
Sustainable electricity supply plays a key role in economic development. Cost recovery, profitability and affordability of electricity through power tariff regulation, have become a subject of conflict between private providers and regulators. Consequently, regulators need to balance the interests of all stakeholders. The objective of this study, is to measure to which extent, Electricity Net Consumption (EC), Electricity Net Generation (EG), electricity transmission and distribution losses (Losses), International Average Crude oil prices (FP), Consumer Price Index (CPI), Industry Value Added (IVA) could influence the Average Electricity Prices (EP) in East Africa, especially in Rwanda, Uganda, Tanzania, Burundi, and Kenya. The data are from World Bank Indicators and cover the period from 2000 to 2019. This study adopts a three-stage approach, consisting of panel unit root tests, panel cointegration tests and estimating the long run cointegration relationship of the variables in a panel context. We applied four different panel unit root tests including ADF-Fisher Chi-square, Levin, Lin and Chu (LLC); PP-Fisher Chi-square, and Im, Pesaran, and Shin, (IPS). The results reveal that the variables are non-stationary at "level", stationary at first-differences and integrated with order one denoted as I(1). The Pedroni, Kao and Johansen Fisher co-integration tests were performed. This study uses full modified ordinary least squares (FMOLS) and dynamic ordinary least squares (DOLS) to estimate the long run relationship among the variables. We find that the increase in EG, FP, and CPI increase the Average Electricity Prices (EP); while the increase in Losses, EC, and IVA decreases EP. Therefore, we recommend the promotion of long-term investment policies in renewable sources and efficient policies to reduce technical and commercial losses. In addition, this study suggests that appropriate policies related to subsidized electricity prices would, however, prevent adverse effects related to inefficient over-consumption of electricity.
Citation: Mburamatare Daniel, William K. Gboney, Hakizimana Jean de Dieu, Akumuntu Joseph, Fidele Mutemberezi. Empirical assessment of drivers of electricity prices in East Africa: Panel data experience of Rwanda, Uganda, Tanzania, Burundi, and Kenya[J]. AIMS Energy, 2023, 11(1): 1-30. doi: 10.3934/energy.2023001
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Sustainable electricity supply plays a key role in economic development. Cost recovery, profitability and affordability of electricity through power tariff regulation, have become a subject of conflict between private providers and regulators. Consequently, regulators need to balance the interests of all stakeholders. The objective of this study, is to measure to which extent, Electricity Net Consumption (EC), Electricity Net Generation (EG), electricity transmission and distribution losses (Losses), International Average Crude oil prices (FP), Consumer Price Index (CPI), Industry Value Added (IVA) could influence the Average Electricity Prices (EP) in East Africa, especially in Rwanda, Uganda, Tanzania, Burundi, and Kenya. The data are from World Bank Indicators and cover the period from 2000 to 2019. This study adopts a three-stage approach, consisting of panel unit root tests, panel cointegration tests and estimating the long run cointegration relationship of the variables in a panel context. We applied four different panel unit root tests including ADF-Fisher Chi-square, Levin, Lin and Chu (LLC); PP-Fisher Chi-square, and Im, Pesaran, and Shin, (IPS). The results reveal that the variables are non-stationary at "level", stationary at first-differences and integrated with order one denoted as I(1). The Pedroni, Kao and Johansen Fisher co-integration tests were performed. This study uses full modified ordinary least squares (FMOLS) and dynamic ordinary least squares (DOLS) to estimate the long run relationship among the variables. We find that the increase in EG, FP, and CPI increase the Average Electricity Prices (EP); while the increase in Losses, EC, and IVA decreases EP. Therefore, we recommend the promotion of long-term investment policies in renewable sources and efficient policies to reduce technical and commercial losses. In addition, this study suggests that appropriate policies related to subsidized electricity prices would, however, prevent adverse effects related to inefficient over-consumption of electricity.
Recently, the interest of researchers to fractional-order models is greatly increased because of their numerous opportunities for applications in population dynamics [1,2,3,4], bioengineering and neuroscience [5,6,7,8], economics [9,10], and in general, in every area of science, engineering and technology [11,12,13,14,15]. Indeed, fractional differentiation provides neurons with a fundamental and general computation ability that can contribute to efficient information processing, stimulus anticipation and frequency-independent phase shifts of oscillatory neuronal firing [6].
