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Research article

Dynamic analysis of a stochastic vector-borne model with direct transmission and media coverage

  • Received: 05 December 2023 Revised: 04 February 2024 Accepted: 07 February 2024 Published: 06 March 2024
  • MSC : 60G51, 60G57, 92B05

  • This paper presents a stochastic vector-borne epidemic model with direct transmission and media coverage. It proves the existence and uniqueness of positive solutions through the construction of a suitable Lyapunov function. Immediately after that, we study the transmission mechanism of vector-borne diseases and give threshold conditions for disease extinction and persistence; in addition we show that the model has a stationary distribution that is determined by a threshold value, i.e., the existence of a stationary distribution is unique under specific conditions. Finally, a stochastic model that describes the dynamics of vector-borne diseases has been numerically simulated to illustrate our mathematical findings.

    Citation: Yue Wu, Shenglong Chen, Ge Zhang, Zhiming Li. Dynamic analysis of a stochastic vector-borne model with direct transmission and media coverage[J]. AIMS Mathematics, 2024, 9(4): 9128-9151. doi: 10.3934/math.2024444

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  • This paper presents a stochastic vector-borne epidemic model with direct transmission and media coverage. It proves the existence and uniqueness of positive solutions through the construction of a suitable Lyapunov function. Immediately after that, we study the transmission mechanism of vector-borne diseases and give threshold conditions for disease extinction and persistence; in addition we show that the model has a stationary distribution that is determined by a threshold value, i.e., the existence of a stationary distribution is unique under specific conditions. Finally, a stochastic model that describes the dynamics of vector-borne diseases has been numerically simulated to illustrate our mathematical findings.



    Vector-borne disease seriously threatens global health, and it is usually caused by vector-borne parasites, viruses, and bacteria that transmits pathogens between humans or from animals to humans. According to the World Health Organization, the disease accounts for 17% of all infectious and has caused 700,000 deaths annually [1]. Despite scientific and technological advances and the growing influence in all regions, vector-borne diseases remain one of the leading causes of global disease. Mathematical modeling has become an essential method for studying epidemics. Since the first attempt to model malaria transmission by Ross [2] and subsequent modifications by MacDonald [3], a series of vector-borne disease models have been proposed [4,5,6,7]. Various disease models based on influencing factors (e.g., time delay, vaccination, age structure, etc.) have been extensively studied [8,9,10,11].

    It is commonly known that direct and indirect transmissions are two significant ways that various diseases are spread. Although vector-borne diseases are mainly transmitted by vectors, i.e., indirect transmission, vector-borne diseases are often transmitted directly through blood transfusions, organ transplantation, laboratory exposure, or mother-to-baby during pregnancy, childbirth, or breastfeeding. Furthermore Zika can be transmitted through sexual contact[12]. Thus, direct transmission plays a vital role in the dynamics of vector-borne diseases and has attracted widespread attention [13,14,15,16]. In the deterministic model proposed by Wei et al. [16], the host population is assumed to be divided into three subpopulations, i.e., susceptible, infected, and recovered individuals. The infected individuals will not relapse once recovered, i.e., the recovered individuals will not become susceptible or infected. Let S(t),I(t), and R(t) be the numbers of susceptible, infected, and recovered individuals at time t. The vector population is divided into two parts, i.e., susceptible and infected vectors, denoted by M(t) and V(t) as the corresponding numbers at time t. The newly recruited vectors are susceptible when vertical transmission is ignored. On the other hand, media coverage is a crucial factor in the control of the spread of epidemics [17]. The media helps people to understand the progress of an epidemic and provide beneficial guidance [18]. Many scholars have studied the impact of media coverage on disease transmission from the perspective of mathematical modeling [19,20].

    Based on the above discussion, we introduce media coverage into the epidemic model and investigate the dynamics of vector-borne diseases with direct transmission. Let β1 be the transmission rate without media intervention, and β2I/(m+I) be the effect of media coverage on transmission, where β1>β2 and m measures how quickly people react to media reports [21]. During the spread of the vector-borne epidemic, two transmission rates can lead to the susceptible becoming infected : the rate denoted by β3 from an infected vector to a susceptible person, and the one denoted by β4 from an infected person to a susceptible vector. We propose a vector-borne model with direct transmission and media coverage as follows

    {dS=(Λ1(β1β2Im+I)SI1+α1Iβ3SV1+α2Vd1S)dt,dI=((β1β2Im+I)SI1+α1I+β3SV1+α2V(μ+d1+γ)I)dt,dR=(γId1R)dt,dM=(Λ2β4MI1+α3Id2M)dt,dV=(β4MI1+α3Id2V)dt, (1.1)

    where Λi is a recruitment rate, di(i=1,2), and μ are the natural, and disease-related death rates of people and vector population, αi(i=1,2,3) denotes the saturated constants during different transmission processes, and γ is the recovery rate of infected people. Here, β1SI, β3SV, and β4MI measure the contagiousness of the vector-borne disease, and 1/(1+α1I), 1/(1+α2V), and 1/(1+α3I) reflect the behavioral change of susceptible individuals. The basic reproduction number is R0=β1Λ1d1(d1+γ+μ)+β3β4Λ1Λ2d1d22(d1+γ+μ), which determines whether the epidemic occurs. If R0<1, system (1.1) has a unique disease-free equilibrium E0=(Λ1d1,0,0,Λ2d2,0). This represents no infected individuals in either population. If R0>1, then model (1.1) has two equilibria: a disease-free equilibrium E0 and an endemic equilibrium E=(S,I,R,M,V). This means that some individuals of both populations have been infected.

