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Comparative analysis on bifurcation of fourneuron fractional ring networks without or with leakage delays
Advances in Difference Equations volume 2019, Article number: 179 (2019)
Abstract
This paper is concerned with the problem of bifurcation for a ring fractional Hopfield neural network with leakage time delay and communication time delay. The stability and the Hopf bifurcations of such a network without and with time delays are investigated by analyzing the associated characteristic equations. Specifically, some criteria for the occurrence of Hopf bifurcations at the trivial steady state are established. It is shown that the dynamical property of the network is not only crucially dependent on the communication time delay, but also significantly influenced by the leakage time delay. Furthermore, the effects of the order on the Hopf bifurcation are numerically demonstrated. Finally, four numerical examples are provided to illustrate the feasibility of the theoretical results.
1 Introduction
The studies for various Hopfield neural networks (HNNs) have been continuously active over the past three decades because of their successful applications in numerous areas, for instance, optimizations, signal processing, image processing, solving nonlinear algebraic equations, pattern recognitions, associative memories [1,2,3,4,5]. Since the applications of HNNs rely heavily on network dynamics, many efforts have been undertaken to investigate their dynamical properties and a lot of valuable results have been reported, including stability [6], oscillation [7], bifurcation [8,9,10], chaos [11], and synchronization [12, 13] and the references.
One major and often encountered difficulty in the analysis of neural network dynamics is the ubiquity of time delays that can result in instability, oscillation, periodic solution, antiperiodic solution, almost periodic solution, quasiperiodic solution, and even give rise to multistability and chaotic motion. Among them, the time delays resulting from the communication and response of neurons are regarded as a critical player due to the finite switching speed of amplifiers and the noninstantaneous signal transmission between neurons [14]. Over the years, the study of dynamics of HNNs or population with such time delays has received considerable interest of many researchers [2,3,4,5, 7, 11, 15]. Additionally, it has been observed that a typical time delay called leakage delay also has important consequences on dynamics of neural networks [16,17,18,19,20,21]. In particular, the leakage delay in a negative feedback terms can drive a stable system to be unstable [22]. It is therefore also of great significance to clarify the dynamics of HNNs subject to leakage delays.
In 2009, Hu and Huang [23] investigated a ring of HNN with four neurons and delays, which is described as follows:
where \(\dot{x}=\mathrm{d}x/\mathrm{d}t\); \(x_{i}(t)\) represents the state of the ith neuron at time t; \(r_{i}\geq 0\) is the internal decay rate; \(f_{i}\) is the connection function between neurons; \(g_{i}\) represents the nonlinear feedback function; \(\tau _{j}\geq 0\) is the communication time delay; and \(i=1,2,3,4\), \(j=1,2\). By using the associated characteristic equation, the stability and Hopf bifurcations of the HNN are studied, as well as the stability and direction on the Hopf bifurcation are determined by employing the normal form method and the center manifold reduction. For more ring networks research results, one can read the references [8, 24,25,26] and the references cited therein.
Fractional calculus, a classical mathematical notion that has a history of over 300 years, is a generalization of the ordinary differentiation and integration to arbitrary noninteger order, having been demonstrated to play important roles in physics, biology and engineering [27,28,29,30,31,32,33,34,35]. In fact, the importance of fractional calculus is reflected in three main points: first, the orders of derivatives and integrals in fractional calculus are real numbers; second, fractionalorder derivative acts as an effective measure for the description of memory and hereditary properties of various materials and processes; and third, the fractionalorder derivative makes a real object models more accurately than the integer order. Based on these advantages, fractional calculus has been proposed to model, design, and control various neural networks in recent years. For instance, several works concerning fractional neural networks have appeared recently: undamped oscillations generated by Hopf bifurcations in fractionalorder recurrent neural networks with Caputo derivative were studied in [36, 37]; for a fractional BAM neural network with leakage delay, conditions for the Hopf bifurcation were discussed in [38], and so on.
Oscillations are ubiquitous in dynamic neuronal networks and play critical roles in fundamental processes such as controlling dynamics of neurons at subthreshold potentials, regulating rhythmic neuronal ensembles within local networks, and determining global oscillations measured by electroencephalography [12]. It is well known that Hopf bifurcations, which include supercritical and subcritical Hopf bifurcations, can help us to efficiently design biochemical oscillators. In this regard, it is important to note that most of the results on Hopf bifurcation theory of integerorder neural networks cannot be simply generalized to those for the cases of fractional neural networks because of the substantial differences between integerorder system and fractionalorder system. To the best of our knowledge, up to today only a few results on the Hopf bifurcation of fractionalorder system have been reported, and thus, it is still an open problem to study Hopf bifurcations of fractionalorder dynamical systems [39]. This finding motivates the search for the properties of bifurcated oscillations of a ring of fractionalorder neural network with four neurons further.
Based on the above motivations, the present work is devoted to the study of stability and Hopf bifurcation for a delayed ring of fractionalorder neural network with four neurons and leakage delays. The main contributions can be summarized in three aspects:

(1)
A new delayed fourneuron fractionalorder ring network with leakage delays is proposed.

(2)
Two important dynamical properties—stability and oscillation—of the four neurons fractionalorder ring networks without and with explicit leakage delays are investigated.

(3)
The effects of the order on the Hopf bifurcation are discussed.
The rest of this paper is organized as follows. In Sect. 2, several definitions and lemma of fractionalorder calculus are recalled. In Sect. 3, the discussed models are proposed. In Sect. 4, by analyzing the associated characteristic equation, the local stability of the trivial steady state for the delayed fractionalorder HNN is examined. Moreover, the existence of the Hopf bifurcation of the delayed fractionalorder HNN without and with leakage time delays is established. In Sect. 5, illustrative examples are provided to demonstrate the theoretical results. Some conclusions are given in the last section.
2 Preliminaries
In this section, we introduce some definitions and lemmas of fractional derivatives, which serve as a basis for the proofs of the main result of Sect. 4.
Generally, there exist mainly three widely used fractional operators, namely the Grünwald–Letnikov definition, the Riemann–Liouville definition, and the Caputo definition. Since the Caputo derivative only requires the initial conditions, which are based on integerorder derivative and represents wellunderstood features of physical situation, it is more applicable to real world problems. With this notion in mind, we shall use the Caputo fractionalorder derivative to model and analyze the stability of the proposed fractionalorder algorithms in this paper.
Definition 2.1
([28])
The fractional integral of order ϕ for a function \(g(t)\) is defined as follows:
here, \(t\geq t_{0}\), \(\phi >0\), and \(\varGamma (\cdot )\) is the gamma function satisfying \(\varGamma (s)=\int _{0}^{\infty }t^{s1}e^{t}\,d \mathrm{t}\).
Definition 2.2
([28])
Caputo fractional derivative of order ϕ for a function \(g(t)\in C^{n}([t_{0}, \infty ),R)\) is defined in the following form:
here, \(t\geq t_{0}\), and \(n1\leq \phi < n\), \(n\in N^{+}\).
Moreover, if \(0<\phi <1\), then
Lemma 2.1
([29])
For the following autonomous system
in which \(0<\phi <1\), \(y\in R^{n}\), \(A\in R^{n\times n}\) is asymptotically stable if and only if \(\vert \arg (\lambda _{i}) \vert >\phi \pi /2\) (\(i=1,2,\ldots,n\)), then each component of the states decays towards 0 like \(t^{\phi }\). Furthermore, this system is stable if and only if \(\vert \arg (\lambda _{i}) \vert \geq \phi \pi /2\) and those critical eigenvalues that satisfy \(\vert \arg (\lambda _{i}) \vert =\phi \pi /2\) have geometric multiplicity one.
3 Model description
This paper considers the following ring fractional HNN with four neurons and time delays in leakage terms:
where \(\phi _{i}\in (0,1]\) (\(i=1,2,3,4\)) is fractional order; \(x_{i}(t)\) (\(i=1,2,3,4\)) represents state variables; \(r_{i}\geq 0\) (\(i=1,2,3,4\)) specifies the internal decay rate; a, \(b_{i}\), \(c_{i}\) (\(i=1,2,3,4\)) denote the connection weights; \(f_{i}(\cdot )\) is the connection function between neurons; \(g_{i}(\cdot )\) (\(i=1,2,3,4\)) represents the nonlinear feedback function; σ is the leakage delay; \(\tau _{1}\) and \(\tau _{2}\) are the communication time delays.
Remark 3.1
In fact, if \(\phi _{i}=1\) (\(i=1,2,3,4\)), the fractionalorder system (3.1) changes into the following integerorder system:
In this work, for the sake of simplicity, we discuss the fractionalorder system (3.1) when \(\sigma =\tau _{1}=\tau _{2}=\tau \), \(\phi =\phi _{1}=\phi _{2}=\phi _{3}=\phi _{4}\), and so system (3.1) can be rewritten as
Moreover, when system (3.2) does not involve leakage time delay, then system (3.2) can be described by
Accordingly, the primary objective of this paper is to study the stability and the Hopf bifurcations of networks (3.2) and (3.3) by taking time delay as the bifurcation parameter through the approach of stability analysis [27]. Moreover, the effects of the order on the creation of bifurcation for the two proposed models are also numerically discussed.
Throughout of this paper, some basic assumptions are presented first.
 \((\mathbf{C1})\) :