The advantages of fractional-order derivatives have generated much recent interest to the study of fractional neural networks and have resulted in a large amount of papers devoted to the dynamical properties of such networks. See, for example, [16,17,18,19,20,21,22] and the references therein. The numerous applications of fractional-order neural networks to solve optimization, associative memory, pattern recognition and computer vision problems heavily depend on the dynamic behavior of networks; therefore, the qualitative analysis of these dynamic behaviors is an essential step in the workable design of such neural networks. It is worth mentioning that most of the existing studies on delayed fractional-order neural network models considered bounded delays. However, the corresponding investigations on fractional-order delayed neural networks with distributed delays are relatively less. In addition, to the best of our knowledge, unbounded delays are not examined in the existing literature.This interesting open problem is one of the motivations of our study.
The control theory of systems is an important part of their qualitative theory. Among the numerous excellent results on control methods in the literature, we will refer to [23], where a very good comprehensive discussion on several important for neural network models control strategies is given. Recently, the type of control called Impulsive Control, attracts the attention of researchers. This type of control arises naturally in a wide variety of applications and it allows the control action only at some discrete instances which may reduce the amount of information to be transmitted and increase the robustness against the disturbance, see [24,25,26,27,28,29,30,31,32,33]. The impulsive control strategies are also applied to some fractional-order neural networks [34,35,36,37,38]. However, there are still many challenging open questions in this direction. The stability behavior of fractional neural networks with unbounded delays under an impulsive control is not investigated previously, which is the next motivation for the present paper.
On the other side, the concept of Mittag-Leffler stability for fractional-order systems has been introduced in [39]. The importance of the notion lies in the fact that it generalizes the exponential stability concept to the fractional-order case. Since, for integer-order neural network models the exponential convergence is the most desirable behavior, the Mittag-Leffler stability notion of fractional-order systems received a great deal of interest among scientists [35,36,37,39,40,41,42]. However, the concept has not been applied to fractional-order neural networks with unbounded delays, and we plan to fill the gap. The contribution of our paper is in following aspects:
1. Unbounded delays are introduced intro a fractional-order neural network model, and their effects on the qualitative behavior of the solutions are examined.
2. An impulsive control approach is applied to achieve a synchronization between fractional neural networks with mixed bounded and unbounded delays.
3. The concept of global Mittag-Leffler synchronization is adapted to fractional neural network models with mixed delays under impulsive control.
4. New global Mittag-Leffler synchronization criteria are established for the model under consideration.
The rest of the paper is structured as follows. In Section 2, we introduce our fractional-order neural network model with bounded and unbounded delays. The corresponding impulsive control strategy and the impulsive control system are also developed. The concept of global Mittag-Leffler synchronization is proposed for the fractional-order master and controlled systems. Some basic fractional Lyapunov function method nomenclatures and lemmas are presented. In Section 3, by using the fractional Lyapunov method and designing an appropriate impulsive controller, we obtain two main global Mittag-Leffler synchronization criteria. The synchronization results can be easily applied to the stability analysis of such systems. Our results generalize and complement some existing results on integer-order and fractional-order neural networks. Two examples are given to illustrate the efficiency of the results established in Section 4. The conclusion is given in Section 5.
In this paper we will use the standard notation Rn for the n-dimensional Euclidean space. Let ||x||=n∑i=1|xi| denote the norm of x∈Rn, R+=[0,∞), t0∈R+, and let Γ denotes the Gamma function.
Consider a q, 0<q<1. Following [14], the Caputo fractional derivative of order q for a function g∈C1[[t0,b],R], b>t0, is given as
Ct0Dqtg(t)=1Γ(1−q)∫tt0g′(ξ)(t−ξ)qdξ, t≥t0. |
Since distributed and unbounded delays are more realistic, in this research we will consider the following fractional-order neural network with bounded and unbounded delays
{Ct0Dqtxi(t)=−di(t)xi(t)+n∑j=1aijfj(xj(t))+n∑j=1bijfj(xj(t−τj(t)))+n∑j=1cij∫t−∞Kj(t,s)fj(xj(s))ds+Ii, t≥t0, | (2.1) |
where i=1,2,...,n, x(t)=(x1(t),x2(t),...,xn(t))T and xi(t) is the state of ith neuron at time t, fj(xj(t)) denotes the activation function of the jth unit at time t, aij, bij, cij denote the interconnection strength representing the weight coefficient of the neurons, di(t) is a continuous function that represents the self-feedback connection weight of the ith unit at time t, di(t)>0, t≥t0, the bounded time delays τj(t) are such that 0≤τj(t)≤τ, Ii is the external input on the ith neuron, the delay kernel Kj(t,s)=Kj(t−s), (j=1,2,...,n) is of convolution type with an initial condition
x(s)=ˉφ0(s), s∈(−∞,0], ˉφ0∈C[(−∞,0],Rn]. |
The main objective in this paper is to control the stability behavior of the fractional-order network (2.1) by adding an impulsive controller to its nodes such that the trajectories of all nodes can be synchronized onto that of system (2.1).