    In the real world, random fluctuations are essential to ecosystems [22,23,24]. Random factors, such as temperature and humidity, inevitably affect the epidemic's spread. Many stochastic models have been studied in recent years [25,26,27]. Considering the complex environmental changes, Liu and Jiang claimed that the random perturbation may depend on the square of the state variables S and I in the system [28,29]. Recently, nonlinear perturbations have received much attention [30,31,32]. In addition to this, sometimes ecosystems are also affected by violent random perturbations such as typhoons and tsunamis. To reflect reality better, Levy jumps were introduced into the model [33,34]. However, this noise differs in detail and often leads to different results. It is worth noting that in the model of vector-borne diseases, Jovanović and Krstić [35] proposed that the random perturbation is proportional to the distance. Ran et al. [36] studied the dynamics of a stochastic vector-borne model with age structure and saturation incidence, considering the environmental noise on the mosquito bite rate and transmission rate between vector and host. Son and Denu [37] provided another stochastic vector-borne model with direct transmission, in which environmental noise affects the mortality of hosts and vectors. We did not want to add complex perturbations to make the model unmanageable; simple perturbations are more likely to reveal the inherent nature of the model. In our work, suppose that the environmental white noise is proportional to the number of subpopulations [38,39]. Next, we extend the deterministic model (1.1) to a stochastic model. The recovered class is decoupled from the others in the model and then neglected. Then, we propose the following stochastic model

    {dS=(Λ1(β1β2Im+I)SI1+α1Iβ3SV1+α2Vd1S)dt+σ1SdB1(t),dI=((β1β2Im+I)SI1+α1I+β3SV1+α2V(μ+d1+γ)I)dt+σ2IdB2(t),dM=(Λ2β4MI1+α3Id2M)dt+σ3MdB3(t),dV=(β4MI1+α3Id2V)dt+σ4VdB4(t), (1.2)

    where Bi(t)(i=1,2,3,4) denotes independent standard Brownian motions, σi(i=1,2,3,4) represents the white noise intensity, and the remaining parameters are the same as in model (1.1).

    The rest of this paper is organized as follows. Section 2 reviews some basic concepts and valuable lemmas used later. The uniqueness and positivity of the solution are proved in Section 3. Section 4 provides sufficient conditions for determining whether a disease is extinct. In Section 5, we explore the persistence in the mean. In Section 6, we prove the existence of a unique ergodic stationary distribution under certain conditions. In Section 7, we validate the results of analysis through numerical simulations. A brief conclusion is given in the last section.

    Let (Ω,F,P) be a complete probability space with a filtration {Ft}t0 that satisfies the usual conditions (i.e., it is increasing and right continuous while F0 contains all P-null sets). Denote Rn+={yRn:yi>0,1in}. Consider an n-dimensional stochastic differential equation of the following form [40]

    dy(t)=f(y(t),t)dt+g(y(t),t)dB(t) (2.1)

    with the initial value y(0)=y0Rn, where B(t) denotes an n-dimensional standard Brownian motion defined on the complete probability space (Ω,F,{Ft}t0,P). Define a differential operator L of Eq (2.1) as follows

    L=t+ni=1fi(y,t)yi+12ni,j=1[gT(y,t)g(y,t)]ij2yiyj.

    If L acts on a nonnegative function VC2,1(Rn×[t0,];R+), then

    LV(y,t)=Vt(y,t)+Vy(y,t)f(y,t)+12trace[gT(y,t)Vyy(y,t)g(y,t)],

    where Vt=Vt,Vy=(Vy1,,Vyn),Vyy=(2Vyiyj)n×n. By Itô's formula, it follows that

    dV(y(t),t)=LV(y(t),t)dt+Vy(y(t),t)g(y(t),t)dB(t),y(t)Rn.

    Lemma 1. (Strong law of large numbers, [41]) Let M={Mt}t0 be a real- valued continuous local martingale vanishing at t=0. Then

    limtM,Mt=a.s.limtMtM,Mt=0.a.s.lim suptM,Mtt<a.s.limtMtt=0. a.s.

    Let Y(t) be a regular time-homogeneous Markov process in Rn in the following form

    dY(t)=a(Y)dt+ki=1σidBi(t),

    where the diffusion matrix ˉA(Y)=(bij(y)) and bij(y)=kr=1σir(y)σjr(y).

    Lemma 2. [42] The Markov process Y(t) has a unique stationary distribution π() if there is a bounded domain DRn with a regular boundary and the following holds

    (i) There is a positive number M such that ni,j=1bij(y)ξiξjM|ξ|2,yD,ξRn.

    (ii) There exists a nonnegative C2 -function V such that LV is negative for any RnD; then

    P{lim supT1TT0f(Y(t))dt=Rnf(y)π(dy)}=1.

    Theorem 1. For a given initial value Y(0)=(S(0),I(0),M(0),V(0))R4+, the solution Y(t)=(S(t),I(t),M(t),V(t)) of model (1.2) is unique on t0 and will maintain in R4+ with probability one.