\(f_{i}, g_{i}\in \mathrm{C}(R,R)\), \(f_{i}(0)=g_{i}(0)=0\), \(xf_{i}(x)>0\), \(xg_{i}(x)>0\) (\(i=1,2,3,4\)) for \(x\neq 0\).
4 Stability and bifurcation analysis
4.1 Existence of bifurcation without leakage delays
In this subsection, by applying the previous analytic technique, we shall investigate the stability and bifurcation of system (3.3) by taking communication time delay as the bifurcation parameter. Accordingly, it is easy to show that the origin is an equilibrium point of system (3.3) under assumption \((\mathbf{C1})\). The linearization of (3.3) at the origin is given by
whose characteristic equation is
where \(k_{i}=r_{i}ag_{i}'(0)\), \(m_{i}=b_{i}f_{i}'(0)\), \(n_{i}=c_{i} f _{i}'(0)\) (\(i=1,2,3,4\)).
By (4.2), we have
where
Let \(P_{1}(s)=A_{1}+iB_{1}\), \(P_{2}(s)=A_{2}+iB_{2}\), \(P_{3}(s)=A_{3}\), and from Eq. (4.3), we have
Let \(s=iw=w(\cos \frac{\pi }{2}+i\sin \frac{\pi }{2})\) (\(\omega >0\)) be a root of Eq. (4.4). Substituting s into Eq. (4.4) and separating the real and imaginary parts yields the following equations:
which lead to
It is easy to see that
From (4.6), one can obtain
Define the bifurcation point
To theoretically gain the sufficient conditions for the Hopf bifurcation, we assume that the following assumptions hold:
 \((\mathbf{C2})\) :

Eq. (4.7) has no positive real root;
 \((\mathbf{C3})\) :

Eq. (4.7) has at least a positive real root.
Denote
where
Now, we will reconsider the stability of system (3.3) when \(\tau =0\). According to the Routh–Hurwitz criterion, we have the following lemma.
Lemma 4.1
If \(\tau =0\) and \(\varXi _{1}>0\), \(\varXi _{2}>0\), \(\varXi _{3}>0\), \(\varXi _{4}>0\), then system (3.3) is asymptotically stable.
Proof
When \(\tau =0\), by (4.3), we get
If the conditions of \(\varXi _{1}>0\), \(\varXi _{2}>0\), \(\varXi _{3}>0\), \(\varXi _{4}>0\) hold, then the roots \(\lambda _{i}\) of Eq. (4.4) satisfy \(\vert \arg (\lambda _{i}) \vert >\phi \pi /2\). Thus, according to Lemma 2.1, system (3.3) is asymptotically stable when \(\tau =0\). □
To throw up our main results, we further give the following assumption:
 \((\mathbf{C4})\) :