Let the points
0=t0<t1<t2<...<tk<... |
are such that limk→∞tk=∞, and let the functions Pik are defined on R for any i=1,2,...,n and k=1,2,....
Now we consider the corresponding fractional impulsive control system
{Ct0Dqtyi(t)=−di(t)yi(t)+n∑j=1aijfj(yj(t))+n∑j=1bijfj(yj(t−τj(t)))+n∑j=1cij∫t−∞Kj(t,s)fj(yj(s))ds+Ii, t≠tk, t≥t0,Δyi(tk)=yi(t+k)−yi(tk)=Pik(yi(tk)), k=1,2,..., | (2.2) |
where tk, k=1,2,... are the impulsive control instants and the numbers yi(tk)=yi(t−k) and yi(t+k) are, respectively, the states of the ith unit before and after an impulse input at the moment tk. The functions Pik are the impulsive functions that measure the rate of changes of the states yi(t) at the impulsive moments tk.
The impulsive control model (2.2) generalizes many existing fractional-order neural network systems with bounded and distributed delays [15,36], as well as integer-order neural networks to the fractional-order case. See, for example, [25,26,27,28,29,30,31,32,33] and the references therein. By means of appropriate impulsive functions Pik we can impulsively control the qualitative behavior of the states of type (2.1) fractional models.
The initial conditions associated with system (2.2) are given in the form:
{y(t;t0,φ)=φ(t−t0),−∞<t≤t0,y(t+0;t0,φ)=φ(0), | (2.3) |
where the initial function φ∈Rn is bounded and piecewise continuous on (−∞,0] with points of discontinuity of the first kind at which it is continuous from the left. The set of all such functions will be denoted by PCB[(−∞,0],Rn], and the norm of a function φ∈PCB[(−∞,0], Rn] is defined as ||φ||∞=sups∈(−∞,0]||φ(s)||=supt∈(−∞,t0]||φ(t−t0)||.
According to the theory of impulsive control systems [15,28,29,32,33,34,35,36,37], the solution y(t)=y(t;t0,φ)∈Rn of the initial value problem (2.2), (2.3) is a piecewise continuous function with points of discontinuity of the first kind tk, k=1,2,..., where it is continuous from the left, i.e. the following relations are valid
yi(t−k)=yi(tk), yi(t+k)=yi(tk)+Pik(yi(tk)), i=1,2,...,n, k=1,2,.... |
We introduce some assumptions for the system parameters in (2.2) which will be used in the proofs of our main results. These assumptions also guarantee the existence and uniqueness of the solutions of (2.2):
A2.1. There exist constants Li>0 such that
|fi(u)−fi(v)|≤Li|u−v| |
for all u,v∈R, i=1,2,...,n.
A2.2. There exist constants Mi>0 such that for all u∈R and i=1,2,...,n
|fi(u)|≤Mi<∞. |
A2.3. The delay kernel Ki:R2→R+ is continuous, and there exist positive numbers κi such that
∫t−∞Ki(t,s)ds≤κi<∞ |
for all t≥t0, t≠tk, k=1,2,... and i=1,2,...,n.
A2.4. The functions Pik are continuous on R, i=1,2,...,n, k=1,2,....
A2.5. t0<t1<t2<...tk<tk+1<... and tk→∞ as k→∞.
Remark 2.1. The assumptions A2.1 and A2.2 are used in the existence and uniqueness results for the solutions of fractional-order neural network models of type (2.1). See, for example, [15,16,17,19]. The consideration of more general activation functions that are discontinuous and satisfy a nonlinear growth property as in [18,21] can motivate the researchers for future results on the topic.