    Proof. For a given initial value (S(0),I(0),M(0),V(0))R4+, the coefficient in the model (1.2) satisfies the local Lipschitz continuity condition. Hence, there is a unique local solution when t[0,τe), where τe is the explosion time [43,44]. To obtain the global property of the solution, we need to prove that τe= almost surely (a.s.). Suppose that k01 is sufficiently large such that S(0),I(0),M(0) and V(0) all lie within the interval [1/k0,k0]. For each integer kk0, define a stopping time

    τk=inf{t[0,τe):min{S(t),I(t),M(t),V(t)}1/k  or  max{S(t),I(t),M(t),V(t)}k}, (3.1)

    where is an empty set and inf=. It can be seen that τk increases as k and τ=limkτk with 0ττe a.s. In other words, if τe= a.s. does not hold, there must exists constants T,k1>0 and ϵ(0,1) such that P{τkT}>ϵ for all kk1. Define a C2-function W:R4R+ and

    W(S(t),I(t),M(t),V(t))=(S(t)1logS(t))+(I(t)1logI(t))+(M(t)1logM(t))+(V(t)1logV(t)). (3.2)

    Obviously, W is a non-negative function. Applying Itô's formula to Eq (3.2) yields

    dW(S(t),I(t),M(t),V(t))=[(11S)(Λ1(β1β2Im+I)SI1+α1Iβ3SV1+α2Vd1S)+12σ21+(11I)((β1β2Im+I)SI1+α1I+β3SV1+α2V(μ+d1+γ)I)+12σ22+(11M)(Λ2β4MI1+α3Id2M)+12σ23+(11V)(β4MI1+α3Id2V)+12σ24]dt+σ1(S1)dB1(t)+σ2(I1)dB2(t)+σ3(M1)dB3(t)+σ3(V1)dB4(t)=LWdt+σ1(S1)dB1(t)+σ2(I1)dB2(t)+σ3(M1)dB3(t)+σ4(V1)dB4(t),

    where LW:R4+R+ can be written in the following form

    LW(S(t),I(t),M(t),V(t))=[(11S)(Λ1(β1β2Im+I)SI1+α1Iβ3SV1+α2Vd1S)+12σ21+(11I)((β1β2Im+I)SI1+α1I+β3SV1+α2V+(μ+d1+γ)I)+12σ22+(11M)(Λ2β4MI1+α3Id2M)+12σ23+(11V)(β4MI1+α3Id2V)+12σ24]Λ1+Λ2+2d1+2d2+β1α1+β3α2+β4α3+μ+γ+β1I1+α1I+β3V1+α2Vβ1S1+α1Iβ3SV(1+α2V)I+β4I1+α3Iβ4MI(1+α3I)V+12σ21+12σ22+12σ23+12σ24Λ1+Λ2+2d1+2d2+β1α1+β3α2+β4α3+μ+γ+12σ21+12σ22+12σ23+12σ24=:κ.

    Hence, we have

    dW(S(t),I(t),M(t),V(t))κdt+σ1(S1)dB1(t)+σ2(I1)dB2(t)+σ3(M1)dB3(t)+σ4(V1)dB4(t). (3.3)

    Integrate both sides of Eq (3.3) from 0 to τkT. It is easy to get that

    τkT0dW(S(u),I(u),M(u),V(u))τkT0κdu+τkT0{σ1(S1)dB1+σ2(I1)dB2+σ3(M1)dB3+σ4(V1)dB4}. (3.4)

    Setting Ω={τkT} for kk1 and by using Eq (3.1), we get that P(Ωk)ϵ. Further, every ω from Ω is associated with at least one among S(τk,ω),I(τk,ω),M(τk,ω), and V(τk,ω) that is equal to k or 1/k. Hence, W(S(τk),I(τk),M(τk),V(τk)) is not less than k1logk or 1k1+logk. That is to say,

    W(S(τk),I(τk),M(τk),V(τk))(k1logk)(1k1log1k). (3.5)

    Combining Eqs (3.4) and (3.5), we have

    W(S(0),I(0),M(0),V(0))+κ(τkT)E[1Ω(ω)W(S(τk),I(τk),M(τk),V(τk))]ϵ(k1logk)(1k1log1k),

    where 1Ω(ω) denotes an indicator function of set Ω. Letting k leads to the following contradiction

    W(S(0),I(0),M(0),V(0))+κ(τkT)=.

    It implies that τe= a.s. The proof is complete.

    It is clear that model (1.1) has a disease-free equilibrium E0=(Λ1/d10,Λ2/d2,0) whereby the disease tends to become extinct within the time limit. However, there is no disease-free equilibrium in the stochastic version of the model, which requires other ways to consider its extinction. Define a threshold value

    RS0=1μ1+σ2/2(βΛ1d1+β4Λ2d2),σ=min{σ2,σ4}.

    Theorem 2. Assume that d1>σ21σ222 and d2>σ31σ422. Let (S(t),I(t),M(t),V(t)) be the solution of system (1.2) with any initial value (S(0),I(0),M(0),V(0)). If RS0<1, then

    lim suptlog(I+V)t(μ1+σ22)(RS01)<0,a.s..

    Moreover,

    limt1tt0S(u)du=Λ1d1,limt1tt0I(u)du=0a.s.,limt1tt0M(u)du=Λ2d2,limt1tt0V(u)du=0a.s..

    Proof. According to Reference [45], we have

    limtS(t)t=limtI(t)t=limtM(t)t=limtV(t)t=0,  a.s.,  (4.1)
    limtt0S(u)dB1(u)t=limtt0I(u)dB2(u)t=limtt0M(u)dB3(u)t=limtt0V(u)dB4(u)t=0  a.s.. (4.2)

    We integrate both sides of the proposed model (1.2) and obtain

    S(t)S(0)t+I(t)I(0)t=Λ1d1tt0S(u)duμ+d1+γtt0I(u)du+σ1tt0S(u)dB1(u)+σ2tt0I(u)dB2(u).

