
In this paper, we study fixed-deviation stabilization and synchronization for fractional-order complex-valued neural networks with delays. By applying fractional calculus and fixed-deviation stability theory, sufficient conditions are given to ensure the fixed-deviation stabilization and synchronization for fractional-order complex-valued neural networks under the linear discontinuous controller. Finally, two simulation examples are presented to show the validity of theoretical results.
Citation: Bingrui Zhang, Jin-E Zhang. Fixed-deviation stabilization and synchronization for delayed fractional-order complex-valued neural networks[J]. Mathematical Biosciences and Engineering, 2023, 20(6): 10244-10263. doi: 10.3934/mbe.2023449
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In this paper, we study fixed-deviation stabilization and synchronization for fractional-order complex-valued neural networks with delays. By applying fractional calculus and fixed-deviation stability theory, sufficient conditions are given to ensure the fixed-deviation stabilization and synchronization for fractional-order complex-valued neural networks under the linear discontinuous controller. Finally, two simulation examples are presented to show the validity of theoretical results.
Fractional calculus is a theory of differentiation and integration of arbitrary order, which is an extension of integer order calculus. Initially, the study of fractional calculus theory was mainly conducted in the field of pure number theory, but as it developed further, fractional calculus was widely used in fluid mechanics [1], mechanical systems [2], signal processing [3,4], system identification [5], and many other fields. Fractional calculus has become an essential theory in many fields. Many scholars have applied fractional-order derivatives to neural networks and have built fractional-order neural networks (FONNs). So far, the study of FONNs has yielded some interesting results [6,7,8,9,10,11,12,13,14,15,16,17]. Zhang and Zeng [18] showed asymptotic stability of nonlinear FONNs with unbounded time-varying delays and asymptotic synchronization of FONNs under a linear controller. Ding et al. [19] investigated the robust finite-time stability of FONNs.
Complex-valued neural networks (CVNNs), whose input/output signals, connection weights, and activation functions are derived from the complex domain. Unlike real-valued neural networks, functions that are both bounded and analytic in the complex domain must be constant according to Liouville's theorem [20]. Therefore, the study of the dynamics of CVNNs is essential. In recent years, the dynamic behavior of fractional-order CVNNs (FOCVNNs) has been reported in many kinds of literatures, including finite-time stability [21,22], impulse stability and synchronization [23], and Mittag-Leffler stability and synchronization [24,25].
In neural networks, time delays are prevalent. Failure to take into account time delays will cause stable systems to be unstable and lead to a reduction in the capabilities of the neural network [26,27]. Therefore it is relevant to study FOCVNNs with time delays in practical applications. Bao et al. [28] obtained sufficient conditions to guarantee the synchronization of FOCVNNs with time delays using linear delay feedback control and fractional-order inequalities. Liu and Yu [29] derived several conditions for quasi-projective synchronization and complete synchronization of FOCVNNs with time delays based on generalized discrete fractional Halanay inequality and Lyapunov generalized function methods without dividing the complex-valued neural network into two real-valued systems.
Deviation dynamics is particularly important for the evolutionary characterization of control systems. Fixed-deviation stabilization and synchronization are very important dynamical behaviors of discontinuous neural network systems. There have been some important findings about fixed-deviation dynamics [30,31]. Chen et al. [30] initially proposed the concept of fixed-deviation stability to describe the stability properties of discontinuous systems, and sufficient conditions to ensure globally uniform asymptotic fixed-deviation stability of delayed fractional-order memristive neural networks were given. Based on the theory of fixed-deviations in [30], Zhang [31] used linear-type discontinuous control and fractional-order calculus methods to address fixed-deviation stability and synchronization problems of FONNs. Clearly, the investigation of fixed-deviation dynamics for FONNs is an important topic. But so far, there are few results on the fixed-deviation dynamics of FOCVNNs.
In the above view, we present the problems of fixed-deviation stability and synchronization of FOCVNNs. Continuous FONNs are difficult to achieve fixed-deviation stability and synchronization, and a special control method needs to be imposed to make the continuous system generate fixed-deviation dynamics behavior. A natural idea is to add a discontinuous controller so that continuous FOCVNNs turn into the discontinuous system under the discontinuous controller, and then impose complex-valued conditions to make the FOCVNNs achieve fixed-deviation stability and synchronization. Also based on the theory of fixed-deviations in [30], fractional-order calculus and Lyapunov method, sufficient conditions for the formation of fixed-deviation stability and synchronization of FOCVNNs under linear discontinuous controllers are obtained.
In this section, necessary definitions and lemmas will be provided for the proof of the theorem in Section 3.
The Caputo's fractional derivative of a function H(t)∈Cλ+1([t0,+∞),R) with order α>0 is defined by
CDαt0H(t)=1Γ(λ−α)∫tt0H(λ)(s)(t−s)α−λ+1 ds, |
where t≥t0, λ−1<α<λ, λ is positive integer, α is a positive constant and Γ(⋅) is Gamma function, that is
Γ(α)=∫∞0tα−1e−tdt. |
The Riemann-Liouville fractional derivative of order α>0 for a function H(t)∈Cλ+1([t0,+∞),R) is defined by
RLDαt0H(t)=1Γ(λ−α)dλdtλ∫tt0H(s)(t−s)α−λ+1 ds, |
where λ−1<α<λ, λ>0.
By the above definition, the following relation holds:
CDαt0H(t)=RLDαt0H(t)−H(t0)Γ(1−α)(t−t0)−α. |
Now, we introduce delayed FOCVNNs as follows:
CDαt0zk(t)=−akzk(t)+n∑ℓ=1bkℓfℓ(zℓ(t))+n∑ℓ=1dklgℓ(zℓ(t−ϖkl(t)))+Uk(t), | (2.1) |
where 0<α<1, zk(t)∈C denotes the state variable; ak>0 is the self-feedback connective weight of the kth neuron; bkℓ and dkℓ are the connective weights matrix without and with time delay respectively; fℓ(zℓ(t)), gℓ(zℓ(t−ϖkℓ(t))) represent the complex-valued state activation functions at time t and t−ϖkℓ(t); ϖkℓ(t) is the time-varying delay satisfying 0≤ϖkℓ(t)≤ϖ; Uk(t) stands for the external input.
