Asymptotic Stability of Impulsive Cellular Neural Networks with Infinite Delays via Fixed Point Theory
Abstract
We employ the new method of fixed point theory to study the stability of a class of impulsive cellular neural networks with infinite delays. Some novel and concise sufficient conditions are presented ensuring the existence and uniqueness of solution and the asymptotic stability of trivial equilibrium at the same time. These conditions are easily checked and do not require the boundedness and differentiability of delays.
1. Introduction
Cellular neural networks (CNNs), proposed by Chua and Yang in 1988 [1, 2], have become a hot topic for their numerous successful applications in various fields such as optimization, linear and nonlinear programming, associative memory, pattern recognition, and computer vision.
Due to the finite switching speed of neurons and amplifiers in the implementation of neural networks, it turns out that the time delays should not be neglected, and therefore, the model of delayed cellular neural networks (DCNNs) is put forward, which is naturally of better realistic significances. In fact, besides delay effects, stochastic and impulsive as well as diffusing effects are also likely to exist in neural networks. Accordingly many experts are showing a growing interest in the research on the dynamic behaviors of complex CNNs such as impulsive delayed reaction-diffusion CNNs and stochastic delayed reaction-diffusion CNNs, with a result of many achievements [3–9] obtained.
Synthesizing the reported results about complex CNNs, we find that the existing research methods for dealing with stability are mainly based on Lyapunov theory. However, we also notice that there are still lots of difficulties in the applications of corresponding results to specific problems; correspondingly it is necessary to seek some new techniques to overcome those difficulties.
Encouragingly, in recent few years, Burton and other authors have applied the fixed point theory to investigate the stability of deterministic systems and obtained some more applicable results; for example, see the monograph [10] and papers [11–22]. In addition, more recently, there have been a few publications where the fixed point theory is employed to deal with the stability of stochastic (delayed) differential equations; see [23–29]. Particularly, in [24–26], Luo used the fixed point theory to study the exponential stability of mild solutions to stochastic partial differential equations with bounded delays and with infinite delays. In [27, 28], Sakthivel used the fixed point theory to investigate the asymptotic stability in pth moment of mild solutions to nonlinear impulsive stochastic partial differential equations with bounded delays and with infinite delays. In [29], Luo used the fixed point theory to study the exponential stability of stochastic Volterra-Levin equations.
Naturally, for complex CNNs which have high application values, we wonder if we can utilize the fixed point theory to investigate their stability, not just the existence and uniqueness of solution. With this motivation, in the present paper, we aim to discuss the stability of impulsive CNNs with infinite delays via the fixed point theory. It is worth noting that our research skill is the contraction mapping theory which is different from the usual method of Lyapunov theory. We employ the fixed point theorem to prove the existence and uniqueness of solution and the asymptotic stability of trivial equilibrium all at once. Some new and concise algebraic criteria are provided, and these conditions are easy to verify and, moreover, do not require the boundedness and differentiability of delays.
2. Preliminaries
Let Rn denote the n-dimensional Euclidean space and let ∥·∥ represent the Euclidean norm. 𝒩≜{1,2, …, n}. R+ = [0, ∞). C[X, Y] corresponds to the space of continuous mappings from the topological space X to the topological space Y.
Throughout this paper, we always assume that fi(0) = gi(0) = Iik(0) = 0 for i ∈ 𝒩 and k = 1,2, …. Thereby, problem (1) and (2) admits a trivial equilibrium x = 0.
Definition 1. The trivial equilibrium x = 0 is said to be stable, if, for any ε > 0, there exists δ > 0 such that for any initial condition φ(s) ∈ C[[ϑ, 0], Rn] satisfying |φ| < δ:
Definition 2. The trivial equilibrium x = 0 is said to be asymptotically stable if the trivial equilibrium x = 0 is stable, and for any initial condition φ(s) ∈ C[[ϑ, 0], Rn], lim t→∞∥x(t; s, φ)∥ = 0 holds.
The consideration of this paper is based on the following fixed point theorem.
Theorem 3 (see [30].)Let Υ be a contraction operator on a complete metric space Θ, then there exists a unique point ζ ∈ Θ for which Υ(ζ) = ζ.
3. Main Results
- (A1)
There exist nonnegative constants lj such that, for any η, υ ∈ R,
() - (A2)
There exist nonnegative constants kj such that, for any η, υ ∈ R,
() - (A3)
There exist nonnegative constants pjk such that, for any η, υ ∈ R,
()
- (1)
ϕi(t) is continuous on t ≠ tk (k = 1,2, …);
- (2)
and exist; furthermore, for k = 1,2, …;
- (3)
ϕi(s) = φi(s) on s ∈ [ϑ, 0];
- (4)
ϕi(t) → 0 as t → ∞;
In what follows, we will give the main result of this paper.
Theorem 4. Assume that conditions (A1)–(A3) hold. Provided that
- (i)
there exists a constant μ such that inf k=1,2,…{tk − tk−1} ≥ μ,
- (ii)
there exist constants pi such that pik ≤ piμ for i ∈ 𝒩 and k = 1,2, …,
- (iii)
,
- (iv)
, where ,
Proof. Multiplying both sides of (1) with gives, for t > 0 and t ≠ tk,
Letting ε → 0 in (11), we have
Noting xi(tk − 0) = xi(tk), (14) can be rearranged as
Combining (12) and (15), we reach that
Note xi(0) = φi(0) in (19). We then define the following operator π acting on ℋ, for :
The subsequent part is the application of the contraction mapping principle, which can be divided into two steps.