    It is obvious that

    1tt0S(u)du=Λ1d1(d1+μ+γ)d1tt0I(u)du+σ1d1tt0S(u)dB1(t)+σ2d1tt0I(u)dB2(t)S(t)S(0)d1tI(t)I(0)d1t. (4.3)

    From Eqs (4.1) and (4.2), the limit of Eq (4.3) given by

    limt1tt0S(u)du=Λ1d1limt(d1+μ+γd1tt0I(u)du). (4.4)

    Similarly, we integrate on both sides of the last two equations of the model (1.2). Hence,

    M(t)M(0)t+V(t)V(0)t=Λ2d2t(t0M(u)du+t0V(u)du)+σ3tt0M(u)dB3(u)+σ4tt0V(u)dB4(u).

    Combining (4.1) and (4.2), we can get the following equation

    limt1tt0V(u)du=Λ2d2limt1tt0M(u)du. (4.5)

    On the other hand, by Itô's formula, it follows that

    dlog(I+V)=β4MI(1+α1I)(I+V)dt+β3SV(1+α2V)(I+V)dt+(β1β2Im+I)SI(1+α1I)(I+V)dtσ22I2(I+V)2dtσ24V2(I+V)2dt+σ2II+VdB2(t)+σ4VI+VdB4(t)(μ+d1+γ)II+Vdtd2VI+Vdt.β4MI(I+V)dt+βS(I+V)(I+V)dt+σ22II+VdB2(t)+σ42VI+VdB4(t)μ1I+VI+Vdtσ2(I+V)22(I+V)2dt.

    The last term here uses the inequality 2IV(I+V)2. Integrate on both sides of the equation and divide it by t. Thus,

    1tlog(I+V)βtt0S(u)du+β4tt0M(u)du+1tt0σ2II+VdB2(u)+1tt0σ4II+VdB4(u)1tt0σ22dt1tt0μ1du,

    where μ1=min{μ+d1+γ,d2},σ=min{σ2,σ4}, and β=max{β1,β3}. From Eqs (4.4) and (4.5), we can get

    1tlog(I+V)β1(Λ1d1(d1+μ)d1tt0I(u)du)+β4(Λ2d21tt0V(u)du)+1tt0σ2II+VdB2(u)+1tt0σ4II+VdB4(u)1tt0σ22dt1tt0μ1du. (4.6)

    According to Lemma 1, it is obtained that

    limt(1tt0σ4VI+VdB4(u)+1tt0σ2II+VdB2(u))=0,a.s.. (4.7)

    By using Eqs (4.6) and (4.7), we have

    lim suptlog(I+V)t(μ1+σ22)(RS01)<0,a.s..

    It means that limt1tt0I(u)du=0 and limt1tt0V(u)du=0,a.s. Combining Eqs (4.4) and (4.5), it is obvious that

    limt1tt0S(u)du=Λ1d1,limt1tt0M(u)du=Λ2d2,  a.s..

    The proof is complete.

    The most interesting aspect in the study of epidemic modeling is the extinction and persistence of the epidemic; in the previous section we studied disease extinction and in this section we will show that diseases are persistent in the mean.

    Theorem 3. Assume that d1>σ21σ222 and d2>σ31σ422. If

    RS1=99Λ21Λ2d21d2(β1β2)β3β4+12(σ21+σ22+σ23+σ24)4d1+3d2+μ+γ>1,

    then for any given initial value (S(0),I(0),M(0),V(0))R4+, the solution of system (1.2) has the following properties

    (i)limt1tt0S(u)duΛ1d1+β1/α1+β2/α2,a.s..(ii)limt1tt0M(u)duΛ2d2+β4/α3,a.s..(iii)limt1tt0I(u)du+limt1tt0V(u)du4d1+3d2+μ+γ(β1+β4+d1α3+d1α1)(β3+d2α2)(RS11),a.s..

    Proof. (i) From the first equation of system (1.2) integrating the above inequality and dividing both sides by t, we get

    S(t)S(0)t=Λ11tt0(β1β2I(t)I(t)+m)S(u)I(u)1+α1I(u)du1tt0β3S(u)V(u)1+α2V(u)du1tt0d1S(u)duσ1tt0S(u)dB1(u).

    In view of Theorem 1, for any initial value (S(0),I(0),M(0),V(0))R4+, there is a unique global solution (S(t),I(t),M(t),V(t))R4+. Thus,

    S(t)S(0)t+σ1tt0S(u)dB1(u)Λ11tt0β1S(u)α1du1tt0β3S(u)α2du1tt0d1S(u)du. (5.1)

    Through the strong law of large numbers for local martingales, we have

    limt(S(t)S(0)t+σ1tt0S(u)dB1(u))=0a.s., 

    which together with Eq (5.1) yields

    limt1tt0S(u)duΛ1d1+β1/α1+β2/α2a.s.. 

    This is the required assertion (i).

    (ii) From the third equation of system (1.2), integrating the above inequality and dividing both sides by t, we get

    M(t)M(0)t=Λ21tt0β4M(u)I(u)1+α3I(u)du1tt0d2M(u)duσ3tt0M(u)dB3(u).

