Abstract and Applied Analysis

Volume 2012, Article ID 613038, 14 pages

http://dx.doi.org/10.1155/2012/613038

## A Generalized Nonuniform Contraction and Lyapunov Function

^{1}Nanjing College of Information Technology, Nanjing 210046, China^{2}Department of Mathematics, College of Science, Hohai University, Nanjing 210098, China

Received 19 November 2012; Accepted 1 December 2012

Academic Editor: Juntao Sun

Copyright © 2012 Fang-fang Liao et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

For nonautonomous linear equations , we give a complete characterization of general nonuniform contractions in terms of Lyapunov functions. We consider the general case of nonuniform contractions, which corresponds to the existence of what we call nonuniform -contractions. As an application, we establish the robustness of the nonuniform contraction under sufficiently small linear perturbations. Moreover, we show that the stability of a nonuniform contraction persists under sufficiently small nonlinear perturbations.

#### 1. Introduction

We consider nonautonomous linear equations where is a continuous function with values in the space of bounded linear operators in a Banach space . Our main aim is to characterize the existence of a general nonuniform contraction for (1.1) in terms of Lyapunov functions.

We assume that each solution of (1.1) is global, and we denote the corresponding evolution operator by , which is the linear operator such that
for any solution of (1.1). Clearly, and
We shall say that an increasing function is a *growth rate* if
Given two growth rates , we say that (1.1) admits a *nonuniform **-contraction* if there exist constants and such that
We emphasize that the notion of nonuniform -contraction often occurs under reasonably weak assumptions. We refer the reader to [1] for details.

In this work, we mainly consider more general nonuniform contractions (see (2.1) below) and we give a complete characterization of such contractions in terms of Lyapunov functions, especially in terms of quadratic Lyapunov functions, which are Lyapunov functions defined in terms of quadratic forms. The importance of Lyapunov functions is well established, particularly in the study of the stability of trajectories both under linear and nonlinear perturbations. This study goes back to the seminal work of Lyapunov in his 1892 thesis [2]. For more results, we refer the reader to [3–6] for the classical exponential contractions and dichotomies, [7–9] for the nonuniform exponential contractions and nonuniform exponential dichotomies.

The proof of this paper follows from the ideas in [9, 10]. As an application, we provide a very direct proof of the robustness of the nonuniform contraction, that is, of the persistence of the nonuniform contraction in the equation for any sufficiently small linear perturbation . We remark that the so-called robustness problem also has a long history. In particular, the problem was discussed by Massera and Schäffer [11], Perron [12], Coppel [3] and in the case of Banach spaces by Daletskiĭ and Kreĭn [13]. For more recent work we refer to [14–16] and the references therein.

Furthermore, for a large class of nonlinear perturbations with for every , we show that if (1.1) admits a nonuniform contraction, then the zero solution of the equation is stable. The proof uses the corresponding characterization between the nonuniform contractions and quadratic Lyapunov functions.

#### 2. Lyapunov Functions and Nonuniform Contractions

Given a growth rate and a function , we say that (1.1) admits a *nonuniform **-contraction* if there exists a constant such that
The nonuniform -contraction is a special case of nonuniform -contraction with .

Now we introduce the notion of Lyapunov functions. We say that a continuous function is a *strict Lyapunov function* to (1.1) if (1)for every and ,
(2)for every and ,
(3)there exists a constant such that for every and ,

The following result gives an optimal characterization of nonuniform -contractions in terms of strict Lyapunov functions.

Theorem 2.1. *(1.1) admits a nonuniform -contraction if and only if there exists a strict Lyapunov function for (1.1). *

*Proof. *We assume that there exists a strict Lyapunov function for (1.1). By and , for every and , we have
Therefore, (1.1) admits a nonuniform -contraction with .

Next we assume that (1.1) admits a nonuniform -contraction. For and , we set
By (2.1), we have . Moreover, setting , we obtain . This establishes . Furthermore, for , we have
Therefore, is a strict Lyapunov function for (1.1).