Let Cϖ=C([−ϖ,0],Rn) be the Banach space of continuous functions mapping [−ϖ,0] into Rn. For ψ∈Cϖ,‖ψ‖c=sup−ϖ≤s≤0‖ψ(s)‖.
Note the initial conditions of delayed FOCVNNs (2.1) as
zk(t0+s)=ψRk(s)+ψIk(s),−ϖ≤s≤0,k=1,⋯,n. | (2.2) |
Let z=zR+izI∈C. For any ℓ, fℓ(z) and gℓ(z(t−ϖ)) can be shown by dividing into its real and imaginary parts as
fℓ(z)=fRℓ(zR,zI)+ifIℓ(zR,zI),gℓ(z(t−ϖ))=gRℓ(zR(t−ϖ),zI(t−ϖ))+igIℓ(zR(t−ϖ),zI(t−ϖ)). | (2.3) |
Let zk(t)=zRk(t)+izIk(t). Delayed FOCVNNs (2.1) can be described as the following equation:
CDαt0zRk(t)=−akzRk(t)+n∑ℓ=1bRkℓfRℓ(zℓ(t))−n∑ℓ=1bIkℓfIℓ(zℓ(t))+n∑ℓ=1dRkℓgRℓ(zℓ(t−ϖkℓ(t)))−n∑ℓ=1dIkℓgIℓ(zℓ(t−ϖkℓ(t)))+URk(t), |
CDαt0zIk(t)=−akzIk(t)+n∑ℓ=1bRkℓfIℓ(zℓ(t))+n∑ℓ=1bIkℓfRℓ(zℓ(t))+n∑ℓ=1dRkℓgIℓ(zℓ(t−ϖkℓ(t)))+n∑ℓ=1dIkℓgRℓ(zℓ(t−ϖkℓ(t)))+UIk(t). | (2.4) |
Definition 1 ([30]): FOCVNNs (2.1) is called globally uniformly β-stable if for any ξ>0 and any initial values ϕ,φ∈Cϖ, ‖ϕ−φ‖C≤ξ, there is a constant T(ξ)≥0, such that
‖z(t,t0,ϕ)−z(t,t0,φ)‖≤β |
for all t≥t0+T(ξ), where β>0.
Remark 1: β-stability, also known as fixed-deviation stability, specifically, when the difference between two different initial values of the described neural network are kept in a certain range, the difference among final values of the system trajectories starting from these two initial values will be maintained in a fixed-deviation degree.
Definition 2: The zero solution of delayed FOCVNNs (2.1) is called globally uniformly β-stable if for any ψ∈Cϖ, ξ>0, ‖ψ‖C≤ξ, there is a constant T(ξ)≥0, such that
‖z(t,t0,ψ)‖≤β |
for all t≥t0+T(ξ), where β>0 is a constant.
In this paper, we propose the below assumptions:
(i) The activation functions fℓ(⋅) and gℓ(⋅) satisfy fℓ(0)=gℓ(0)=0.
(ii) For functions fRℓ(⋅,⋅), fIℓ(⋅,⋅), gRℓ(⋅,⋅), gIℓ(⋅,⋅), there exist positive constants FRRℓ, FRIℓ, FIRℓ, FIIℓ, GRRℓ, GRIℓ, GIRℓ, GIIℓ, such that
{|fRℓ(˜zR,˜zI)−fRℓ(zR,zI)|≤FRRℓ|˜zR−zR|+FRIℓ|˜zI−zI||fIℓ(˜zR,˜zI)−fIℓ(zR,zI)|≤FIRℓ|˜zR−zR|+FIIℓ|˜zI−zI||gRℓ(˜zR,˜zI)−gRℓ(zR,zI)|≤GRRℓ|˜zR−zR|+GRIℓ|˜zI−zI||gIℓ(˜zR,˜zI)−gIℓ(zR,zI)|≤GIRℓ|˜zR−zR|+GIIℓ|˜zI−zI|. | (2.5) |
Remark 2: Condition (i) holds if and only if both its real and imaginary parts are 0, i.e., fRℓ(0,0)=fIℓ(0,0)=0 and gRℓ(0,0)=gIℓ(0,0)=0 for any ℓ∈R.
Next, we present two necessary lemmas.
Lemma 1 ([30]): If functions f(t) and g(t) together with their derivatives are continuous in [t0,t], then fractional differentiation of the Leibniz rule is in the form
RLDαt0(p(t)q(t))=n∑m=0(αm)dmp(t)dtmRLDα−mt0q(t)−Iαn(t), |
where n≥α+1,
(αm)=Γ(α+1)m!Γ(α−m+1), |
and
Iαn(t)=(−1)n(t−α)n−α+1n!Γ(−α)∫10∫10ϝα(t,ζ,ℏ)dζdℏ,ϝα(t,ζ,ℏ)=q(t0+ℏ(t−t0))p(n+1)(t0+(t−t0)(ζ+ℏ−ζℏ)). |
Lemma 2: For a continuous differentiable function P(t):[t0,+∞)→[0,+∞) and Q(t)=(t−t0+σ)αP(t), then
CDαt0Q(t)≤(t−t0+σ)αCDαt0P(t)+1−α+α2σαΓ(2−α)¯Q(t), |
where t≥t0, σ>0 and ¯Q(t)=supt0≤s≤tQ(s).