    Then

    M(t)M(0)t+σ3tt0M(u)dB3(u)Λ21tt0β4M(u)α3du1tt0d2M(u)du. (5.2)

    According to the strong law of large numbers of local martingales, we have

    limt(M(t)M(0)t+σ3tt0M(u)dB3(u))=0a.s.,

    which together with Eq (5.2) yields

    limt1tt0M(u)duΛ2d2+β4/α3a.s..

    This is the required assertion (ii).

    (iii) First, define a function W2(S,I,V)=lnSlnIlnMlnV. According to the Itô's formula:

    dW2(t)=LW2(t)dtσ1dB1(t)σ2dB2(t)σ3dB3(t)σ4dB4(t),

    where

    LW2(t)=1S(Λ1(β1β2Im+I)SI1+α1Iβ3SV1+α2Vd1S)1I((β1β2Im+I)SI1+α1I+β3SV1+α2V(μ+d1+γ)I)1M(Λ2β4MI1+α3Id2M)1V(β4MI1+α3Id2V)12(σ21+σ22+σ23+σ24)=Λ1S+β1I1+α1I(β2Im+I)I1+α1I+β3V1+α2V+d1β3SVI(1+α2V)(β1β2Im+I)S1+α1I+(d1+μ+γ)Λ2M+β4I(1+α3I)β4MIV(1+α3I)+2d2d2(1+α2V)d1(1+α3I)d1(1+α1I)+d2(1+α2V)+d1(1+α3I)+d1(1+α1I)12(σ21+σ22+σ23+σ24)(β1+β4+d1α3+d1α1)I+(β3+d2α2)VΛ12SΛ2Mβ4MIV(1+α3I)β3SVI(1+α2V)(β1β2)S1+α1IΛ12Sd2(1+α2V)d1(1+α3I)d1(1+α1I)+(4d1+3d2+μ+γ)12(σ21+σ22+σ23+σ24)(β1+β4+d1α3+d1α1)I+(β3+d2α2)V99Λ21Λ2d21d2(β1β2)β3β4+(4d1+3d2+μ+γ)12(σ21+σ22+σ23+σ24).

    We integrate the above inequality in the interval (0,t), divide it by t, and take the limit to t. Thus,

    099Λ21Λ2d21d2(β1β2)β3β4+(4d1+3d2+μ+γ)12(σ21+σ22+σ23+σ24)+limt(β1+β4+d1α3+d1α1)tt0I(u)du+limt(β3+d2α2)tt0V(u)dulimt1tt0σ1dB1(u)limt1tt0σ2dB2(u)limt1tt0σ3dB3(u)limt1tt0σ4dB4(u). (5.3)

    According to the law of large numbers for a martingale,

    limt1tt0σ1dB1(u)=limt1tt0σ2dB2(u)=limt1tt0σ3dB3(u)=limt1tt0σ4dB4(u)=0.

    It follows that Eq (5.3) becomes

    limt(β1+β4+d1α3+d1α1)tt0I(u)du+limt(β3+d2α2)tt0V(u)du99Λ21Λ2d21d2(β1β2)β3β4(4d1+3d2+μ+γ)+12(σ21+σ22+σ23+σ24)a.s.

    The proof is complete.

    The ergodic property for an epidemic model means that the stochastic model has a unique stationary distribution that forecasts the permanence of the epidemic in the future. That means the disease persists for all time regardless of the initial condition[46].

    In this section, we provide a sufficient condition for the existence of a stationary distribution in the model (1.2). Denote

    RS2=min{RS3,RS4},RS3=7r17(β1β2)β3β4Λ21Λ24,RS4=8r28(β1β2)β3β4Λ21Λ24,

    where r1=124i=1σ2i+2d1+3d2+μ+γ+β1α1+β3α2+β4α3, and r2=124i=1σ2i+4d1+2d2+μ+γ+β1α1+β3α2+β4α3.

    Theorem 4. If RS2>1, then model (1.2) has a unique stationary distribution π() with ergodicity.

    Proof. The diffusion matrix for model (1.2) is given by

    ˉA=(σ21S20000σ22I20000σ23M20000σ24V2).

    Denote M=min(S,I,M,V)DR4+{σ21S2,σ22I2,σ23M2,σ24V2}. It follows that

    4i,j=1bij(S,I,M,V)ξiξj=σ21S2ξ21+σ22E2ξ22+σ23I2ξ23+σ24R2ξ24M|ξ|2

    for (S,I,M,V)D,ξ=(ξ1,ξ2,ξ3,ξ4)R4, where D=(1k,k)×(1k,k)×(1k,k)×(1k,k) and k is a sufficiently large integer. Therefore, the condition (i) in Lemma 2 is satisfied. Next, we prove the condition (ii) in Lemma 2. Let

    V1=logSlogMlogVlogI+α2d2V,V2=logSlogMlogV+(α1+α3)(S+I),V3=logSlogM,V4=1θ+2(S+I+M+V)θ+2.