Step 1. We need to prove π(ℋ) ⊂ ℋ. Choosing yi(t) ∈ ℋi (i ∈ 𝒩), it is necessary to testify π(yi)(t) ⊂ ℋi.
First, since π(yi)(s) = φi(s) on s ∈ [ϑ, 0] and φi(s) ∈ C[[ϑ, 0], R], we know π(yi)(s) is continuous on s ∈ [ϑ, 0]. For a fixed time t > 0, it follows from (21) that
Owing to yi(t) ∈ ℋi, we see that yi(t) is continuous on t ≠ tk (k = 1,2, …); moreover, and exist, and .
Consequently, when t ≠ tk (k = 1,2, …) in (22), it is easy to find that Qi → 0 as r → 0 for i = 1, …, 4, and so π(yi)(t) is continuous on the fixed time t ≠ tk (k = 1,2, …).
On the other hand, as t = tk (k = 1,2, …) in (22), it is not difficult to find that Qi → 0 as r → 0 for i = 1,2, 3. Furthermore, if letting r < 0 be small enough, we derive
According to the above discussion, we find that π(yi)(t) : [ϑ, ∞) → R is continuous on t ≠ tk (k = 1,2, …); moreover, and exist; in addition, .
Next, we will prove π(yi)(t) → 0 as t → ∞. For convenience, denote
Due to yj(t) ∈ ℋj (j ∈ 𝒩), we know lim t→∞yj(t) = 0. Then for any ε > 0, there exists a Tj > 0 such that t ≥ Tj implies |yj(t) | < ε. Choose T* = max j∈𝒩{Tj}. It is derived from (A1) that, for t ≥ T*,
On the other hand, since t − τj(t) → ∞ as t → ∞, we get lim t→∞yj(t − τj(t)) = 0. Then for any ε > 0, there also exists a such that implies |yj(s − τj(s))| < ε. Select . It follows from (A2) that
Furthermore, from (A3), we know that |Iik(yi(tk))| ≤ pik|yi(tk)|. So
As yi(t) ∈ ℋi, we have lim t→∞yi(t) = 0. Then for any ε > 0, there exists a nonimpulsive point Ti > 0 such that s ≥ Ti implies |yi(s)| < ε. It then follows from conditions (i) and (ii) that
From (30), (32), and (35), we deduce π(yi)(t) → 0 as t → ∞ for i ∈ 𝒩. We therefore conclude that π(yi)(t) ⊂ ℋi (i ∈ 𝒩) which means π(ℋ) ⊂ ℋ.
Step 2. We need to prove π is contractive. For and , we estimate
Note
It hence follows from (37) that
Therefore,
In view of condition (iii), we see π is a contraction mapping, and, thus there exists a unique fixed point of π in ℋ which means the transposition of is the vector-valued solution to (1)–(3) and its norm tends to zero as t → ∞.
To obtain the asymptotic stability, we still need to prove that the trivial equilibrium x = 0 is stable. For any ε > 0, from condition (iv), we can find δ satisfying 0 < δ < ε such that . Let |φ| < δ. According to what has been discussed above, we know that there exists a unique solution to (1)–(3); moreover,
Suppose there exists t* > 0 such that ∥x(t*; s, φ)∥ = ε and ∥x(t; s, φ)∥ < ε as 0 ≤ t < t*. It follows from (41) that
So . This contradicts the assumption of ∥x(t*; s, φ)∥ = ε. Therefore, ∥x(t; s, φ)∥ < ε holds for all t ≥ 0. This completes the proof.
Corollary 5. Assume that conditions (A1)–(A3) hold. Provided that
- (i)
inf k=1,2,…{tk − tk−1} ≥ 1,
- (ii)
there exist constants pi such that pik ≤ pi for i ∈ 𝒩 and k = 1,2, …,
- (iii)
,
- (iv)
, where ,
Remark 6. In Theorem 4, we can see it is the fixed point theory that deals with the existence and uniqueness of solution and the asymptotic analysis of trivial equilibrium at the same time, while Lyapunov method fails to do this.
Remark 7. The presented sufficient conditions in Theorems 4 and Corollary 5 do not require even the boundedness and differentiability of delays, let alone the monotone decreasing behavior of delays which is necessary in some relevant works.
Theorem 8. Assume that conditions (A1)-(A2) hold. Provided that
- (i)
,
- (ii)
, where ,
4. Example
5. Conclusions
This work is devoted to seeking new methods to investigate the stability of complex neural networks. From what has been discussed above, we find that the fixed point theory is feasible. With regard to a class of impulsive cellular neural networks with infinite delays, we utilize the contraction mapping principle to deal with the existence and uniqueness of solution and the asymptotic analysis of trivial equilibrium at the same time, for which Lyapunov method feels helpless. Now that there are different kinds of fixed point theorems and complex neural networks, our future work is to continue the study on the application of fixed point theory to the stability analysis of complex neural networks.
Acknowledgment
This work is supported by the National Natural Science Foundation of China under Grants 60904028, 61174077, and 41105057.