
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−(β1−β2Im+I)SI1+α1I−β3SV1+α2V−d1S)dt,dI=((β1−β2Im+I)SI1+α1I+β3SV1+α2V−(μ+d1+γ)I)dt,dR=(γI−d1R)dt,dM=(Λ2−β4MI1+α3I−d2M)dt,dV=(β4MI1+α3I−d2V)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−(β1−β2Im+I)SI1+α1I−β3SV1+α2V−d1S)dt+σ1SdB1(t),dI=((β1−β2Im+I)SI1+α1I+β3SV1+α2V−(μ+d1+γ)I)dt+σ2IdB2(t),dM=(Λ2−β4MI1+α3I−d2M)dt+σ3MdB3(t),dV=(β4MI1+α3I−d2V)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}t≥0 that satisfies the usual conditions (i.e., it is increasing and right continuous while F0 contains all P-null sets). Denote Rn+={y∈Rn:yi>0,1≤i≤n}. 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)=y0∈Rn, where B(t) denotes an n-dimensional standard Brownian motion defined on the complete probability space (Ω,F,{Ft}t≥0,P). Define a differential operator L of Eq (2.1) as follows
L=∂∂t+n∑i=1fi(y,t)∂∂yi+12n∑i,j=1[gT(y,t)g(y,t)]ij∂2∂yi∂yj. |
If L acts on a nonnegative function V∈C2,1(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=∂V∂t,Vy=(∂V∂y1,…,∂V∂yn),Vyy=(∂2V∂yi∂yj)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}t⩾0 be a real- valued continuous local martingale vanishing at t=0. Then
limt→∞⟨M,M⟩t=∞a.s.⇒limt→∞Mt⟨M,M⟩t=0.a.s.lim supt→∞⟨M,M⟩tt<∞a.s.⇒limt→∞Mtt=0. a.s. |
Let Y(t) be a regular time-homogeneous Markov process in Rn in the following form
dY(t)=a(Y)dt+k∑i=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 D∈Rn with a regular boundary and the following holds
(i) There is a positive number M such that ∑ni,j=1bij(y)ξiξj≥M|ξ|2,y∈D,ξ∈Rn.
(ii) There exists a nonnegative C2 -function V such that LV is negative for any Rn∖D; then
P{lim supT→∞1T∫T0f(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 t≥0 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 k0≥1 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 k≥k0, 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∞=limk→∞τk with 0≤τ∞≤τe 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{τk≤T}>ϵ for all k≥k1. Define a C2-function W:R4→R+ and