\(\frac{\varUpsilon _{1}\varOmega _{1}+\varUpsilon _{2}\varOmega _{2}}{ \varOmega _{1}^{2}+\varOmega _{2}^{2}}\neq 0\),
where
Lemma 4.2
Let \(s(\tau )=\nu (\tau )+iw(\tau )\) be a root of Eq. (4.3) near \(\tau =\tau _{j}\) satisfying \(\nu (\tau _{j})=0\), \(w(\tau _{j})=w_{0}\), then the following transversality condition holds:
Proof
By using the implicit function theorem and differentiating (4.3) with respect to τ, we have
where \(P_{i}'(s)\) is the derivative of \(P_{i}(s)\).
Noting that \(P_{3}'(s)=0\), therefore we have
where
Let \({P'}_{i}^{R}\), \({P'}_{i}^{I}\) be the real and imaginary parts of \(P_{i}(s)\) (\(i=1,2,3\)), respectively. We further suppose that \(\varUpsilon _{1}\), \(\varUpsilon _{2}\) are the real and imaginary parts of \(\varUpsilon (s)\), respectively, and \(\varOmega _{1}\), \(\varOmega _{2}\) are the real and imaginary parts of \(\varOmega (s)\), respectively, then
And from \((\mathbf{C3})\) we conclude that the transversality condition is satisfied. This completes the proof of Lemma 4.2. □
From the above analysis, we can obtain the following results.
Theorem 4.1
If system (3.3) satisfies:

(1)
Under assumptions \((\mathbf{C1})\)–\((\mathbf{C4})\), then the zero equilibrium point is globally asymptotically stable for \(\tau \in [0,+ \infty )\).

(2)
Under assumptions \((\mathbf{C1})\), \((\mathbf{C3})\), and \((\mathbf{C4})\), then

(i)
the zero equilibrium point is locally asymptotically stable for \(\tau \in [0,\tau _{0})\);

(ii)
system (3.3) undergoes a Hopf bifurcation at the origin when \(\tau =\tau _{0}\). That is, a family of periodic solutions can bifurcate from the zero equilibrium point at \(\tau =\tau _{0}\).

(i)
Theorem 4.1 shows that there is an explicit communication time delay value \(\tau =\tau _{0}\), which can determine the stability of system (3.3) and can induce oscillatory dynamics even when the deterministic counterpart of system (3.3) exhibits no oscillations.
4.2 Bifurcation analysis involving leakage delays
In this subsection, we first study the stability of system (3.2) by taking the leakage time delay as the bifurcation parameter. Then we further look for the sufficient conditions of Hopf bifurcation for the proposed system.
It is obvious that the origin is an equilibrium point of system (3.2) under assumption \((\mathbf{C1})\). The linear equation of system (3.2) at the origin is
and the associated characteristic equation of system (4.13) is
which equals to the following equation:
in which
Multiplying \(e^{4s\tau }\) on both sides of Eq. (4.15), we get
Suppose that \(h+ik=(s^{\phi }u) e^{s\tau }\) in Eq. (4.16), it follows that
Since \(Q_{i}\) are constants, for all the roots \((h+ik)\) of Eq. (4.17), the details can be seen in [38].
\(s=i\omega =\omega (\cos \frac{\pi }{2}+i\sin \frac{\pi }{2})\) (\(\omega >0\)) is a purely imaginary root of Eq. (4.17) if and only if
If \(\omega ^{2\phi }2u\omega ^{\phi }\cos \frac{\phi \pi }{2}+u^{2} \neq 0\), then by Eq. (4.18) we have that
Because \(\sin ^{2}\omega \tau +\cos ^{2}\omega \tau =1\), Eq. (4.19) implies that
By a direct computation, one can have
According to \(\cos \omega \tau =\frac{\omega ^{\phi }(h\cos \frac{ \phi \pi }{2} +k\sin \frac{\phi \pi }{2})hu}{\omega ^{2\phi }2u \omega ^{\phi }\cos \frac{\phi \pi }{2}+u^{2}}\), we obtain that
To establish the main results for system (3.2), it is necessary to make the following assumptions.
 \((\mathbf{C5})\) :