To realize the impulsive control and synchronization between the fractional-order neural network systems (2.1) and (2.2) we will use the following impulsive controller:
Pik(yi(t))=Qik(yi(t)−xi(t)), i=1,2,...,n, t=tk, k=1,2,.... | (2.4) |
Define the synchronization error as e(t)=(e1(t),e2(t),...,en(t))T, ei(t)=yi(t)−xi(t), i=1,2,...,n, t>0.
Therefore, the error fractional dynamical system is given as:
{Ct0Dqtei(t)=−di(t)ei(t)+n∑j=1aijˉfj(ej(t))+n∑j=1bijˉfj(ej(t−τj(t)))+n∑j=1cij∫t−∞Kj(t,s)ˉfj(ej(s))ds, t≠tk, t≥t0,ei(t+k)=ei(tk)+Qik(ei(tk)), k=1,2,..., | (2.5) |
where ˉfj(ej(t))=fj(yj(t))−fj(xj(t)), ˉfj(ej(t−τj(t)))=fj(yj(t−τj(t)))−fj(xj(t−τj(t))), and ˉfj(ej(s))=fj(yj(s))−fj(xj(s)), −∞<s≤t, t≥t0, j=1,2,...,n, the impulsive control functions Qik are continuous on R and Qik(0)=0 for all i=1,2,...,n, k=1,2,...,
e(s)=φ0(s)−ˉφ0(s), s∈(−∞,0], e(t+0)=φ0(0)−ˉφ0(0). |
Since we will investigate the Mittag-Leffler synchronization opportunities of the impulsive control approach, we will use the standard Mittag-Leffler function [14] given as
Eq(z)=∞∑κ=0zκΓ(qκ+1), |
where q>0 in our analysis.
In addition, the following definition of global Mittag-Leffler synchronization between fractional-order systems, which is inspired by the Mittag-Leffler stability definition introduced in [39], will be important.
Definition 2.2. The controlled system (2.2) is said to be globally Mittag-Leffler synchronized onto the system (2.1), if for ˉφ0∈PCB[(−∞,0],Rn] there exist constants λ>0 and d>0 such that
||e(t)||≤{M(ˉφ0)Eq(−λtq)}d, t>t0, |
where M(0)=0, M(ˉφ0)≥0, and M(ˉφ0) is Lipschitzian with respect to ˉφ0∈PCB[(−∞,0],Rn].
In other words, the global Mittag-Leffler synchronization between fractional-order systems (2.1) and (2.2) is equivalent to a global Mittag-Leffler stability of the zero solution of the error system (2.5).
We note that, for integer-order systems where q=1, the concept of global Mittag-Leffler synchronization reduces to that of global exponential synchronization, which is a particular type of global asymptotic synchronization. This particular type of synchronization provides the fastest convergent rate and that is why it attracts the high interest. It is also well known, [39] that for fractional-order systems the Mittag-Leffler stability demonstrates a faster convergence speed than the exponential stability near the origin. This is the main motivation of our research.
Introduce the following notations:
Gk=(tk−1,tk)×Rn,k=1,2,...; G=∪∞k=1Gk.
Further on we will apply the Lyapunov approach and to this end we will use piecewise continuous Lyapunov functions V: [t0,∞)×Rn→R+.
Definition 2.3. We say that the function V:[t0,∞)×Rn→R+, belongs to the class V0 if the following conditions are fulfilled:
1. The function V is continuous in ∪∞k=1Gk and V(t,0)=0 for t∈[t0,∞).
2. The function V satisfies locally the Lipschitz condition with respect to e on each of the sets Gk.
3. For each k=1,2,... and e∈Rn there exist the finite limits
V(t−k,e)=limt→tkt<tk V(t,e), V(t+k,e)=limt→tkt>tk V(t,e). |
4. For each k=1,2,... and e∈Rn the following equalities are valid
V(t−k,e)=V(tk,e). |
We will also need the following auxiliary lemma, which is an impulsive generalization of Lemma 2.1 in [42] for systems with unbounded delays. The proof is identical to the proof of (21) in [42] and we omit it. Similar comparison results are proved in [15,36,38] and some of the references therein.