W(S(t),I(t),M(t),V(t))=(S(t)−1−logS(t))+(I(t)−1−logI(t))+(M(t)−1−logM(t))+(V(t)−1−logV(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))=[(1−1S)(Λ1−(β1−β2Im+I)SI1+α1I−β3SV1+α2V−d1S)+12σ21+(1−1I)((β1−β2Im+I)SI1+α1I+β3SV1+α2V−(μ+d1+γ)I)+12σ22+(1−1M)(Λ2−β4MI1+α3I−d2M)+12σ23+(1−1V)(β4MI1+α3I−d2V)+12σ24]dt+σ1(S−1)dB1(t)+σ2(I−1)dB2(t)+σ3(M−1)dB3(t)+σ3(V−1)dB4(t)=LWdt+σ1(S−1)dB1(t)+σ2(I−1)dB2(t)+σ3(M−1)dB3(t)+σ4(V−1)dB4(t), |
where LW:R4+→R+ can be written in the following form
LW(S(t),I(t),M(t),V(t))=[(1−1S)(Λ1−(β1−β2Im+I)SI1+α1I−β3SV1+α2V−d1S)+12σ21+(1−1I)((β1−β2Im+I)SI1+α1I+β3SV1+α2V+(μ+d1+γ)I)+12σ22+(1−1M)(Λ2−β4MI1+α3I−d2M)+12σ23+(1−1V)(β4MI1+α3I−d2V)+12σ24]≤Λ1+Λ2+2d1+2d2+β1α1+β3α2+β4α3+μ+γ+β1I1+α1I+β3V1+α2V−β1S1+α1I−β3SV(1+α2V)I+β4I1+α3I−β4MI(1+α3I)V+12σ21+12σ22+12σ23+12σ24≤Λ1+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(S−1)dB1(t)+σ2(I−1)dB2(t)+σ3(M−1)dB3(t)+σ4(V−1)dB4(t). | (3.3) |
Integrate both sides of Eq (3.3) from 0 to τk∧T. It is easy to get that
∫τk∧T0dW(S(u),I(u),M(u),V(u))≤∫τk∧T0κdu+∫τk∧T0{σ1(S−1)dB1+σ2(I−1)dB2+σ3(M−1)dB3+σ4(V−1)dB4}. | (3.4) |
Setting Ω={τk≤T} for k≥k1 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 k−1−logk or 1k−1+logk. That is to say,
W(S(τk),I(τk),M(τk),V(τk))≥(k−1−logk)∧(1k−1−log1k). | (3.5) |
Combining Eqs (3.4) and (3.5), we have
W(S(0),I(0),M(0),V(0))+κ(τk∧T)≥E[1Ω(ω)W(S(τk),I(τk),M(τk),V(τk))]≥ϵ(k−1−logk)∧(1k−1−log1k), |
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(τk∧T)=∞. |
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>σ21∨σ222 and d2>σ31∨σ422. 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 supt→∞log(I+V)t≤(μ1+σ2∗2)(RS0−1)<0,a.s.. |
Moreover,
limt→∞1t∫t0S(u)du=Λ1d1,limt→∞1t∫t0I(u)du=0a.s.,limt→∞1t∫t0M(u)du=Λ2d2,limt→∞1t∫t0V(u)du=0a.s.. |
Proof. According to Reference [45], we have
limt→∞S(t)t=limt→∞I(t)t=limt→∞M(t)t=limt→∞V(t)t=0, a.s., | (4.1) |
limt→∞∫t0S(u)dB1(u)t=limt→∞∫t0I(u)dB2(u)t=limt→∞∫t0M(u)dB3(u)t=limt→∞∫t0V(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=Λ1−d1t∫t0S(u)du−μ+d1+γt∫t0I(u)du+σ1t∫t0S(u)dB1(u)+σ2t∫t0I(u)dB2(u). |
It is obvious that
1t∫t0S(u)du=Λ1d1−(d1+μ+γ)d1t∫t0I(u)du+σ1d1t∫t0S(u)dB1(t)+σ2d1t∫t0I(u)dB2(t)−S(t)−S(0)d1t−I(t)−I(0)d1t. | (4.3) |
From Eqs (4.1) and (4.2), the limit of Eq (4.3) given by
limt→∞1t∫t0S(u)du=Λ1d1−limt→∞(d1+μ+γd1t∫t0I(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=Λ2−d2t(∫t0M(u)du+∫t0V(u)du)+σ3t∫t0M(u)dB3(u)+σ4t∫t0V(u)dB4(u). |