Proof: From Lemma 1, we know
CDαt0Q(t)=RLDαt0Q(t)−Q(t0)Γ(1−α)(t−t0)−α=(t−t0+σ)αRLDαt0P(t)+α2(t−t0+σ)α−1RLDα−1t0P(t)−Rα2(t)−σαP(t0)Γ(1−α)(t−t0)−α≤(t−t0+σ)α(CDαt0P(t)+P(t0)Γ(1−α)(t−t0)−α)−σαP(t0)Γ(1−α)(t−t0)−α+α2(t−t0+σ)α−1RLDα−1t0P(t)≤(t−t0+σ)αCDαt0P(t)+P(t0)Γ(1−α)+α2(t−t0+σ)α−1RLDα−1t0P(t)≤(t−t0+σ)αCDαt0P(t)+¯Q(t)σαΓ(1−α)+α2(t−t0+σ)α−1RLDα−1t0P(t). |
Also by the definition of Riemann-Liouville fractional derivative,
α2(t−t0+σ)α−1RLDα−1t0P(t)=α2Γ(1−α)(t−t0+σ)α−1∫tt0(t−s)−αP(s)ds≤α2σαΓ(2−α)¯Q(t). |
Therefore,
CDαt0Q(t)≤(t−t0+σ)αCDαt0P(t)+¯Q(t)σαΓ(1−α)+α2σαΓ(2−α)¯Q(t)=(t−t0+σ)αCDαt0P(t)+1−α+α2σαΓ(2−α)¯Q(t) |
for t≥t0. Proof of Lemma 2 is finished.
In this section, we will provide some sufficient conditions to guarantee fixed-deviation stability and synchronization of delayed FOCVNNs (2.1).
We design linear discontinuous control for system (2.1):
Uk(t)=Mkzk(t)+Nk[sgn(zRk(t))+isgn(zIk(t))], | (3.1) |
where k=1,⋯,n.
Thus by controller (3.1), system (2.4) is converted as
CDαt0zRk(t)=−akzRk(t)+n∑ℓ=1bRkℓfRℓ(zℓ(t))−n∑ℓ=1bIkℓfIℓ(zℓ(t))+n∑ℓ=1dRkℓgRℓ(zℓ(t−ϖkℓ(t)))n∑ℓ=1dIkℓgIℓ(zℓ(t−ϖkℓ(t)))+MkzRk(t)+Nksgn(zRk(t)), |
CDαt0zIk(t)=−akzIk(t)+n∑ℓ=1bRkℓfIℓ(zℓ(t))+n∑ℓ=1bIkℓfRℓ(zℓ(t))+n∑ℓ=1dRkℓgIℓ(zℓ(t−ϖkℓ(t)))+n∑ℓ=1dIkℓgRℓ(zℓ(t−ϖkℓ(t)))+MkzIk(t)+Nksgn(zIk(t)). | (3.2) |
Theorem 1: If there are positive constants σ>ϖ≥0 and μr>0,vr>0(r=1,⋯,n) such that the following conditions
ar−|Mr|−1−α+α2σαΓ(2−α)−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))(σ−ϖ+σ)α]μℓ>0 | (3.3) |
and
ar−|Mr|−1−α+α2σαΓ(2−α)−1vrn∑ℓ=1[|bRrℓ|(FIRℓ+FIIℓ)+|bIrℓ|(FRRℓ+FRIℓ)+(|dRrℓ|(GIRℓ+GIIℓ)+|dIrℓ|(GRRℓ+GRIℓ))(σ−ϖ+σ)α]vℓ>0 | (3.4) |
hold, then delayed FOCVNNs (3.2) is globally uniformly β-stable, that is, delayed FOCVNNs (2.1) is globally uniformly β-stable via control rule (3.1).
Proof: Construct an auxiliary function as follows
P(t)=max1≤k≤nmax{|zRk(t)|μk,|zIk(t)|vk}. |
Let
Q(t)=(t−t0+σ)αP(t),¯Q(t)=supt0−σ≤s≤tQ(s). |
There exists r∈{1,⋯,n} for given t≥t0 having
P(t)=max{|zRr(t)|μr,|zIr(t)|vr}. |
Then we get P(t)=|zRr(t)|μr, P(t)=|zIr(t)|vr. Now, we let P(t)=|zRr(t)|μr, and another case is similar. By (2.5) and (2.7) it follows that
CDαt0P(t)=1μrCDαt0|zRr(t)|≤sgn(zRr(t))μrCDαt0zRr(t)≤−(ar−|Mr|)μr|zRr(t)|+|Nr|μr+1μrn∑ℓ=1|bRrℓ|(FRRℓ|zRℓ(t)|+FRIℓ|zIℓ(t)|)+1μrn∑ℓ=1|bIrℓ|(FIRℓ|zRℓ(t)|+FIIℓ|zIℓ(t)|)+1μrn∑ℓ=1|dRrℓ|(GRRℓ|zRℓ(t−ϖrℓ(t))|+GRIℓ|zIℓ(t−ϖrℓ(t))|)+1μrn∑ℓ=1|dIrℓ|(GIRℓ|zRℓ(t−ϖrℓ(t))|+GIIℓ|zIℓ(t−ϖrℓ(t))|)≤−(ar−|Mr|)P(t)+|Nr|μr+1μrn∑ℓ=1|bRrℓ|(FRRℓ+FRIℓ)μℓP(t)+1μrn∑ℓ=1|bIrℓ|(FIRℓ+FIIℓ)μℓP(t)+1μrn∑ℓ=1|dRrℓ|(GRRℓ+GRIℓ)μℓP(t−ϖrℓ(t))+1μrn∑ℓ=1|dIrℓ|(GIRℓ+GIIℓ)μℓP(t−ϖrℓ(t))={−(ar−|Mr|)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)]μℓ}P(t)+1μrn∑ℓ=1[|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ)]μℓP(t−ϖrℓ(t))+|Nr|μr. | (3.5) |
By using Lemma 2 and (3.5), then
CDαt0Q(t)≤(t−t0+σ)αCDαt0P(t)+1−α+α2σαΓ(2−α)¯Q(t)≤{−(ar−|Mr|)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)]μℓ}Q(t)+1μrn∑ℓ=1[|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ)]μℓ(t−t0+σt−ϖrℓ(t)−t0+σ)αQ(t−ϖrℓ(t))+(t−t0+σ)α|Nr|μr+1−α+α2σαΓ(2−α)¯Q(t)≤{−(ar−|Mr|)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)]μℓ}Q(t)+1μrn∑ℓ=1[|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ)]μℓ(t−t0+σt−ϖrℓ(t)−t0+σ)α¯Q(t)+(t−t0+σ)α|Nr|μr+1−α+α2σαΓ(2−α)¯Q(t). |
It is known that σ+EE−ϖrℓ(t)+σ is monotone non-increasing for E≥0, and thus
t−t0+σt−ϖrℓ(t)−t0+σ≤σ−ϖrl(t)+σ≤σ−ϖ+σ, |
therefore,
CDαt0Q(t)≤{−(ar−|Mr|)+1−α+α2σαΓ(2−α)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))(σ−ϖ+σ)α]μℓ}Q(t)+(t−t0+σ)α|Nr|μr≤−AQ(t)+(t−t0+σ)αB | (3.6) |
when Q(t)=¯Q(t), for t≥t0, where
A≜min1≤r≤n{ar−|Mr|−1−α+α2σαΓ(2−α)−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))(σ−ϖ+σ)α]μℓ},B≜max1≤r≤n(|Nr|μr). |
Next, from the definition ¯Q(t)=supt0−σ≤s≤tQ(s), we will divide into three cases to prove fixed-deviation stable.