Lemma 2.4. Assume that the function V∈V0 is such that for t∈[t0,∞), φ∈PCB[(−∞,0],Rn],
V(t+,e(t+)+Δ(e(t)))≤V(t,e(t)), t=tk, k=1,2,..., |
and the inequality
Ct0DqtV(t,φ(t))≤MV(t,φ(0)), t≠tk, k=1,2,... |
is valid whenever V(t+s,φ(s))≤V(t,φ(0)) for −∞<s≤0, where M∈R.
Then sup−∞<s≤0V(s,φ0(s))≤V(t,φ0(0)) implies
V(t,e(t))≤sup−∞<s≤0V(t+0,e(s))Eq(Mtq),t∈[t0,∞). |
In the case, when the Lyapunov-like function is of the type V(t,e)=n∑i=1e2i(t) we will use the following result from [43].
Lemma 2.5. Let ei(t)∈R be a continuous and differentiable function, i=1,2,...,n. Then, for t≥t0 and 0<q<1, the following inequality holds
12Ct0Dqte2i(t)≤ei(t)Ct0Dqtei(t), i=1,2,...,n. |
In this section, sufficient conditions for the global Mittag-Leffler synchronization of the controlled system (2.2) onto the system (2.1), which imply global asymptotic stability of the zero equilibrium of error system (2.5) are derived.
Theorem 3.1. Assume that assumptions A2.1–A2.5 hold and there exist positive constants d_i such that d_i≤di(t) for t∈R+.
Then, the neural network system (2.2) is globally Mittag-Leffler synchronized onto the system (2.1) under the impulsive controller (2.4), if the following conditions simultaneously hold:
min1≤i≤n(d_i−Lin∑j=1|aji|)>max1≤i≤n(Li(n∑j=1|bji|+κin∑j=1|cji|))>0 | (3.1) |
Qik(ei(tk))=−γik(yi(tk)−xi(tk)),0<γik<2, | (3.2) |
i=1,2,...,n, k=1,2,....
Proof. For the error system (2.5) we construct a Lyapunov function as:
V(t,e)=n∑i=1|ei(t)|. |
Case 1. Consider first the case when t≥t0 and t∈[tk−1,tk). Then, by the definition of the Caputo fractional derivative of order q, we have [14,15,42]
Ct0Dqt|ei(t)|=sgn(ei(t))Ct0Dqtei(t) i=1,2,...,n. |
Using A2.1 and A2.3 and the assumptions of Theorem 3.1, we obtain
Ct0Dqt|ei(t)|≤−d_i|ei(t)|+n∑j=1Lj|aij||ej(t)|+n∑j=1Lj|bij||ej(t−τj(t))|+n∑j=1Ljκj|cij|sup−∞<s≤t|ej(s)|, |
for i=1,2,...,n.
After taking the sum for all i=1,2,...,n, we have
Ct0DqtV(t,e(t))≤−n∑i=1[d_i−Lin∑j=1|aji|]|ei(t)|+n∑j=1n∑i=1Lj|bij||ej(t−τj(t))| |
+n∑j=1n∑i=1Ljκj|cij|sup−∞<s≤t|ej(s)|≤−ν1V(t,e(t))+ν2sup−∞<s≤tV(s,e(s)), |
where
ν1=min1≤i≤n(d_i−Lin∑j=1|aji|)>0, |
ν2=max1≤i≤n(Li(n∑j=1|bji|+κin∑j=1|cji|))>0. |
According to the above estimate for any solution e(t) of (2.5) such that
V(s,e(s))≤V(t,e(t)),−∞<s≤t, |
we have
Ct0DqtV(t,e(t))≤−(ν1−ν2)V(t,e(t)), t≠tk, k=1,2,.... |
Condition (3.1) of Theorem 3.1 implies the existence of a real number λ>0 such that
ν1−ν2≥λ, |
and, it follows that
Ct0DqtV(t,e(t))≤−λV(t,e(t)), t≠tk, t≥t0. | (3.3) |
Case 2. For t=tk, k=1,2,..., from condition (3.2), we obtain
V(t+k,e(tk)+Δ(e(tk)))=n∑i=1|ei(tk)+Qik(e(tk))| |
=n∑i=1|yi(tk)−xi(tk)−γik(yi(tk)−xi(tk))|=n∑i=1|1−γik||yi(tk)−xi(tk)| |
<n∑i=1|yi(tk)−xi(tk)|=V(tk,e(tk)),k=1,2,.... | (3.4) |
Thereupon, using (3.3) and (3.4), it follows from Lemma 2.4 that
V(t,e(t))≤sup−∞<s≤0V(t+0,e(s))Eq(−λtq),t∈[t0,∞). |
Therefore, we have
||e(t)||=n∑i=1|ei(t)|≤||φ0−ˉφ0||∞Eq(−λtq),t≥t0. |
Denote by M=||φ0−ˉφ0||∞. Hence,
||e(t)||≤MEq(−λtq),t>t0, |
where M≥0 and M=0 holds only if φ0(s)=ˉφ0(s) for s∈(−∞,0], which implies that the closed-loop neural network (2.2) is globally Mittag-Leffler synchronized onto system (2.1) under the designed impulsive control law (2.4).
