Complexity

Complexity / 2017 / Article

Research Article | Open Access

Volume 2017 |Article ID 9878369 | https://doi.org/10.1155/2017/9878369

Yongkun Li, Xiaofang Meng, "Existence and Global Exponential Stability of Pseudo Almost Periodic Solutions for Neutral Type Quaternion-Valued Neural Networks with Delays in the Leakage Term on Time Scales", Complexity, vol. 2017, Article ID 9878369, 15 pages, 2017. https://doi.org/10.1155/2017/9878369

Existence and Global Exponential Stability of Pseudo Almost Periodic Solutions for Neutral Type Quaternion-Valued Neural Networks with Delays in the Leakage Term on Time Scales

Academic Editor: Sigurdur F. Hafstein
Received10 Sep 2017
Accepted22 Nov 2017
Published26 Dec 2017

Abstract

We propose a class of neutral type quaternion-valued neural networks with delays in the leakage term on time scales that can unify the discrete-time and the continuous-time neural networks. In order to avoid the difficulty brought by the noncommutativity of quaternion multiplication, we first decompose the quaternion-valued system into four real-valued systems. Then, by applying the exponential dichotomic theory of linear dynamic equations on time scales, Banach’s fixed point theorem, the theory of calculus on time scales, and inequality techniques, we obtain some sufficient conditions on the existence and global exponential stability of pseudo almost periodic solutions for this class of neural networks. Our results are completely new even for both the case of the neural networks governed by differential equations and the case of the neural networks governed by difference equations and show that, under a simple condition, the continuous-time quaternion-valued network and its corresponding discrete-time quaternion-valued network have the same dynamical behavior for the pseudo almost periodicity. Finally, a numerical example is given to illustrate the feasibility of our results.

1. Introduction

The quaternion, which was discovered by the Irish mathematician Hamilton [1] in order to generalize complex number properties to multidimensional space, is extensively used in several fields, such as modern mathematics, physics, and computer graphics [24]. One of the advantages by the use of quaternions is that it can treat and operate three- or four-dimensional vectors as one entity, which allows a significant decrease of computational complexity in three- or four-dimensional problems, so the effective information processing can be achieved by the operations for quaternionic variables. Therefore, the quaternion-valued neural network is able to cope with multidimensional issues more efficiently by employing quaternion directly.

In this respect, the quaternion-valued neural network is a fast growing field of research in both theoretical and application points of view (see [59]). Quaternion neural networks have been widely used in many fields and demonstrated better performances than the real number neural networks in chaotic time series prediction [10], approximate quaternion-valued functions [11], 3D wind forecasting [12, 13], image processing [14, 15], color-face recognition [16], vector sensor processing [17], and so on.

In reality, it is well known that the time delay is inevitable. In the circuit implementation of neural networks, time delays occur naturally due to the processing and transmission of signals in the network and the finite switching speed of amplifiers. And they may change the dynamical behaviors of considered neural networks. Therefore, the consideration of time delays is more and more significant in the study of the dynamics of neural networks.

Many scholars have devoted themselves into the dynamics analysis of neural networks with various types of time delays and many valuable results have been achieved in the existing literature see [1826]. There are three typical types of time delays for incorporating time delays into neural networks: (i) introduce transmission delays into the neural networks, and consider discrete delays, distributed delays, mixed delays, even state depended delays, or complex delays; (ii) consider the delays in the leakage term; (iii) take into account neutral type delays. All of the above three types of time delays may alter the dynamics of the neural network under consideration.

On the one hand, the concept of pseudo-almost periodicity was introduced by Zhang [27, 28] in the early 1990s. It quickly aroused the interest of some mathematical researchers [2931]. The pseudo almost periodicity is more general and complicated than the periodicity and the almost periodicity. In the last few years, the pseudo almost periodicity has become a hot research topic, especially for the pseudo almost periodic oscillation of neural networks [3239].

On the other hand, as it is known, both continuous-time and discrete-time neural networks are important in theocratic studies and applications. Moreover, discrete-time neural networks are more convenient for computation and numerical simulation than continuous-time neural networks. Therefore, we must not only study continuous-time neural networks, but also study discrete-time neural networks. Fortunately, the theory of time scales, which was initiated by Hilger [40] in his Ph.D. thesis in 1988, can unify the continuous and discrete cases. Studying dynamic equations on time scales can unify the differential equation case and the difference equation case. In recent years, the time scale theory has been widely concerned and rapidly developed [4145]. And, many authors have studied the dynamical behavior of neural networks on time scales [4654].

However, to the best of our knowledge, there is no paper published on the existence and stability of pseudo almost periodic solutions of quaternion-valued neural networks on time scales. This is important in theory and application, and it is also a very challenging issue.

Motivated by the above statement, in this paper, we propose the following neutral type quaternion-valued neural network with delays in the leakage term on time scales:where is an almost periodic time scale, is the state of the th neuron at time ; is the self-feedback connection weight, denotes the set of all quaternion-valued functions defined on time scale ; and are the delay connection weight and the neutral delay connection weight from neuron to neuron at time , respectively; is an external input on the th unit at time ; denotes the leakage delay satisfying for ; and are transmission delays satisfying and for .

