Abstract

Exponential periodic attractor of impulsive Hopfield-type neural network system with piecewise constant argument

Highlights

  • CNNs models of the mixed type impulsive differential equation (IDE)-DEPCA can be found in the mathematical literature of the last decades [5, 8, 13, 56, 57]

  • In [25], the same author investigated some sufficient conditions for the existence, uniqueness and globally exponentially stability of solutions of the following IDEPCAG system with alternately retarded and advanced piecewise constant argument:

  • In this work we have obtained some sufficient conditions for the existence, uniqueness, periodicity and stability of solutions for the impulsive Hopfield-type neural network system with piecewise constant arguments (1.2)

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Summary

Introduction

U. Akhmet considers the equation x (t) = f (t, x(t), x(γ(t))), where γ(t) is a piecewise constant argument of generalized type, that is, given (tk)k∈Z and (ζk)k∈Z such that tk < tk+1 , ∀k ∈ Z with limk→±∞ tk = ±∞ and tk ≤ ζk ≤ tk+1, if t ∈ Ik = [tk, tk+1) , γ(t) = ζk. These equations are called Differential Equations with Piecewise Constant Argument of Generalized Type (in short DEPCAG) They have continuous solutions, even when γ(t) is not, producing a recursive law on tk i.e., a discrete equation. For instance we distinguish between discrete and continuous models, when the time is considered as discrete or a continuous variable, respectively Another general classification is given by the dynamics of the cells by considering the deterministic or probabilistic behavior. CNNs models of the mixed type IDE-DEPCA can be found in the mathematical literature of the last decades [5, 8, 13, 56, 57]

Cellular neural networks with piecewise constant argument
Aim of the paper
General assumptions
A useful Gronwall type result
Green function
Global Lipschitz condition
Local Lipschitz condition
Exponential attraction
The constant coefficients case and simulations
Exponentially global convergence of periodic solutions
Simulation for the constant coefficients case
Equilibrium
Nonzero linear impulse
Simulation for the non-constant coefficients case
Conclusions
Full Text
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