Case 1: ¯Q(s)>Q(s) for any t0<s≤t. Now, we consider ¯Q(t) is the maximum value of Q(s) at moment t0, that is
¯Q(t)=¯Q(t0),∀t≥t0. |
Hence,
‖z(t)‖≤‖μ‖P(t)=‖μ‖(t−t0+σ)αQ(t)≤‖μ‖(t−t0+σ)α¯Q(t)=‖μ‖(t−t0+σ)α¯Q(t0)≤‖μ‖σα(t−t0+σ)μmin‖ψ‖C≤‖μ‖σαξ(t−t0+σ)μmin, |
when ‖ψ‖C≤ξ, where μmin=min1≤r≤n{μr}.
Case 2: ¯Q(t)=Q(t). We obtain
CDαt0¯Q(t)≤CDαt0Q(t),t≥t0. | (3.7) |
From divisional integration method, we have
∫tt0¯Q′(s)−Q′(s)(t−s)αds=lims→t−¯Q(s)−Q(s)(t−s)α−¯Q(t0)−Q(t0)(t−t0)α−α∫tt0¯Q(s)−Q(s)(t−s)α+1ds=lims→t−1−α[¯Q′(s)−Q′(s)](t−s)1−α−¯Q(t0)−Q(t0)(t−t0)α−α∫tt0¯Q(s)−Q(s)(t−s)α+1ds=−¯Q(t0)−Q(t0)(t−t0)α−α∫tt0¯Q(s)−Q(s)(t−s)α+1ds≤0, |
thus, (3.7) holds.
Next, we demand
P(t)≤BA,t≥t0. | (3.8) |
Otherwise, from (3.6) and (3.7) we have
CDαt0¯Q(t)≤CDαt0Q(t)≤−AQ(t)+(t−t0+σ)αB≤−A(t−t0+σ)αP(t)+(t−t0+σ)αB<0. |
It is known that ¯Q(t) is monotonically increasing, so ¯Q′(t)≥0, then
CDαt0¯Q(t)=1Γ(1−α)∫tt0¯Q′(s)(t−s)αds≥0, |
which is a contradiction. Hence, (3.8) is true.
Therefore,
‖z(t)‖≤‖μ‖P(t)≤‖μ‖BA |
for t≥t0.
Case 3: ¯Q(ˆt)=Q(ˆt), t0≤ˆt<t, and ¯Q(s)>Q(s), for ∀s∈(ˆt,t].
Combining Cases 1 and 2, we get
P(ˆt)≤BA |
and
Q(t)<¯Q(t)=¯Q(ˆt)=Q(ˆt)=(ˆt−t0+σ)αP(ˆt)≤(ˆt−t0+σ)αBA. |
Therefore, for t≥t0
‖z(t)‖≤‖μ‖P(t)=‖μ‖Q(t)(t−t0+σ)α≤‖μ‖BA. |
In conclusion, let
T(ξ)=max{[(AξBμmin)1α−1],0}, |
then
‖z(t)‖≤‖μ‖BA≜β |
for all t≥t0+T(ξ), when ‖ψ‖C≤ξ. So, it can be inferred that then delayed FOCVNNs (2.1) is globally uniformly β-stable via control rule (3.1).
Corollary 1: If there are n positive constants μr,vr such that
ar−|Mr|−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))]μℓ>0 | (3.9) |
and
ar−|Mr|−1vrn∑ℓ=1[|bRrℓ|(FIRℓ+FIIℓ)+|bIrℓ|(FRRℓ+FRIℓ)+(|dRrℓ|(GIRℓ+GIIℓ)+|dIrℓ|(GRRℓ+GRIℓ))]vℓ>0 | (3.10) |
hold, then delayed FOCVNNs (2.1) is globally uniformly fixed-deviation stable via control rule (3.1).
Proof: Let
L(ϑ)=ar−|Mr|−1−α+α2ϑαΓ(2−α)−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))(ϑ−ϖ+ϑ)α]μℓ, |
X(ϑ)=ar−|Mr|−1−α+α2ϑαΓ(2−α)−1vrn∑ℓ=1[|bRrℓ|(FIRℓ+FIIℓ)+|bIrℓ|(FRRℓ+FRIℓ)+(|dRrℓ|(GIRℓ+GIIℓ)+|dIrℓ|(GRRℓ+GRIℓ))(ϑ−ϖ+ϑ)α]vℓ, |
where ϑ>ϖ, then from conditions (3.9), (3.10),
limϑ→+∞L(ϑ)=ar−|Mr|−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))]μℓ>0, |
limϑ→+∞X(ϑ)=ar−|Mr|−1vrn∑ℓ=1[|bRrℓ|(FIRℓ+FIIℓ)+|bIrℓ|(FRRℓ+FRIℓ)+(|dRrℓ|(GIRℓ+GIIℓ)+|dIrℓ|(GRRℓ+GRIℓ))]vℓ>0. |
By the property of the limit, there is a constant σ>ϖ such that L(σ)>0 and X(σ)>0. So (3.3) and (3.4) hold. The proof is completed.