Combining (4.1) and (4.2), we can get the following equation
limt→∞1t∫t0V(u)du=Λ2d2−limt→∞1t∫t0M(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+(β1−β2Im+I)SI(1+α1I)(I+V)dt−σ22I2(I+V)2dt−σ24V2(I+V)2dt+σ2II+VdB2(t)+σ4VI+VdB4(t)−(μ+d1+γ)II+Vdt−d2VI+Vdt.≤β4MI(I+V)dt+βS(I+V)(I+V)dt+σ22II+VdB2(t)+σ42VI+VdB4(t)−μ1I+VI+Vdt−σ2∗(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)≤βt∫t0S(u)du+β4t∫t0M(u)du+1t∫t0σ2II+VdB2(u)+1t∫t0σ4II+VdB4(u)−1t∫t0σ2∗2dt−1t∫t0μ1du, |
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)d1t∫t0I(u)du)+β4(Λ2d2−1t∫t0V(u)du)+1t∫t0σ2II+VdB2(u)+1t∫t0σ4II+VdB4(u)−1t∫t0σ2∗2dt−1t∫t0μ1du. | (4.6) |
According to Lemma 1, it is obtained that
limt→∞(1t∫t0σ4VI+VdB4(u)+1t∫t0σ2II+VdB2(u))=0,a.s.. | (4.7) |
By using Eqs (4.6) and (4.7), we have
lim supt→∞log(I+V)t≤(μ1+σ2∗2)(RS0−1)<0,a.s.. |
It means that limt→∞1t∫t0I(u)du=0 and limt→∞1t∫t0V(u)du=0,a.s. Combining Eqs (4.4) and (4.5), it is obvious that
limt→∞1t∫t0S(u)du=Λ1d1,limt→∞1t∫t0M(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>σ21∧σ222 and d2>σ31∧σ422. If
RS1=99√Λ21Λ2d21d2(β1−β2)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)limt→∞1t∫t0S(u)du≥Λ1d1+β1/α1+β2/α2,a.s..(ii)limt→∞1t∫t0M(u)du≥Λ2d2+β4/α3,a.s..(iii)limt→∞1t∫t0I(u)du+limt→∞1t∫t0V(u)du≥4d1+3d2+μ+γ(β1+β4+d1α3+d1α1)∧(β3+d2α2)(RS1−1),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=Λ1−1t∫t0(β1−β2I(t)I(t)+m)S(u)I(u)1+α1I(u)du−1t∫t0β3S(u)V(u)1+α2V(u)du−1t∫t0d1S(u)du−σ1t∫t0S(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+σ1t∫t0S(u)dB1(u)≥Λ1−1t∫t0β1S(u)α1du−1t∫t0β3S(u)α2du−1t∫t0d1S(u)du. | (5.1) |
Through the strong law of large numbers for local martingales, we have
limt→∞(S(t)−S(0)t+σ1t∫t0S(u)dB1(u))=0a.s., |
which together with Eq (5.1) yields
limt→∞1t∫t0S(u)du≥Λ1d1+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=Λ2−1t∫t0β4M(u)I(u)1+α3I(u)du−1t∫t0d2M(u)du−σ3t∫t0M(u)dB3(u). |
Then
M(t)−M(0)t+σ3t∫t0M(u)dB3(u)≥Λ2−1t∫t0β4M(u)α3du−1t∫t0d2M(u)du. | (5.2) |
According to the strong law of large numbers of local martingales, we have
limt→∞(M(t)−M(0)t+σ3t∫t0M(u)dB3(u))=0a.s., |
which together with Eq (5.2) yields
limt→∞1t∫t0M(u)du≥Λ2d2+β4/α3a.s.. |
This is the required assertion (ii).