Theorem 3.2. Assume that assumptions of Theorem 3.1 hold, and (3.1) is replaced by
min1≤i≤n(2d_i−n∑j=1(Lj(|aij|+|bij|+κj|cij|)+Li|aji|))>max1≤i≤n(Li(n∑j=1|bji|+κin∑j=1|cji|))>0 | (3.5) |
Then, the neural network system (2.2) is globally Mittag-Leffler synchronized onto the system (2.1) under the impulsive controller (2.4).
Proof. The proof of Theorem 3.2 is similar to those of Theorem 3.1. We will mention just some main points.
For the error system (2.5) we construct a Lyapunov function as:
V(t,e)=n∑i=1e2i(t). |
First, for t=tk, k=1,2,..., from condition (3.2), we obtain
V(t+k,e(tk)+Δ(e(tk)))=n∑i=1(ei(tk)+Qik(e(tk)))2 |
=n∑i=1(yi(tk)−xi(tk)−γik(yi(tk)−xi(tk)))2=n∑i=1(1−γik)2(yi(tk)−xi(tk))2 |
<n∑i=1(yi(tk)−xi(tk))2=V(tk,e(tk)),k=1,2,.... | (3.6) |
Secondly, for t≥t0 and t∈[tk−1,tk), k=1,2,..., we apply again A2.1, A2.3 and the assumptions of Theorem 3.1 to get
Ct0DqtV(t,e(t))≤n∑i=12|ei(t)|sgn(ei(t))[−di(t)ei(t)+n∑j=1aijˉfj(ej(t))+n∑j=1bijˉfj(ej(t−τj(t))) |
+n∑j=1cij∫t−∞Kj(t,s)ˉfj(ej(s))ds] |
≤n∑i=1[−2d_ie2i(t)+2n∑j=1Lj|aij||ei(t)||ej(t)|+2n∑j=1Lj|bij||ei(t)||ej(t−τj(t))| |
+2n∑j=1Ljκj|cij||ei(t)|sups∈(−∞,t]|ej(s)|] |
≤n∑i=1[−2d_ie2i(t)+n∑j=1Lj|aij|(e2i(t)+e2j(t))+n∑j=1Lj|bij|(e2i(t)+e2j(t−τj(t))) |
+n∑j=1Ljκj|cij|(e2i(t)+sups∈(−∞,t]e2j(s))] |
=−n∑i=1[2d_i+n∑j=1(Lj(|aij|+|bij|+κj|cij|)+Li|aji|)]e2i(t) |
+n∑j=1n∑i=1(Lj|bij|e2j(t−τj(t))+Ljκj|cij|sups∈(−∞,t]e2j(s))) |
≤−ˉν1V(t,e(t))+ν2sup−∞<s≤tV(s,e(s)), |
where
ˉν1=min1≤i≤n(2d_i−n∑j=1(Lj(|aij|+|bij|+κj|cij|)+Li|aji|))>0, |
ν2=max1≤i≤n(Li(n∑j=1|bji|+κin∑j=1|cji|))>0. |
The rest of the proof repeats the end of the proof of Theorem 3.1 using (3.5) instead of (3.1).
Remark 3.3. Theorems 3.1 and 3.2 offer an impulsive control law with control gains γik that can be applied to the Mittag-Leffler synchronization of the fractional neural network model (2.2) into the model (2.1). Since the synchronization is directly related to the stability and stabilization problems of systems, the proposed impulsive control strategy is a power tool for studying the stability dynamics of fractional-order neural networks.