Regard the following system (3.11) as the drive system,
CDαt0zk(t)=−akzk(t)+n∑ℓ=1bkℓfℓ(zℓ(t))+n∑ℓ=1dkℓgℓ(zℓ(t−ϖkℓ(t))), | (3.11) |
and the response system is defined by the following:
CDαt0˜zk(t)=−ak˜zk(t)+n∑ℓ=1bkℓfℓ(˜zℓ(t))+n∑ℓ=1dkℓgℓ(˜zℓ(t−ϖkℓ(t)))+Uk(t). | (3.12) |
where ˜zk(t)=˜zRk(t)+i˜zIk(t).
The initial values of system (3.12) is given by
˜zk(t0+s)=˜ψRk(s)+˜ψIk(s),−ϖ≤s≤0. |
Define Λk(t)=˜zk(t)−zk(t),
ΛRk(t)=˜zRk(t)−zRk(t),ΛIk(t)=˜zIk(t)−zIk(t), |
then we consider the following error system
CDαt0Λk(t)=−akΛk(t)+n∑ℓ=1bkℓfℓ(Λℓ(t))+n∑ℓ=1dkℓgℓ(Λℓ(t−ϖkℓ(t)))+Uk(t), | (3.13) |
where
fℓ(Λℓ(t))=fℓ(˜zℓ(t))−fℓ(zℓ(t)),gℓ(Λℓ(t−ϖkℓ(t)))=gℓ(˜zℓ(t−ϖkℓ(t)))−gℓ(zℓ(t−ϖkl(t))). |
The initial value of the error system (3.13) is noted in the following form:
Λk(t0+s)=˜ψk(s)−ψk(s)=Ψk(s),−ϖ≤s≤0. |
For error system (3.13), we construct the following controller:
Uk(t)=MkΛk(t)+Nk[sgn(ΛRk(t))+isgn(ΛIk(t))]. | (3.14) |
Thus by controller (3.14), system (3.13) is converted as
CDαt0ΛRk(t)=−akΛRk(t)+n∑ℓ=1bRkℓfRℓ(Λℓ(t))−n∑ℓ=1bIkℓfIℓ(Λℓ(t))+n∑ℓ=1dRkℓgRℓ(Λℓ(t−ϖkℓ(t)))−n∑ℓ=1dIkℓgIℓ(Λℓ(t−ϖkℓ(t)))+MkΛRk(t)+Nksgn(ΛRk(t)),CDαt0ΛIk(t)=−akΛIk(t)+n∑ℓ=1bRkℓfIℓ(Λℓ(t))+n∑ℓ=1bIkℓfRℓ(Λℓ(t))+n∑ℓ=1dRkℓgIℓ(Λℓ(t−ϖkℓ(t)))+n∑ℓ=1dIkℓgRℓ(Λℓ(t−ϖkℓ(t)))+MkΛIk(t)+Nksgn(ΛIk(t)). | (3.15) |
Under assumption (ii), the following inequality holds:
{|fRℓ(Λℓ(t))|≤FRRℓ|ΛRℓ(t)|+FRIℓ|ΛIℓ(t)||fIℓ(Λℓ(t))|≤FIRℓ|ΛRℓ(t)|+FIIℓ|ΛIℓ(t)||gRℓ(Λℓ(t−ϖkℓ(t)))|≤GRRℓ|ΛRℓ(t−ϖkℓ(t))|+GRIℓ|ΛIℓ(t−ϖkℓ(t))||gIℓ(Λℓ(t−ϖkℓ(t)))|≤GIRℓ|ΛRℓ(t−ϖkℓ(t))|+GIIℓ|ΛIℓ(t−ϖkℓ(t))|. | (3.16) |
Theorem 2: If there are positive constants σ>ϖ≥0 and μr>0,vr>0(r=1,⋯,n) such that the following conditions
ar−|Mr|−1−α+α2σαΓ(2−α)−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))(σ−ϖ+σ)α]μℓ>0 | (3.17) |
and
ar−|Mr|−1−α+α2σαΓ(2−α)−1vrn∑ℓ=1[|bRrℓ|(FIRℓ+FIIℓ)+|bIrℓ|(FRRℓ+FRIℓ)+(|dRrℓ|(GIRℓ+GIIℓ)+|dIrℓ|(GRRℓ+GRIℓ))(σ−ϖ+σ)α]vℓ>0 | (3.18) |
hold, then delayed FOCVNNs (3.15) is globally uniformly β-stable. In other words, fixed-deviation synchronization between the drive system (3.11) and the response system (3.12) can be achieved.