    Denote λi=ri(Ri1)(i=1,2), σ2=σ21σ22σ23σ24, b=2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232 and d=d1d2. We construct a C2-function ˜V:R4+R as follows

    ˜V(S,I,M,V)=Θ1V1+Θ2V2+V3+V4,

    where Θi(i=1,2) denotes sufficiently large positive constants satisfying Θ1λ1+F23, Θ2λ2+F32, and

    F2=sup(S,I,M,V)R4+{12(α2d2β4)2M212(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+b+B},F3=sup(S,I,M,V)R4+{Θ1α2d2β4MI12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+b+B},B=sup(S,I,M,V)R4+{(Λ1+Λ2)(S+I+M+V)θ+112(d(θ+1)σ22)(S+I+M+V)θ+2}<,

    Here, θ is a positive constant satisfying that d>(θ+1)σ2/2. It means that

    lim infk,(S,I,M,V)R4+D˜V(S,I,M,V)=,

    and ˜V(S,I,M,V) is a continuous function. Then the function ˜V(S,I,M,V) must have a minimum point (ˉS,ˉI,ˉM,ˉV)R4+. Further, we construct a nonnegative C2-function V:R4+R+ in the following form

    V(S,I,M,V)=Θ1V1+Θ2V2+V3+V4˜V(ˉS,ˉI,ˉM,ˉV).

    Applying Itô's formula to V1, we get

    LV1=1S[Λ1d1S(β1β2II+m)SI1+α1Iβ3SV1+α2V]+σ2121I[(d1+μ+γ)I+(β1β2II+m)SI1+α1I+β3SV1+α2V]+σ2221M[Λ1β4MI1+α3Id2M]+σ2321V[β4MI1+α3Id2V]+σ242α2d2β4MI(1+α3I)d2α2VΛ12SΛ2M(β1β2)S1+α1IΛ12Sβ3SV(1+α2V)I+β4MI(1+α3I)V+d2(1+α2V)
    +σ212+σ222+σ232+σ242+2d1+3d2+(μ+γ)+β1α1+β3α2+β4α3+α2d2β4MI77(β1β2)β3β4Λ21Λ24(1+α1I)(1+α3I)+σ212+σ222+σ232+σ242+2d1+3d2+(μ+γ)+β1α1+β3α2+β4α3+α2d2β4MI,LV2=1S[Λ1d1S(β1β2II+m)SI1+α1Iβ3SV1+α2V]+σ2121I[(d1+μ+γ)I+(β1β2II+m)SI1+α1I+β3SV1+α2V]+σ2221M[Λ1β4MI1+α3Id2M]+σ2421V[β4MI1+α3Id2V]+σ242d1(α1+α3)Id1(α1+α3)S(μ+γ)(α1+α3)IΛ12SΛ2M(β1β2)S1+α1IΛ12Sβ3SV(1+α2V)Iβ4MI(1+α3I)Vd1(1+α1I)d1(1+α3I)+σ212+σ222+σ232+σ242+4d1+2d2+(μ+γ)+β1α1+β3α2+β4α388(β1β2)β3β4Λ21Λ24(1+α3V)+σ212+σ222+σ232+σ242+4d1+2d2+(μ+γ)+β1α1+β3α2+β4α3,
    LV3=1S[Λ1d1S(β1β2II+m)SI1+α1Iβ3SV1+α2V]+σ2121M[Λ2β4MI1+α3Id2M]+σ232Λ1SΛ2M+2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232,LV4=(S+I+M+V)θ+1[Λ1d1(S+I+R)(μ+γ)I+Λ2d2(M+V)]+(θ+1)(S+I+M+V)θ[σ212S2+σ232I2+σ232M2+σ242V2](S+I+M+V)θ+1(Λ1+Λ2)(S+I+R+M+V)θ+2(d1d2)+12(θ+1)(S+I+M+V)θσ2(S+I+M+V)2(S+I+M+V)θ+1(Λ1+Λ2)(d(θ+1)σ22)(S+I+M+V)θ+2B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2),

    where

    B=sup(S,I,M,V)R4+{(Λ1+Λ2)(S+I+M+V)θ+112(d(θ+1)σ22)(S+I+M+V)θ+2}<.

    Thus, it follows that

    LVΘ1r1(RS31)Θ2r2(RS41)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+Θ1(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)Λ1SΛ2M.

    A closed subset is defined as follows:

    D={(S,I,M,V)R4+:ϵS1ϵ,ϵI1ϵ,ϵM1ϵ,ϵV1ϵ},

    where ϵ>0 represents sufficiently small constants satisfying the following conditions

    Λ1ϵ+F3<1, (6.1)
    Θ1r3(77(β1β2)β3β4Λ21Λ24(1+αϵ)(1+αϵ)1)+F2+Θ21ϵ22<1, (6.2)
    H+Θ1(α2d2β4)1ϵ212(d(θ+1)σ22)(1ϵ)θ+2<1, (6.3)
    Λ2ϵ+F2<1, (6.4)
    Θ2r2(88(β1β2)β3β4Λ21Λ24(1+α3ϵ)1)+F3<1, (6.5)
    H+Θ1(α2d2β4)1ϵ212(d(θ+1)σ22)(1ϵ)θ+2<1, (6.6)

    where H is a constant and is determined later. Denote Y=(S,I,M,V). We divide R4+D into the following eight cases

    D1={YR4+,0<S<ϵ},D2={YR4+,0<I<ϵ},D3={YR4+,S>1ϵ,ϵ<M<1ϵ,ϵ<I<1ϵ},D4={YR4+,I>1ϵ,ϵ<M<1ϵ},D5={YR4+,0<M<ϵ},D6={YR4+,0<V<ϵ4,},D7={YR4+,1ϵ<M,ϵ<I<1ϵ},D8={YR4+,1ϵ<V,ϵ<M<1ϵ,ϵ<I<1ϵ}.

