), 429-458 [22 (1976), 478-496, 497-522].10.1016/0022-0396(76)90042-5Search in Google Scholar

[29] R. J. Sacker, G. R. Sell, A spectral theory for linear differential systems, J. Differential Equations, 27 (1978), 320-358.10.1016/0022-0396(78)90057-8Search in Google Scholar

[30] S. Siegmund, Spektral-Theorie, glatte Faserungen und Normalformen für Differentialgleichungen vom Carathéodory-Typ, Dissertation, Augsburger Mathematisch-Naturwissenschaftliche Schriften 30, Wiϐner Verlag, Augsburg, 1999.Search in Google Scholar

[31] S. Siegmund, Dichotomy spectrum for nonautonomous differential equations, J. Dynam. Differential Equations, 14 (2002), 243-258.10.1023/A:1012919512399Search in Google Scholar

[32] S. Siegmund, Reducibility of nonautonomous linear differential equations, J. London Math. Soc. 65 (2002), 397-410.10.1112/S0024610701002897Search in Google Scholar

[33] H. Wu, W. Li, Poincaré type theorems for non-autonomous systems, J. Differential Equations, 245 (2008), 2958-2978.10.1016/j.jde.2008.05.005Search in Google Scholar

[34] Y. Xia, Y. Bai, D. O'Regan, A new method to prove the nonuniform dichotomy spectrum theorem in ℝn, Proc. Amer. Math. Soc. 147 (2019), 3905-3917.10.1090/proc/14535Search in Google Scholar

[35] X. Zhang, Nonuniform dichotomy spectrum and normal forms for nonautonomous differential systems, J. Funct. Anal. 267 (2014), 1889-1916.10.1016/j.jfa.2014.07.029Search in Google Scholar

Received: 2021-03-22
Accepted: 2021-06-15
Published Online: 2021-07-24

© 2021 Jifeng Chu et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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