Next we consider another class of Lyapunov functions, namely, those defined in terms of quadratic forms.

Let be a symmetric positive-definite operator for each . A *quadratic Lyapunov function * is given as
Given linear operators , we write if for .

Theorem 2.2. *Assume that there exist constants and such that
**
Then (1.1) admits a nonuniform -contraction (up to a multiplicative constant) if and only if there exist symmetric positive definite operators and constants such that is of class in and
*

*Proof. *We first assume that (1.1) admits a nonuniform -contraction. Consider the linear operators
for some constant . Clearly, is symmetric for each . Moreover, by (2.8), we have
Since is symmetric, we obtain
and therefore (2.10) holds. Since
we find that is of class in with derivative
which implies that
Therefore,
which establishes (2.11) with .

Now we assume that conditions (2.9) and (2.10)-(2.11) hold. Set . By (2.10), we have

Lemma 2.3.* There exists a constant ** such that**Proof of Lemma 2.3.* Note that
Hence, by condition (2.11), and the fact that we obtain
Now given , take such that with as in (2.9). Then
It follows from (2.9) that
Since , we have
which yields (2.20) with .

Lemma 2.4.* For *,* one has**Proof of Lemma 2.4.* By conditions (2.11) and (2.21), we have
Therefore,
It follows from Gronwall’s lemma that
which yields the desired result.

By Lemmas 2.3 and 2.4 together with (2.19), we obtain
and therefore,
which implies that (1.1) admits a nonuniform -contraction.

As an application of Theorem 2.2, we establish the robustness of nonuniform -contractions. Roughly speaking, a nonuniform contraction for (1.1) is said to be *robust* if (1.6) still admits a nonuniform contraction for any sufficiently small perturbation .

**Theorem 2.5.*** Let ** be continuous functions such that *(1.1) *admits a nonuniform **-contraction with condition* (2.9). *Suppose further that ** for every ** and**for some ** sufficiently small. Then *(1.6) *admits a nonuniform **-contraction. *

*Proof. *Let be the evolution operator associated to (1.6). It is easy to verify that
For every with , we have
Using Gronwall’s inequality, we obtain
for every with . Therefore condition (2.9) also holds for the perturbed equation (1.6).

Now we consider the matrices in (2.12). Condition (2.10) can be obtained as in the proof of Theorem 2.2. For condition (2.11), it is sufficient to show that
for some constant . Using (2.10) and (2.32), we have
and taking sufficiently small, we find that (2.36) holds with some .

#### 3. Stability of Nonlinear Perturbations

Before stating the result, we fist prove an equivalent characterization of property . Given matrices for each , we consider the functions whenever the derivatives are well defined and are given as (2.8).

Lemma 3.1. *Let be functions. Then property is equivalent to
*

*Proof. *Now we assume that property holds. If and , then
Similarly, if is such that , then
This establishes (3.2).

Next we assume that (3.2) holds. We rewrite (3.2) in the form
which implies that
and hence property holds.

Theorem 3.2. *Assume that (1.1) admits a nonuniform -contraction satisfying (2.9). Suppose further that there exists a constant such that and
**
Then for each , there exists such that
**
for every solution of (1.7). *

*Proof. *For as in (2.12) and as in (2.8), we have, for every ,
Since , we have
Applying Lemma 3.1, we obtain
In particular, for ,
From the identity that for every and , we have
On the other hand,
Therefore,
and hence
Therefore, if is a solution of (1.7), then
If is small enough such that , then
and hence
It follows from Gronwall’s inequality that
Now given , take such that with as in (2.9). Then
Taking
then
It follows from (2.13) and (3.20) that
Now the proof is finished.

#### Acknowledgments

The authors would like to deliver great thanks to Professor Jifeng Chu for his valuable suggestions and comments. Y. Jiang was supported by the Fundamental Research Funds for the Central Universities.

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