Complex patterns of an SIR model with a saturation treatment on complex networks: An edge-compartmental approach

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Abstract

In this paper, we adopt an edge-compartmental approach to deeply investigate an SIR model with a saturation treatment on complex networks. We find that the system may exhibit the coexistence of multi-endemic equilibria, whose stabilities are determined by signs of tangent slopes of the epidemic curve. Numerical examples illustrate the theoretical results.

Introduction

In [1], Li and Yousef proposed an SIR epidemic model with a saturation treatment function complex network as follows: dSk(t)dt=ΛβkSk(t)Θ(t)μSk(t),dIk(t)dt=βkSk(t)Θ(t)rIk(t)1+αΘ(t)(μ+γ)Ik(t),dRk(t)dt=rIk(t)1+αΘ(t)+γIkμRk(t),k=1,2,,n,where Sk,Ik and Rk denote densities of susceptible nodes, infected nodes and recovered nodes at time t and degree k, respectively. Λ represents the input rate; β stands for the transmission rate; γ is the natural treatment; μ denotes the natural death rate; rIk/(1+αΘ) is a form of the saturation treatment with a delay effect α. n denotes the maximal degree of a network. Let Nk(t)=Sk(t)+Ik(t)+Rk(t) represent the subtotal population with degree k at time t and then the total population is denoted by N(t)=k=1nNk(t) at time t. The term Θ(t) represents the probability of one infected edge connecting other uninfected edges and it is defined by Θ(t)=1kk=1nkp(k)Ik(t)with average degree k=k=1nkp(k) and the degree distribution p(k)=Nk/N. Since the dimension of model (2) is 3n, the calculation and analysis processes must be tedious. Actually, epidemic models on complex networks are concerned with the variations of infected edges, which have been presented in forms of the pairwise models [2] and the edge-compartmental models [3]. In [4], Wang and Yang proposed a mixed degree-edge-compartmental model and considered the evolution of susceptible nodes and infected edges. Inspired by those ideas, we transform model (2) into dSk(t)dt=ΛβkSk(t)Θ(t)μSk(t),dΘ(t)dt=βkk=1nk2p(k)Sk(t)r1+αΘ(t)(μ+γ)Θ(t),dR(t)dt=rΘ1+αΘ(t)+γΘ(t)μR(t),k=1,2,,n,where R(t)=1kk=1nkp(k)Rk(t). Apparently, the (n+2)th equation of system (2) has no relation with other equations. Hence, we can drop it off and reconsider the following system dSk(t)dt=ΛβkSk(t)Θ(t)μSk(t),dΘ(t)dt=βkk=1nk2p(k)Sk(t)r1+αΘ(t)(μ+γ)Θ(t),k=1,2,,nwith initial conditions Sk(0)=Sk0,Θ(0)=Θ0,k=1,2,,n.Without loss of the generality, we assume that Λ=μ. In this case, Ω=ϕ(R+)n+1|0<Sk1,0Θ<1is a positively invariant set. Define the basic reproduction number of system (3) by R0=βk2(μ+γ+r)k,which characterizes that the average number of infected edges produced by one infected [SI] edge during its infected period 1μ+γ+r at total size of susceptible nodes. k2=k=1nk2p(k) denotes the two movement of the network with degree distribution p(k) and maximal degree n.

Section snippets

Stability of the disease-free equilibrium

The stability of the disease-free equilibrium determines an outbreak of the disease or not. In this section, we introduce a concise method to address such mentioned issues and such method averts some tedious calculations as in Lemma 3 and Theorem 1 in [1]. System (3) always has a disease-free equilibrium E0=(1,0).

Theorem 2.1

If R0<1, then the disease-free equilibrium E0 is locally asymptotically stable; Otherwise, if R0>1, it is unstable.

Proof

Linearizing model (3) at the disease-free equilibrium E0 yields to dSk

Existence and stability of feasible endemic equilibria

In this section, we try to look for the existence of each feasible equilibrium and set up a general result for their stability. The components of each feasible endemic equilibria E=(Sk,Θ) satisfy the following equations 0=μβkSkΘμSk,0=βkk=1nk2p(k)Skr1+αΘ(μ+γ),k=1,2,,n.The first equation suggests that Sk=μμ+βkΘ,k=1,2,,n.Replacing Sk in the (n+1)th equation of Eq. (7) by (8), one gets a self-compatible equation F(Θ)r1+αΘ+μ+γβkk=1nk2p(k)μμ+βkΘ=0.It is easy to see that F(0

Conclusion

The saturation treatment has been identified an important factor in resulting in the occurrence of the backward bifurcation. Generally, once it happens, the equilibrium with lower value is unstable and the other one with larger value is stable, i.e., a bistable phenomena appears accordingly (See Fig. 1(b)). Indeed, such phenomena have been extensively studied by many scholars, but most of them were confined to concern the homogeneously mixed models [7], [8], [9], [10]. As we know, there are few

Acknowledgments

This work was partially supported by the National Natural Science Foundation of China (Nos. 61573016, 11771017), the Shanxi Province Science Foundation for Youths, China (No. 201901D211413) and Shanxi Scholarship Council of China (No. 2015-094).

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