The initial condition of system (1) is of the form where , , , , .

Throughout this paper, we denote . For convenience, for an rd-continuous pseudo almost periodic function , we denote and .

Our main purpose of this paper is to study the existence and global exponential stability of pseudo almost periodic solutions of (1). Our results are completely new even for both the case of the neural networks governed by quaternion-valued differential equations and the case of the neural networks governed by quaternion-valued difference equations.

The rest of this paper is organized as follows. In Section 2, we introduce some definitions and preliminary lemmas and transform the quaternion-valued system (1) into four real-valued systems. In Section 3, we establish some sufficient conditions for the existence and global exponential stability of pseudo almost periodic solutions of (1). In Section 4, we give an example to demonstrate the feasibility of our results. This paper ends with a brief conclusion in Section 5.

2. Preliminaries

In this section, we shall first recall some fundamental definitions, lemmas which are used in what follows.

The skew field of quaternions is denoted by where , , , and are real numbers and the elements , , and obey Hamilton’s multiplication rules: The quaternion conjugate is defined by , and the norm of is defined as .

A time scale is an arbitrary nonempty closed subset of the real set with the topology and ordering inherited from . The forward jump operator is defined by , , while the backward jump operator is defined by , , and the graininess function is defined by .

The point is called left-dense, left-scattered, right-dense, or right-scattered if , , , or , respectively. Points that are right-dense and left-dense at the same time are called dense. If has a left-scattered maximum , define ; otherwise, set . If has a right-scattered maximum , define ; otherwise, set .

Assume that is a function and let . Then we define to be the number (provided its exists) with the property that, given any , there is a neighborhood of such thatfor all . We call the delta derivative of at . Moreover, we say that is delta differentiable on provided that exists for all .

By writing in the form of with , , it is easy to verify that is delta differentiable if and only if , , , are delta differentiable. Moreover, if is delta differentiable, then

A function is said to be regressive provided for all The set of all regressive and rd-continuous functions is denoted by . We define for all . For more knowledge about calculus on time scales, we refer to [41, 42].

Definition 1 (see [47]). A time scale is called an almost periodic time scale if

Definition 2 (see [47]). Let be an almost periodic time scale. A function is called an almost periodic on if for any given , there exists a constant such that each interval of length contains at least one such that

Let be almost and denote the space of all bounded continuous functions from to .

Similar to Definition   in [55], we introduce the following definition.

Definition 3. A function is called pseudo almost periodic if , where and is -measurable such that , where .

We denote by the set of all pseudo almost periodic functions defined on .

Lemma 4 (see [56]). If , then ; if , , then .

Similar to the proof of Lemma   in [56], one can show the following.

Lemma 5. If satisfies the Lipschitz condition, , , and , then .

Definition 6. Function is called pseudo almost periodic if for each , is pseudo almost periodic.

Definition 7 (see [47]). Let be an matrix-valued function on . Then the linear systemis said to admit an exponential dichotomy on if there exist positive constant , , projection , and the fundamental solution matrix of (9), satisfying

Consider the following pseudo almost periodic system:where is an almost periodic matrix function and is a pseudo almost periodic vector function.

Lemma 8 (see [47]). If the linear system (9) admits an exponential dichotomy, then the pseudo almost periodic system (11) has a unique pseudo almost periodic solution as follows: where is the fundamental solution matrix of (9).

Lemma 9 (see [46]). Let be an almost periodic function, , , , and ; then the linear system admits an exponential dichotomy on .

Throughout the rest of this paper, we assume the following:Let , where . Then and can be expressed as

By , we can transform system (1) into the following four real-valued systems: According to (15), we can getwhere

The initial condition associated with (17) is of the form where , .

Remark 10. It is obvious that if , is a solution to system (17), then where , must be a solution to (1). Thus, the problem of finding a pseudo almost periodic solution for (1) reduces to finding one for system (17). For considering the stability of solutions of (1), we just need to consider the stability of solutions of system (17).

3. Main Results

In this section, we will study the existence and global exponential stability of pseudo almost periodic solutions of system (17).

Let with the norm , where , ; then is a Banach space.

Throughout this paper, we assume that the following conditions hold: with is an almost periodic function, , , , , , .Functions and there exist positive constants such that for all and , .There exists a positive constant such that where

Theorem 11. Assume that ()–() hold; then system (17) has a unique pseudo almost periodic solution in the region .

Proof. System (17) can be written as For any , consider the linear dynamic systemSince and , it follows from Lemma 9 that the linear system admits an exponential dichotomy on . Thus, by Lemma 8, we see that system (25) has exactly one pseudo almost periodic solution which can be expressed as follows:Now, we define the operator aswhere , is defined by (27), .
First, we show that, for any , we have . From (27), we haveIn a similar way, we haveOn the other hand, we haveIn a similar way, we haveIt follows from (29) to (32) and that which implies that , so the mapping is a self-mapping from to . Next, we shall prove that is a contraction mapping. In fact, for any , we have