Remark 3.4. Impulsive control approaches are applied to various integer-order neural networks models in the existing literature. See, for example, [26,27,28,29,30,31,32,33] and some of the references therein. Indeed, it is well known that such control strategies have important advantages. In this paper, we generalize the impulsive control approach to the fractional-order case. In fact, the impulsive controllers (2.4) are designed so that to achieve global Mittag-Leffler synchronization between the fractional master system (2.1) and the control fractional system (2.2).
Remark 3.5. In spite of the great possibilities of applications, the theory of the fractional neural networks with distributed delays is still in the initial stage [22]. To the best of our knowledge, there has not been any work so far considering unbounded delays in fractional-order neural network models, which is very important in theories and applications and also is a very challenging problem. Hence, our results extend the existent ones in the literature adding the effect of unbounded delays.
Remark 3.6. A review of the existing results shows that impulsive control strategies have been applied to some fractional-order neural network models [34,35,36,37,38]. With the presented research we complement the existing works by incorporating unbounded delays into the fractional-order neural network model. The results in [36] can be considered as special cases of the proposed results here, when the terms with unbounded delays are removed in (2.1) and (2.2). Hence, as compared to [34,35,36,37,38], the proposed results in this paper are more general. To the best of our knowledge, this is the first paper on fractional-order neural network models with unbounded delays and subject to impulsive control law.
Remark 3.7. The concept of Mittag-Leffler synchronization between fractional-order neural networks is investigated in some papers. See, for example [36,37,40,41]. In this paper, we extended the existing results incorporating unbounded delays and impulsive perturbations into fractional-order neural networks and dealt with an impulsive synchronization analysis for the addressed more general models.
In this section, examples are presented to illustrate the main results.
Example 4.1. Consider a two-dimensional Caputo fractional neural network of type (2.1) with mixed delays as follows
{Ct0Dqtxi(t)=−di(t)xi(t)+n∑j=1aijfj(xj(t))+n∑j=1bijfj(xj(t−τj(t)))+n∑j=1cij∫t−∞Kj(t,s)fj(xj(s))ds+Ii, t≥t0, | (4.1) |
where n=2, t0=0, I1=1, I2=1, d1(t)=d2(t)=3, fi(xi)=12(|xi+1|−|xi−1|), 0≤τi(t)≤τ (τ=1), Ki(s)=e−s, i=1,2,
(aij)2×2=(a11a12a21a22)=(0.50.6−0.51), |
(bij)2×2=(b11b12b21b22)=(0.9−0.2−0.040.07), |
(cij)2×2=(c11c12c21c22)=(0.5−0.6−0.030.08). |
Then, we have that d_1=d_2=3, L1=L2=1, and the assumption A2.3 is satisfied, since ∫∞0e−sds=1.
We consider the following impulsive control system
{Ct0Dqtyi(t)=−di(t)yi(t)+2∑j=1aijfj(yj(t))+2∑j=1bijfj(yj(t−τj(t)))+2∑j=1cij∫t−∞Kj(t,s)fj(yj(s))ds+Ii, t≠tk, t≥0, | (4.2) |
with an impulsive control rule defined as
{Δy1(tk)=−34(y1(tk)−x1(tk)), k=1,2,...,Δy2(tk)=−12(y2(tk)−x2(tk)), k=1,2,..., | (4.3) |
where the impulsive moments are such that 0<t1<t2<..., and limk→∞tk=∞.
Hence, the condition (3.1) of Theorem 3.1 is satisfied for ν1=1.4, ν2=0.97. We also have that the impulsive control gains satisfy condition (3.2), since
0<γ1k=34<2,0<γ2k=12<2. |
According to Theorem 3.1, the master system (4.1) and response system (4.2) with impulsive control (4.3) are globally Mittag-Leffler (globally asymptotically) synchronized. Time responses of the state variables of the synchronization error system are given on Figure 1, for tk=5k, k=1,2,....