Eq. (4.21) has at least one positive real root.
For system (3.2), we define the bifurcation point as follows:
where \(\tau ^{(l)}\) is defined by (4.22).
To produce our main results, furthermore, we assume that the following condition holds:
 \((\mathbf{C6})\) :

\(\frac{\varPhi _{1}\varPsi _{1}+\varPhi _{2}\varPsi _{2}}{\varPsi _{1} ^{2}+\varPsi _{2}^{2}}\neq 0\),
where
Lemma 4.3
Let \(s(\tau )=\mu (\tau )+i\omega (\tau )\) be a root of system (3.2) near \(\tau =\tau _{j}\) satisfying \(\mu (\tau _{j})=0\), \(\omega (\tau _{j})=\omega _{0}\), then the following transversality condition holds:
Proof
Equation (4.15) can be transformed into
where \(m_{1}(s)=(s^{\alpha }\mu )^{4}\), \(m_{2}(s)=Q_{1}(s^{\alpha } \mu )^{3}\), \(m_{3}(s)=Q_{2}(s^{\alpha }\mu )^{2}\), \(m_{4}(s)=Q_{3}(s ^{\alpha }\mu )\), \(m_{5}(s)=Q_{4}\).
Based on the implicit function theorem and differentiating (4.23) with respect to τ, it reads
where \(m_{i}'(s)\) are the derivatives of \(m_{i}(s)\).
Based on Eq. (4.23) and \(m_{5}'(s)=0\), one can have
where
Let \({m'}_{i}^{R}\), \({m'}_{i}^{I}\) be the real and imaginary parts of \(m_{i}(s)\) (\(i=1,2,3\)), respectively; \(\varPhi _{1}\), \(\varPhi _{2}\) be the real and imaginary parts of \(\varPhi (s)\), respectively; and \(\varPsi _{1}\), \(\varPsi _{2}\) be the real and imaginary parts of \(\varPsi (s)\), respectively, then it can be derived from (4.25) that
From \((\mathbf{C6})\), we can conclude that the transversality condition is met. □
Assume that \((\mathbf{C1})\), \((\mathbf{C5})\)–\((\mathbf{C6})\), Lemma 2.1, and Lemma 4.3 hold, we can obtain the following theorem.
Theorem 4.2
For system (3.2), the following results hold:

(1)
If \((\mathbf{C1})\) and \((\mathbf{C5})\) are satisfied, then the zero equilibrium point is globally asymptotically stable for \(\tau \in [0,+\infty )\).

(2)
If \((\mathbf{C1})\), \((\mathbf{C5})\)–\((\mathbf{C6})\) hold, then

(i)
the zero equilibrium point is locally asymptotically stable for \(\tau \in [0,\tau _{0}^{*})\);

(ii)
system (3.2) undergoes a Hopf bifurcation at the origin when \(\tau =\tau _{0}^{*}\), i.e., it has one branch of periodic solutions bifurcating from the zero equilibrium point near \(\tau =\tau _{0}^{*}\).