Proof: Construct an auxiliary function as follows
P(t)=max1≤k≤nmax{|ΛRk(t)|μk,|ΛIk(t)|vk}. |
Let
Q(t)=(t−t0+σ)αP(t),¯Q(t)=supt0−σ≤s≤tQ(s). |
There exists r∈{1,⋯,n} for given t≥t0 having
P(t)=max{|ΛRr(t)|μr,|ΛIr(t)|vr}. |
Then we get P(t)=|ΛRr(t)|μr, P(t)=|ΛIr(t)|vr. Now, we let P(t)=|ΛRr(t)|μr, another case is similar. By (3.15) and (3.16) it follows that
CDαt0P(t)=1μrCDαt0|ΛRr(t)|≤sgn(ΛRr(t))μrCDαt0ΛRr(t)≤−(ar−|Mr|)μr|ΛRr(t)|+|Nr|μr+1μrn∑ℓ=1|bRrℓ|(FRRℓ|ΛRℓ(t)|+FRIℓ|ΛIℓ(t)|)+1μrn∑ℓ=1|bIrℓ|(FIRℓ|ΛRℓ(t)|+FIIℓ|ΛIℓ(t)|)+1μrn∑ℓ=1|dRrℓ|(GRRℓ|ΛRℓ(t−ϖrℓ(t))|+GRIℓ|ΛIℓ(t−ϖrℓ(t))|)+1μrn∑ℓ=1|dIrℓ|(GIRℓ|ΛRℓ(t−ϖrℓ(t))|+GIIℓ|ΛIℓ(t−ϖrℓ(t))|)≤−(ar−|Mr|)P(t)+|Nr|μr+1μrn∑ℓ=1|bRrℓ|(FRRℓ+FRIℓ)μℓP(t)+1μrn∑ℓ=1|bIrℓ|(FIRℓ+FIIℓ)μℓP(t)+1μrn∑ℓ=1|dRrℓ|(GRRℓ+GRIℓ)μℓP(t−ϖrℓ(t))+1μrn∑ℓ=1|dIrℓ|(GIRℓ+GIIℓ)μℓP(t−ϖrℓ(t))={−(ar−|Mr|)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)]μℓ}P(t)+1μrn∑ℓ=1[|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ)]μℓP(t−ϖrℓ(t))+|Nr|μr. | (3.19) |
By applying Lemma 2 and (3.19), we have
CDαt0Q(t)≤(t−t0+σ)αCDαt0P(t)+1−α+α2σαΓ(2−α)¯Q(t)≤{−(ar−|Mr|)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)]μℓ}Q(t)+1μrn∑ℓ=1[|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ)]μℓ(t−t0+σt−ϖrℓ(t)−t0+σ)αQ(t−ϖrℓ(t))+(t−t0+σ)α|Nr|μr+1−α+α2σαΓ(2−α)¯Q(t)≤{−(ar−|Mr|)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)]μℓ}Q(t)+1μrn∑ℓ=1[|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ)]μℓ(t−t0+σt−ϖrℓ(t)−t0+σ)α¯Q(t)+(t−t0+σ)α|Nr|μr+1−α+α2σαΓ(2−α)¯Q(t). |
It is known that σ+EE−ϖrℓ(t)+σ is monotone non-increasing for E≥0, and thus
t−t0+σt−ϖrℓ(t)−t0+σ≤σ−ϖrℓ(t)+σ≤σ−ϖ+σ, |
therefore,
CDαt0Q(t)≤{−(ar−|Mr|)+1−α+α2σαΓ(2−α)+1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))(σ−ϖ+σ)α]μℓ}Q(t)+(t−t0+σ)α|Nr|μr≤−AQ(t)+(t−t0+σ)αB, | (3.20) |
when Q(t)=¯Q(t), for t≥t0, where
A≜min1≤r≤n{ar−|Mr|−1−α+α2σαΓ(2−α)−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))(σ−ϖ+σ)α]μℓ},B≜max1≤r≤n(|Nr|μr). |
Similar to cases 1–3 in Theorem 1, we finally obtain
‖z(t)‖≤‖μ‖BA≜β |
for all t≥t0+T(ξ), when ‖Ψ‖C≤ξ, where
T(ξ)=max{[(AξBμmin)1α−1],0}. |
So, fixed-deviation synchronization between the drive system (3.11) and the response system (3.12) can be achieved.
Corollary 2: If there are n positive constants μr,vr such that
ar−|Mr|−1μrn∑ℓ=1[|bRrℓ|(FRRℓ+FRIℓ)+|bIrℓ|(FIRℓ+FIIℓ)+(|dRrℓ|(GRRℓ+GRIℓ)+|dIrℓ|(GIRℓ+GIIℓ))]μℓ>0 | (3.21) |
and
ar−|Mr|−1vrn∑ℓ=1[|bRrℓ|(FIRℓ+FIIℓ)+|bIrℓ|(FRRℓ+FRIℓ)+(|dRrℓ|(GIRℓ+GIIℓ)+|dIrℓ|(GRRℓ+GRIℓ))]vℓ>0 | (3.22) |
hold, then delayed FOCVNNs (3.15) is globally uniformly β-stable. In other words, fixed-deviation synchronization between the drive system (3.11) and the response system (3.12) can be achieved.
Proof: The proof of Corollary 2 is similar to the proof of Corollary 1.
Example 1: We consider the following delayed FOCVNNs:
CD0.9t0zk(t)=−2z1(t)+b11f1(z1(t))+b12f2(z2(t))+d11g1(z1(t−1))+d12g2(z2(t−1))+U1(t), |
CD0.9t0zk(t)=−4z2(t)+b21f1(z1(t))+b22f2(z2(t))+d21g1(z1(t−1))+d22g2(z2(t−1))+U2(t), | (4.1) |
where t0=0, zk(t)=zRk(t)+izIk(t), fℓ(zℓ)=gℓ(zℓ)=tanh(zRℓ)+tanh(zIℓ)i, ℓ=1,2,
B=(bkℓ)2×2=(0.03+0.05i−0.05+0.04i0.02−0.01i−0.03+0.02i),D=(dkℓ)2×2=(−0.07−0.02i0.03+0.01i−0.05+0.03i0.01+0.05i). |
It's not hard to choose that FRRℓ+FRIℓ=FIRℓ+FIIℓ=2, GRRℓ+GRIℓ=GIRℓ+GIIℓ=2.
Let M1=0.06, M2=0.04, σ=10, μ1=μ2=1, v1=v2=1, then (3.3) and (3.4) hold. Hence, system (4.1) is globally uniformly β-stable from Theorem 1. Figure 1 shows the numerical simulation of FOCVNNs (4.1) under discontinuous control rules U1(t)=0.06z1(t)+1.19[sgn(zR1(t))+isgn(zI1(t))] and U2(t)=0.04z2(t)+1.19[sgn(zR2(t))+isgn(zI2(t))].
Example 2: Regard the following FOCVNNs (4.2) as the drive system:
CD0.95t0zk(t)=−5z1(t)+b11f1(z1(t))+b12f2(z2(t))+d11g1(z1(t−1))+d12g2(z2(t−1)), |
CD0.95t0zk(t)=−3z2(t)+b21f1(z1(t))+b22f2(z2(t))+d21g1(z1(t−1))+d22g2(z2(t−1)), | (4.2) |
where t0=0, fℓ(zℓ)=gℓ(zℓ)=cos(zRℓ)+cos(zIℓ)i, ℓ=1,2,
B=(bkℓ)2×2=(−0.02+0.05i0.04+0.06i0.02−0.01i−0.07+0.09i),D=(dkℓ)2×2=(0.03−0.02i−0.08+0.09i−0.05+0.03i0.01+0.05i). |
The response system is given by
CD0.95t0˜zk(t)=−5˜z1(t)+b11f1(˜z1(t))+b12f2(˜z2(t))+d11g1(˜z1(t−1))+d12g2(˜z2(t−1))+U1(t), |
CD0.95t0˜zk(t)=−3z2(t)+b21f1(˜z1(t))+b22f2(˜z2(t))+d21g1(˜z1(t−1))+d22g2(˜z2(t−1))+U2(t), | (4.3) |
where the parameters bkℓ, dkℓ, fℓ(⋅), gℓ(⋅) are all the same as in FOCVNNs (4.2).