(iii) First, define a function W2(S,I,V)=−lnS−lnI−lnM−lnV. According to the Itô's formula:
dW2(t)=LW2(t)dt−σ1dB1(t)−σ2dB2(t)−σ3dB3(t)−σ4dB4(t), |
where
LW2(t)=−1S(Λ1−(β1−β2Im+I)SI1+α1I−β3SV1+α2V−d1S)−1I((β1−β2Im+I)SI1+α1I+β3SV1+α2V−(μ+d1+γ)I)−1M(Λ2−β4MI1+α3I−d2M)−1V(β4MI1+α3I−d2V)−12(σ21+σ22+σ23+σ24)=−Λ1S+β1I1+α1I−(β2Im+I)I1+α1I+β3V1+α2V+d1−β3SVI(1+α2V)−(β1−β2Im+I)S1+α1I+(d1+μ+γ)−Λ2M+β4I(1+α3I)−β4MIV(1+α3I)+2d2−d2(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)V−Λ12S−Λ2M−β4MIV(1+α3I)−β3SVI(1+α2V)−(β1−β2)S1+α1I−Λ12S−d2(1+α2V)−d1(1+α3I)−d1(1+α1I)+(4d1+3d2+μ+γ)−12(σ21+σ22+σ23+σ24)≤(β1+β4+d1α3+d1α1)I+(β3+d2α2)V−99√Λ21Λ2d21d2(β1−β2)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,
0≤−99√Λ21Λ2d21d2(β1−β2)β3β4+(4d1+3d2+μ+γ)−12(σ21+σ22+σ23+σ24)+limt→∞(β1+β4+d1α3+d1α1)t∫t0I(u)du+limt→∞(β3+d2α2)t∫t0V(u)du−limt→∞1t∫t0σ1dB1(u)−limt→∞1t∫t0σ2dB2(u)−limt→∞1t∫t0σ3dB3(u)−limt→∞1t∫t0σ4dB4(u). | (5.3) |
According to the law of large numbers for a martingale,
limt→∞1t∫t0σ1dB1(u)=limt→∞1t∫t0σ2dB2(u)=limt→∞1t∫t0σ3dB3(u)=limt→∞1t∫t0σ4dB4(u)=0. |
It follows that Eq (5.3) becomes
limt→∞(β1+β4+d1α3+d1α1)t∫t0I(u)du+limt→∞(β3+d2α2)t∫t0V(u)du≥99√Λ21Λ2d21d2(β1−β2)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√(β1−β2)β3β4Λ21Λ24,RS4=8r28√(β1−β2)β3β4Λ21Λ24, |
where r1=12∑4i=1σ2i+2d1+3d2+μ+γ+β1α1+β3α2+β4α3, and r2=12∑4i=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)∈D⊂R4+{σ21S2,σ22I2,σ23M2,σ24V2}. It follows that
4∑i,j=1bij(S,I,M,V)ξiξj=σ21S2ξ21+σ22E2ξ22+σ23I2ξ23+σ24R2ξ24≥M|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=−logS−logM−logV−logI+α2d2V,V2=−logS−logM−logV+(α1+α3)(S+I),V3=−logS−logM,V4=1θ+2(S+I+M+V)θ+2. |
Denote λi=ri(Ri−1)(i=1,2), σ2=σ21∨σ22∨σ23∨σ24, b=2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232 and d=d1∧d2. 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+F2≤−3, −Θ2λ2+F3≤−2, and
F2=sup(S,I,M,V)∈R4+{12(α2d2β4)2M2−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+b+B},F3=sup(S,I,M,V)∈R4+{Θ1α2d2β4MI−12(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+1−12(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[Λ1−d1S−(β1−β2II+m)SI1+α1I−β3SV1+α2V]+σ212−1I[−(d1+μ+γ)I+(β1−β2II+m)SI1+α1I+β3SV1+α2V]+σ222−1M[Λ1−β4MI1+α3I−d2M]+σ232−1V[β4MI1+α3I−d2V]+σ242−α2d2β4MI(1+α3I)−d2α2V≤−Λ12S−Λ2M−(β1−β2)S1+α1I−Λ12S−β3SV(1+α2V)I+β4MI(1+α3I)V+d2(1+α2V) |
+σ212+σ222+σ232+σ242+2d1+3d2+(μ+γ)+β1α1+β3α2+β4α3+α2d2β4MI≤−77√(β1−β2)β3β4Λ21Λ24(1+α1I)(1+α3I)+σ212+σ222+σ232+σ242+2d1+3d2+(μ+γ)+β1α1+β3α2+β4α3+α2d2β4MI,LV2=−1S[Λ1−d1S−(β1−β2II+m)SI1+α1I−β3SV1+α2V]+σ212−1I[−(d1+μ+γ)I+(β1−β2II+m)SI1+α1I+β3SV1+α2V]+σ222−1M[Λ1−β4MI1+α3I−d2M]+σ242−1V[β4MI1+α3I−d2V]+σ242−d1(α1+α3)I−d1(α1+α3)S−(μ+γ)(α1+α3)I≤−Λ12S−Λ2M−(β1−β2)S1+α1I−Λ12S−β3SV(1+α2V)I−β4MI(1+α3I)V−d1(1+α1I)−d1(1+α3I)+σ212+σ222+σ232+σ242+4d1+2d2+(μ+γ)+β1α1+β3α2+β4α3≤−88√(β1−β2)β3β4Λ21Λ24(1+α3V)+σ212+σ222+σ232+σ242+4d1+2d2+(μ+γ)+β1α1+β3α2+β4α3, |