(i)
This theorem demonstrates that the stability and the Hopf bifurcation of the neural network are not only crucially dependent on the communication delays, but also heavily influenced by the leakage delay. It is therefore essential for considering the effects of communication and leakage delays in designing or controlling neural networks.
5 Illustrative examples
In this section, we give several examples to show the feasibility and effectiveness of the results obtained in this paper. All of the simulation results are based on Adama–Bashforth–Moulton predictorcorrector scheme [40] with steplength \(h=0.01\).
5.1 Example 1
Consider the following system without leakage delays:
In this case, let \(\phi =0.92\), and the initial values are selected as \((x_{1}(0),x_{2}(0),y_{1}(0),y_{2}(0))=(0.2,0.1,0.2,0.1)\). By computing, we get \(\omega _{0}=1.1675\), and then \(\tau _{0}=0.5421\). Obviously, system (5.1) at the zero equilibrium point is locally asymptotically stable when \(\tau =0.47<\tau _{0}\), as shown in Figs. 1–2. Furthermore, Figs. 3–4 display that the zero equilibrium point of system (5.1) is unstable, and Hopf bifurcation occurs when \(\tau =0.6>\tau _{0}\).
5.2 Example 2
For making a comparison with Example 1, let \(\phi =0.92\), and now we consider the following system with leakage delays:
By a simple calculation, we have \(\omega _{0}=1.5554\), \(\tau _{0}^{*}=0.3976\). Therefore, the zero equilibrium point of system (5.2) is locally asymptotically stable when \(\tau =0.36<\tau _{0}\), as described in Figs. 5–6. Furthermore, the zero equilibrium point of system (5.2) is unstable, and Hopf bifurcation occurs when \(\tau =0.42> \tau _{0}^{*}\), as depicted in Figs. 7–8.
To better reflect the impact of leakage delay on the bifurcation point for system (5.2), the corresponding bifurcation point \(\tau _{0}\), \(\tau _{0}^{*}\) can be determined as the order ϕ varies. It can be seen from Fig. 9 that the values of \(\tau _{0}\) are larger than the case of \(\tau _{0}^{*}\) for the same order ϕ. This implies that Hopf bifurcation easily occurs in advance for system (5.2) involving leakage delay compared with system (5.1) for some fixed order ϕ.
5.3 Example 3
Consider the following system without leakage delays:
Taking the order and initial values as \(\phi =0.96\) and \((x_{1}(0),x _{2}(0),x_{3}(0),x_{4}(0))=(0.05, 0.05, 0.05,0.05)\), respectively, we can have \(\omega _{0}=1.8697\), and then \(\tau _{0}=0.4486\). Thus, the zero equilibrium point of system (3.2) is global asymptotically stable when \(\tau =0.38<\tau _{0}\) (see Figs. 10–11), and when \(\tau =0.46>\tau _{0}\), system (5.3) at the zero equilibrium point is unstable (see Figs. 12–13).
If leakage delay is considered in system (5.3), we will give the following example to demonstrate its impact.
5.4 Example 4
Consider the following system with leakage delays:
The same order and initial values are chosen as those in system (5.3). We now get \(\omega _{0}=2.9997\) and \(\tau _{0}^{*}=0.2477\). Therefore, when \(\tau =0.22<\tau _{0}^{*} \), system (5.4) at the zero equilibrium point is global asymptotically stable (see Figs. 14–15); when \(\tau =0.28>\tau _{0}^{*}\), system (5.4) at the zero equilibrium point is unstable (see Figs. 16–17). Moreover, if the order ϕ varies, the corresponding \(\omega _{0}\), \(\tau _{0}^{*}\) can be obtained. It can be seen from Fig. 18 that the onset of Hopf bifurcation of system (5.4) is gradually postponed as the order increases.
6 Conclusion
In this paper, the issue of bifurcation for a ring of fractional neural networks with four neurons and time delay in leakage terms has been studied. By utilizing time delay as the bifurcation parameter, some criteria to ensure that existence of the Hopf bifurcation for the fractional four neurons networks were established. The analytic results have shown that both the leakage time delay and communication time delay can change the dynamic behavior quantitatively, for example, greatly changing the stability of equilibrium solution, further leading to Hopf bifurcation and oscillation solutions. Moreover, the impact of the order on the creation of bifurcation was also numerically demonstrated. As a continuation of the previously mentioned series of works, our results may enrich our understanding of the bifurcation for delayed ring fractional neural networks. Finally, simulation examples have been performed to illustrate the main results.
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Acknowledgements
The authors would like to thank the editor and the anonymous reviewers for their valuable comments and constructive suggestions to improve the quality of this paper.
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This work was supported by the National Natural Science Foundation of China (Grant No. 1156 1070) and the Natural Scientific Research Fund Project of Yunnan Province (Grant No. 2014 FD049).
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Li, Z., Huang, C. & Zhang, Y. Comparative analysis on bifurcation of fourneuron fractional ring networks without or with leakage delays. Adv Differ Equ 2019, 179 (2019). https://doi.org/10.1186/s1366201921144
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DOI: https://doi.org/10.1186/s1366201921144