If we consider again the system (4.2) but with impulsive perturbations of the form
{Δy1(tk)=−3(y1(tk)−x1(tk)), k=1,2,...,Δy2(tk)=−12(y2(tk)−x2(tk)), k=1,2,..., | (4.4) |
the impulsive control rule (3.2) is not satisfied, and there is nothing we can say about the impulsive synchronization between systems (4.1) and (4.2) with impulsive perturbations (4.4), since γ1k=3>2. The state variable e1(t) of the error system is demonstrated on Figure 2 in the case when tk=5k, k=1,2,.... It is interesting to see that the impulses cannot synchronize both systems in this case.
Remark 4.2. Note that the impulsive functions Qik, i=1,2,...,n, k=1,2,... in the impulsive control rule (2.4) may be of different type. In this paper, we investigate the case, when the controller (2.4) has the form given in (3.2). By means of Example 1, we demonstrate the efficiency of the controllers of type (3.2). We show that, if the impulsive controller is designed according to (3.2), it contributes to the global Mittag-Leffler synchronization between the fractional-order models (4.1)–(4.3). We also illustrate the case, when the impulsive controller does not satisfy (3.2), and the synchronization between (4.1) and (4.2), (4.4) fails, i.e., the zero solution of the error system is globally Mittag-Leffler unstable.
Example 4.3. Consider a two-dimensional Caputo fractional neural network of type (4.1) with mixed delays, where t0=0; I1=1, I2=1; d1(t)=d2(t)=4+t, fi(xi)=12(|xi+1|−|xi−1|), 0≤τi(t)≤τ (τ=1), Ki(s)=e−s, i=1,2,
(aij)2×2=(a11a12a21a22)=(21−12), |
(bij)2×2=(b11b12b21b22)=(0.1−0.2−0.150.1), |
(cij)2×2=(c11c12c21c22)=(0.1−0.2−0.150.2). |
Now, we have that d_1=d_2=4, L1=L2=1.
If the impulsive controllers (2.4) are chosen so that
{P1k(y1(tk))=−45(y1(tk)−x1(tk)), k=1,2,...,P2k(y2(tk))=−23(y2(tk)−x2(tk)), k=1,2,..., | (4.5) |
where the impulsive moments are such that 0<t1<t2<..., and limk→∞tk=∞, then the corresponding impulsive control system is
{Ct0Dqtyi(t)=−di(t)yi(t)+2∑j=1aijfj(yj(t))+2∑j=1bijfj(yj(t−τj(t)))+2∑j=1cij∫t−∞Kj(t,s)fj(yj(s))ds+Ii, t≠tk, t≥t0,Δy1(tk)=−45(y1(tk)−x1(tk)), k=1,2,...,Δy2(tk)=−23(y2(tk)−x2(tk)), k=1,2,.... | (4.6) |
Hence, the condition (3.5) of Theorem 3.2 is satisfied for ν1=1.4, ν2=0.7. We also have that the impulsive control gains satisfy condition (3.2), since
0<γ1k=45<2,0<γ2k=23<2. |
Therefore, we obtain by Theorem 3.2, that the master system (4.1) and response system (4.6) are globally Mittag-Leffler (globally asymptotically) synchronized. Time responses of the state variables of the synchronization error system are represented on Figure 3, for tk=5k, k=1,2,....
Remark 4.4. We presented two examples to demonstrate the efficiency of both theorems that ensure the global Mittag-Leffler synchronization of fractional-order neural networks by employing different Lyapunov function candidates, and hence using different conditions of type (3.1) and (3.5). For both synchronization criteria we apply a unified impulsive control rule (3.2). However, the established criteria can help to check the synchronization of impulsive fractional-order neural networks with different systems parameters.
In this paper, we have investigated the global Mittag-Leffler synchronization problem between two fractional-order neural networks with bounded and unbounded delays. Applying an impulsive control approach, criteria are obtained by constructing appropriate Lyapunov functions and the fractional Lyapunov approach. The obtained results are new and complement the existing global Mittag-Leffler synchronization results for fractional neural networks under impulsive controls. Examples are demonstrated to illustrate the obtained results. Since, the impulsive control approach is preferable in many real-world applications, our results can be extended to fractional-order models with reaction-diffusion terms. The discrete cases are also a subject to future investigations.
This work was supported in part by the European Regional Development Fund through the Operational Program "Science and Education for Smart Growth" under contract UNITe No BG05M2OP001–1.001–0004 (2018–2023).
The authors declare no conflict of interest.
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