As above choose that FRRℓ+FRIℓ=FIRℓ+FIIℓ=2, GRRℓ+GRIℓ=GIRℓ+GIIℓ=2.
Let M1=0.02, M2=0.04, σ=20, μ1=μ2=1, v1=v2=1, then (3.17) and (3.18) hold. Hence, it can be seen that drive system (4.2) and response system (4.3) are fixed-deviation synchronization from Theorem 2. Figure 2 shows the numerical simulation of error system under discontinuous control rules U1(t)=0.02Λ1(t)+2.22[sgn(ΛR1(t))+isgn(ΛI1(t))] and U2(t)=0.04Λ2(t)+2.22[sgn(ΛR2(t))+isgn(ΛI2(t))].
This paper discusses fixed-deviation stability and synchronization of FOCVNNs. The system investigated in this paper is a continuous neural network, and a discontinuous controller is introduced to address this problem. Under the discontinuous controller, fixed-deviation stability theory and fractional calculus method are used to observe the fixed-deviation dynamical behavior of delayed FOCVNNs. In this paper, a continuous system is transformed into a discontinuous system by imposing a discontinuous controller to achieve fixed-deviation dynamics, this technique can be extended to other more complex systems, which would be a future direction of research.
This work is supported by the Natural Science Foundation of China under Grant 61976084, the Natural Science Foundation of Hubei Province of China under Grant 2021CFA080, the Young Top-Notch Talent Cultivation Program of Hubei Province of China.
The authors declare there is no conflict of interest.
[1] |
V. V. Kulish, J. L. Lage, Application of fractional calculus to fluid mechanics, J. Fluids Eng., 124 (2002), 803–806. https://doi.org/10.1115/1.1478062 doi: 10.1115/1.1478062
![]() |
[2] |
J. M. Balthazar, P. B. Goncalves, S. Lenci, Y. V. Mikhlin, Models, methods, and applications of dynamics and control in engineering sciences: state of the art, Math. Probl. Eng., 2010 (2010), 487684. https://doi.org/10.1155/2010/487684 doi: 10.1155/2010/487684
![]() |
[3] |
P. Panda, M. Dash, Fractional generalized splines and signal processing, Signal Process., 86 (2006), 2340–2350. https://doi.org/10.1016/j.sigpro.2005.10.017 doi: 10.1016/j.sigpro.2005.10.017
![]() |
[4] |
M. S. Aslam, M. A. Z. Raja, A new adaptive strategy to improve online secondary path modeling in active noise control systems using fractional signal processing approach, Signal Process., 107 (2015), 433–443. https://doi.org/10.1016/j.sigpro.2014.04.012 doi: 10.1016/j.sigpro.2014.04.012
![]() |
[5] |
C. J. Z. Aguilar, J. F. Gmez-Aguilar, V. M. Alvarado-Martnez, H. M. Romero-Ugalde, Fractional order neural networks for system identification, Chaos, Solitons Fractals, 130 (2020), 109444. https://doi.org/10.1016/j.chaos.2019.109444 doi: 10.1016/j.chaos.2019.109444
![]() |
[6] |
S. Fazzino, R. Caponetto, L. Patanè, A new model of Hopfield network with fractional-order neurons for parameter estimation, Nonlinear Dyn., 104 (2021), 2671–2685. https://doi.org/10.1007/s11071-021-06398-z doi: 10.1007/s11071-021-06398-z
![]() |
[7] |
Y. Liu, Y. Sun, L. Liu, Stability analysis and synchronization control of fractional-order inertial neural networks with time-varying delay, IEEE Access, 10 (2022), 56081–56093. https://doi.org/10.1109/ACCESS.2022.3178123 doi: 10.1109/ACCESS.2022.3178123
![]() |
[8] |
E. Kaslik, S. Sivasundaram, Nonlinear dynamics and chaos in fractional-order neural networks, Neural Networks, 32 (2012), 245–256. https://doi.org/10.1016/j.neunet.2012.02.030 doi: 10.1016/j.neunet.2012.02.030
![]() |
[9] |
H. Wang, Y. Yu, G. Wen, S. Zhan, J. Yu, Global stability analysis of fractional-order Hopfield neural networks with time delay, Neurocomputing, 154 (2015), 15–23. https://doi.org/10.1016/j.neucom.2014.12.031 doi: 10.1016/j.neucom.2014.12.031
![]() |
[10] |
C. Huang, J. Wang, X. Chen, J. Cao, Bifurcations in a fractional-order BAM neural network with four different delays, Neural Networks, 141 (2021), 344–354. https://doi.org/10.1016/j.neunet.2021.04.005 doi: 10.1016/j.neunet.2021.04.005
![]() |
[11] |
C. Xu, D. Mu, Z. Liu, Y. Pang, M. Liao, C. Aouiti, New insight into bifurcation of fractional-order 4D neural networks incorporating two different time delays, Commun. Nonlinear Sci. Numer. Simul., 118 (2023), 107043. https://doi.org/10.1016/j.cnsns.2022.107043 doi: 10.1016/j.cnsns.2022.107043
![]() |
[12] |
C. Huang, H. Liu, X. Shi, X. Chen, M. Xiao, Z. Wang, et al., Bifurcations in a fractional-order neural network with multiple leakage delays, Neural Networks, 131 (2020), 115–126. https://doi.org/10.1016/j.neunet.2020.07.015 doi: 10.1016/j.neunet.2020.07.015
![]() |
[13] | C. Xu, W. Zhang, C. Aouiti, Z. Liu, L. Yao, Bifurcation insight for a fractional-order stage-structured predator-prey system incorporating mixed time delays, Math. Methods Appl. Sci., 2023. https://doi.org/10.1002/mma.9041 |
[14] |