    Now, we will prove that LV(S,I,M,V)<1 on R4+D; this is equivalent to proving that it is valid on the above eight subsets.

    Case 1. When (S,I,M,V)D1, we can get

    LV2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)Λ1SΛ1S+F3Λ1ϵ+F3,

    where

    F3=sup(S,I,M,V)R4+{Θ1α2d2β4MI12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+a+B}.

    According to Eq (6.1), we have that LV(S,I,M,V)<1 for any (S,I,M,V)D1.

    Case 2. When (S,I,M,V)D2, we have

    LVΘ1r3(77(β1β2)β3β4Λ21Λ24(1+α1I)(1+α3I)1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+(α2d2β4)2M22+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+Θ21I22Θ1r3(77(β1β2)β3β4Λ21Λ24(1+α1ϵ)(1+α3ϵ)1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+(α2d2β4)2M22+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+Θ21ϵ22Θ1r3(77(β1β2)β3β4Λ21Λ24(1+α1ϵ)(1+α3ϵ)1)+F2+Θ21ϵ22,

    where

    F2=sup(S,I,M,V)R4+{12(α2d2β4)2M212(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+a+B}.

    Given Eq (6.2), we get that LV(S,I,M,V)<1 for any (S,I,M,V)D2.

    Case 3. When (S,I,M,V)D3, we have that

    LVd1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)H+Θ1(α2d2β4)1ϵ212(d(θ+1)σ22)(1ϵ)θ+2H+Θ1(α2d2β4)1ϵ212(d(θ+1)σ22)(1ϵ)θ+2,

    where H=d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+B, and, from Eq (6.3), we have that LV(S,I,M,V)<1 for any (S,I,M,V)D3.

    Case 4. When (S,I,M,V)D4, then

    LV2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)H+Θ1(α2d2β4)1ϵ212(d(θ+1)σ22)(1ϵ)θ+2=H+Θ1(α2d2β4)(1ϵ)212(d(θ+1)σ22)(1ϵ)θ+2.

    Again, from Eq (6.3), we find that LV(S,I,M,V)<1 for any (S,I,M,V)D4.

    Case 5. When (S,I,M,V)D5, we have

    LV2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)Λ2MΛ2M+F3Λ1ϵ+F3.

    By means of Eq (6.4) we obtain that LV(S,I,M,V)<1 for any (S,I,M,V)D5.

    Case 6. When (S,I,M,V)D6, we can get

    LVΘ2r2(88(β1β2)β3β4Λ21Λ24(1+α3V)1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+Θ(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)Θ2r2(88(β1β2)β3β4Λ21Λ24(1+αϵ)1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+Θ(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)Θ2r2(88(β1β2)β3β4Λ21Λ24(1+αϵ)1)+F3.

    By Eq (6.5), we have that LV(S,I,M,V)<1 for any (S,I,M,V)D6.

    Case 7. When (S,I,M,V)D7, it follows that

    LV2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)1ϵ2+B12(d(θ+1)σ22)(1ϵ)θ+2H+Θ1(α2d2β4)1ϵ212(d(θ+1)σ22)(1ϵ)θ+2,

    Using Eq (6.6), we have that LV(S,I,M,V)<1 for any (S,I,M,V)D7.

    Case 8. When (S,I,M,V)D8, then

    LV2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B12(d(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)1ϵ2+B12(d(θ+1)σ22)(1ϵ)θ+2H+Θ1(α2d2β4)1ϵ212(d(θ+1)σ22)(1ϵ)θ+2.

    Again using Eq (6.6), we have that LV(S,I,M,V)<1 for any (S,I,M,V)D8.

    In Cases 1–8, we have chosen sufficiently small values of ϵ such that LV(S,I,M,V)<1 for any (S,I,M,V)Di(i=1,2,,8). Thus, LV(S,I,M,V)<1 for all (S, I, M, V) R4+D. Then, the condition (ii) in Lemma 2 is satisfied. According to Lemma 2, we can obtain that system (1.2) is ergodic and has a unique stationary distribution. This completes the proof.

    Numerical simulations are presented to support our theoretical findings of the model (1.2) and reveal the impact of media coverage on the spread of disease. Using the Milstein method mentioned by Higham [47], we consider the discretized equations as follows:

    Si+1=Si+(Λ1d1Si(β1β2Iim+Ii)SiIi1+α1Iiβ3SiVi1+α2Vi)Δt+Si(σ1Δtζ1i+σ12Si(ζ21i1)Δt),Ii+1=Ii+((β1β2Iim+Ii)SiIi1+α1Ii+β3SiVi1+α2Vi(d1+μ+γ)Ii)Δt+Ii(σ2Δtζ2i+σ222Ii(ζ22i1)Δt),Mi+1=Mi+(Λ2β4MiIi1+α3Iid2Mi)Δt+Mi(σ3Δtζ3i+σ232Mi(ζ23i1)Δt),Vi+1=Vi+(β4MiIi1+α3Iid2Vi)Δt+Vi(σ4Δtζ4i+σ242Vi(ζ24i1)Δt),

    where the time increment Δt>0 and ζ1i,ζ2i,ζ3i,ζ4i, are mutually independent Gaussian random variables which follow the distribution N(0,1) for i=0,1,2,...,n.

    Vector-borne diseases with two transmission routes may be more likely to become endemic than diseases with one transmission route. Therefore, we tend to choose lower transmission rates and recruitment when numerically modeling disease extinction.