C. Xu, D. Mu, Z. Liu, Y. Pang, M. Liao, P. Li, et al., Comparative exploration on bifurcation behavior for integer-order and fractional-order delayed BAM neural networks, Nonlinear Anal. Modell. Control, 27 (2022), 1030–1053. https://doi.org/10.15388/namc.2022.27.28491 doi: 10.15388/namc.2022.27.28491
![]() |
[15] |
C. Xu, Z. Liu, Y. Pang, S. Saifullah, J. Khan, Torus and fixed point attractors of a new hyperchaotic 4D system, J. Comput. Sci., 67 (2023), 101974. https://doi.org/10.1016/j.jocs.2023.101974 doi: 10.1016/j.jocs.2023.101974
![]() |
[16] |
C. Xu, M. Rahman, D. Baleanu, On fractional-order symmetric oscillator with offset-boosting control, Nonlinear Anal. Modell. Control, 27 (2022), 1–15. https://doi.org/10.15388/namc.2022.27.28279 doi: 10.15388/namc.2022.27.28279
![]() |
[17] |
C. Xu, W. Alhejaili, S. Saifullah, A. Khan, J. Khan, M. A. El-Shorbagy, Analysis of Huanglongbing disease model with a novel fractional piecewise approach, Chaos Solitons Fractals, 161 (2022), 112316. https://doi.org/10.1016/j.chaos.2022.112316 doi: 10.1016/j.chaos.2022.112316
![]() |
[18] |
F. Zhang, Z. Zeng, Asymptotic stability and synchronization of fractional-order neural networks with unbounded time-varying delays, IEEE Trans. Syst. Man Cybern. Syst., 51 (2021), 5547–5556. https://doi.org/10.1109/TSMC.2019.2956320 doi: 10.1109/TSMC.2019.2956320
![]() |
[19] |
Z. Ding, Z. Zeng, L. Wang, Robust finite-time stabilization of fractional-order neural networks with discontinuous and continuous activation functions under uncertainty, IEEE Trans. Neural Networks Learn. Syst., 29 (2018), 1477–1490. https://doi.org/10.1109/TNNLS.2017.2675442 doi: 10.1109/TNNLS.2017.2675442
![]() |
[20] | W. Rudin, Real and Complex Analysis, Mcgraw-Hill, New York, 1987. |
[21] |
X. Ding, J. Cao, X. Zhao, F. E. Alsaadi, Finite-time stability of fractional-order complex-valued neural networks with time delays, Neural Process. Lett., 46 (2017), 561–580. https://doi.org/10.1007/s11063-017-9604-8 doi: 10.1007/s11063-017-9604-8
![]() |
[22] |
T. Hu, Z. He, X. Zhang, S. Zhong, Finite-time stability for fractional-order complex-valued neural networks with time delay, Appl. Math. Comput., 365 (2020), 124715. https://doi.org/10.1016/j.amc.2019.124715 doi: 10.1016/j.amc.2019.124715
![]() |
[23] |
P. Wan, J. Jian, Impulsive stabilization and synchronization of fractional-order complex-valued neural networks, Neural Process. Lett., 50 (2019), 2201–2218. https://doi.org/10.1007/s11063-019-10002-2 doi: 10.1007/s11063-019-10002-2
![]() |
[24] |
X. You, Q. Song, Z. Zhao, Global Mittag-Leffler stability and synchronization of discrete-time fractional-order complex-valued neural networks with time delay, Neural Networks, 122 (2020), 382–394. https://doi.org/10.1016/j.neunet.2019.11.004 doi: 10.1016/j.neunet.2019.11.004
![]() |
[25] |
J. Chen, B. Chen, Z. Zeng, Global asymptotic stability and adaptive ultimate Mittag-Leffler synchronization for a fractional-order complex-valued memristive neural networks with delays, IEEE Trans. Syst. Man Cybern. Syst., 49 (2019), 2519–2535. https://doi.org/10.1109/TSMC.2018.2836952 doi: 10.1109/TSMC.2018.2836952
![]() |
[26] |
X. Li, J. Wu, Stability of nonlinear differential systems with state-dependent delayed impulses, Automatica, 64 (2016), 63–69. https://doi.org/10.1016/j.automatica.2015.10.002 doi: 10.1016/j.automatica.2015.10.002
![]() |
[27] |
X. Li, S. Song, Stabilization of delay systems: delay-dependent impulsive control, IEEE Trans. Autom. Control, 62 (2017), 406–411. https://doi.org/10.1109/TAC.2016.2530041 doi: 10.1109/TAC.2016.2530041
![]() |
[28] |
H. Bao, J. H. Park, J. Cao, Synchronization of fractional-order complex-valued neural networks with time delay, Neural Networks, 81 (2016), 16–28. https://doi.org/10.1016/j.neunet.2016.05.003 doi: 10.1016/j.neunet.2016.05.003
![]() |
[29] |
X. Liu, Y. Yu, Synchronization analysis for discrete fractional-order complex-valued neural networks with time delays, Neural Comput. Appl., 33 (2021), 10503–10514. https://doi.org/10.1007/s00521-021-05808-y doi: 10.1007/s00521-021-05808-y
![]() |
[30] |
J. Chen, B. Chen, Z. Zeng, Global uniform asymptotic fixed-deviation stability and stability for delayed fractional-order memristive neural networks with generic memductance, Neural Networks, 98 (2018), 65–75. https://doi.org/10.1016/j.neunet.2017.11.004 doi: 10.1016/j.neunet.2017.11.004
![]() |
[31] |
J. Zhang, Linear-type discontinuous control of fixed-deviation stabilization and synchronization for fractional-order neurodynamic systems with communication delays, IEEE Access, 6 (2018), 52570–52581. https://doi.org/10.1109/ACCESS.2018.2870979 doi: 10.1109/ACCESS.2018.2870979
![]() |
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