    Example 1. Let Λ1=100, Λ2=100, β1=0.000012, β2=0.0000018, β3=0.000039, β4=0.000039, α1=0.13, α2=0.15, α3=0.15, μ=0.13, γ=0.13, d1=0.1, d2=0.1, m=20, σ1=0.025, σ2=0.25, σ3=0.03, σ4=0.26, μ1=min{μ+d1+γ,d2}, σ=min{σ2, σ4}, β=max{β1,β3}, and the initial values (S(0), I(0), M(0), V(0)) = (1000, 15, 1000, 50). So

    RS0=1μ1+σ2/2(βΛ1d1+β4Λ2d2)0.594<1.

    According to Theorem 2, the solution of the stochastic model (1.2) will eventually approach zero; this means that the disease will die out almost surely. And, from Figure 1, it is observed that the number of infected individuals tends to zero.

    Figure 1.  The disease became extinct in both groups at initial values (S(0), I(0), M(0), V(0)) = (1000, 15, 10000, 50).

    Example 2. We keep the parameters the same as in Example 1, except that Λ1=Λ2=500, β1=0.01 and β3=β4=0.001. Then

    RS1=99Λ21Λ2d21d2(β1β2)β3β4+12(σ21+σ22+σ23+σ24)4d1+3d2+μ+γ3.555>1.

    Theorem 3 implies that the disease is persistent in the mean. Interestingly, in Figure 2, it is clear that the number of infected individuals is higher than that of susceptible individuals.

    Figure 2.  The disease persists in both groups at initial values (S(0),I(0),M(0),V(0))=(500,500,500,500).

    Example 3. Choose the parameters Λ1=35000, Λ2=30000, β1=0.05, β2=0.000002, β3=0.069, β4=0.069, α1=0.1, α2=0.12, α3=0.12, μ=0.23, γ=0.2, d1=0.5, d2=0.058, m=100, σ1=0.015, σ2=0.018, σ3=0.018, σ4=0.02, the initial values μ1=min{μ+d1+γ,d2}, σ=min{σ2, σ4}, β=max{β1, β3}, and the initial values (S(0),I(0),M(0),V(0))=(20000,2000,20000,2000). Using the parameters

    RS3=77(β1β2)β3β4Λ21Λ24/(σ212+σ222+σ232+σ242+2d1+3d2+(μ+γ)+β1α1+β3α2+β4α3),
    RS4=88(β1β2)β3β4Λ21Λ24/(σ212+σ222+σ232+σ242+4d1+2d2+(μ+γ)+β1α1+β3α2+β4α3),

    we can obtain that RS2={RS3,RS4}49.720>1 and the conditions of Theorem 4 are satisfied. Figure 3 shows the histograms of solutions of model (1.2) with white noise. Theoretical conclusions and numerical simulations indicate that the disease will eventually prevail and persist for a long time.

    Figure 3.  Histograms with 100 bins generated from 50,000 simulations of the model (1.2), where the red curves are the probability density functions.

    Example 4. Given β2=0, different transmission rates β1, = 0, 0.02, 0.05, 0.08, 0.12. When the transmission rate β1= 0.05, we select that β2 = 0, 0.006, 0.01, 0.012, 0.016, 0.02. The rest parameters are the same as in the Example 1. Figure 4 shows that as β1 changes from 0, it significantly impacts the system. As β2 increases, the numbers of infections decreases. This shows that the existence of direct transmission via this transmission route has an significant influence on disease transmission, and that reducing the rate of human-to-human contact through media coverage can reduce the scale of vector-borne infectious diseases.

    Figure 4.  The number of individuals infected given different parameters β1 and β2.

    This paper presented a direct transmission model that is saturated with stochastic vector-borne disease incidence and the associated dynamical behavior. We obtained the positive definiteness and uniqueness of the solution to the stochastic model. Then, we established sufficient conditions for the extinction of the disease in two populations. Furthermore, we have proven the uniqueness and existence of an ergodic stationary distribution of the model when RS2>1 by choosing a suitable stochastic Lyapunov function.

    On the other hand, from the simulation, we found that the disease under the condition of an increasing transmission rate β1 showed an increasing transmission scale. It reflected that direct transmission i.e., the transmission route, has a critical influence on the spread of vector-borne diseases. In addition, we observed in the numerical experiments that there is indeed an effect on the number of the infected by increasing the value of the β2. This also validates the inhibitory impact of media coverage on the spread of the disease.

    Finally, reviewing the model we built, we have found that model (1.1) becomes the classical SIR model with media coverage if we set β3=β4=0. This means that the disease can be endemic in the host population if there is no transmission pathway from the vector to the host. The threshold parameters obtained in this study do not explain this phenomenon. Some algorithms that guarantee the positivity of the solution are more useful when numerical simulations are performed [48,49]. We leave these issues for future research.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This research was supported by the National Natural Science Foundation of China under grant No. 12061070, the Natural Science Foundation of Xinjiang Uygur Autonomous Region under grant No. 2021D01E13, the 2023 Annual Planning Project of the Commerce Statistical Society of China under grant No. 2023STY61, the Innovation Project the of Excellent Doctoral Students of Xinjiang University under grant No. XJU2023BS017, and the Research Innovation Program for Postgraduates of Xinjiang Uygur Autonomous Region under grant Nos. XJ2023G016 AND XJ2023G017.

    The authors declare that they have no conflict of interest.



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