LV3=−1S[Λ1−d1S−(β1−β2II+m)SI1+α1I−β3SV1+α2V]+σ212−1M[Λ2−β4MI1+α3I−d2M]+σ232≤−Λ1S−Λ2M+2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232,LV4=(S+I+M+V)θ+1[Λ1−d1(S+I+R)−(μ+γ)I+Λ2−d2(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(d1∧d2)+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+2≤B−12(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+1−12(d−(θ+1)σ22)(S+I+M+V)θ+2}<∞. |
Thus, it follows that
LV≤−Θ1r1(RS3−1)−Θ2r2(RS4−1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+Θ1(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)−Λ1S−Λ2M. |
A closed subset is defined as follows:
D={(S,I,M,V)∈R4+:ϵ⩽S⩽1ϵ,ϵ⩽I⩽1ϵ,ϵ⩽M⩽1ϵ,ϵ⩽V⩽1ϵ}, |
where ϵ>0 represents sufficiently small constants satisfying the following conditions
−Λ1ϵ+F3<1, | (6.1) |
−Θ1r3(77√(β1−β2)β3β4Λ21Λ24(1+αϵ)(1+αϵ)−1)+F2+Θ21ϵ22<−1, | (6.2) |
H+Θ1(α2d2β4)1ϵ2−12(d−(θ+1)σ22)(1ϵ)θ+2<−1, | (6.3) |
−Λ2ϵ+F2<−1, | (6.4) |
−Θ2r2(88√(β1−β2)β3β4Λ21Λ24(1+α3ϵ)−1)+F3<−1, | (6.5) |
H+Θ1(α2d2β4)1ϵ2−12(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={Y∈R4+,0<S<ϵ},D2={Y∈R4+,0<I<ϵ},D3={Y∈R4+,S>1ϵ,ϵ<M<1ϵ,ϵ<I<1ϵ},D4={Y∈R4+,I>1ϵ,ϵ<M<1ϵ},D5={Y∈R4+,0<M<ϵ},D6={Y∈R4+,0<V<ϵ4,},D7={Y∈R4+,1ϵ<M,ϵ<I<1ϵ},D8={Y∈R4+,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
LV≤2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)−Λ1S≤−Λ1S+F3≤−Λ1ϵ+F3, |
where
F3=sup(S,I,M,V)∈R4+{Θ1α2d2β4MI−12(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
LV≤−Θ1r3(77√(β1−β2)β3β4Λ21Λ24(1+α1I)(1+α3I)−1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+(α2d2β4)2M22+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+Θ21I22≤−Θ1r3(77√(β1−β2)β3β4Λ21Λ24(1+α1ϵ)(1+α3ϵ)−1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+(α2d2β4)2M22+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)+Θ21ϵ22≤−Θ1r3(77√(β1−β2)β3β4Λ21Λ24(1+α1ϵ)(1+α3ϵ)−1)+F2+Θ21ϵ22, |
where
F2=sup(S,I,M,V)∈R4+{12(α2d2β4)2M2−12(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
LV≤d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)≤H+Θ1(α2d2β4)1ϵ2−12(d−(θ+1)σ22)(1ϵ)θ+2≤H+Θ1(α2d2β4)1ϵ2−12(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
LV≤2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)≤H+Θ1(α2d2β4)1ϵ2−12(d−(θ+1)σ22)(1ϵ)θ+2=H+Θ1(α2d2β4)(1ϵ)2−12(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
LV≤2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)−Λ2M≤−Λ2M+F3≤−Λ1ϵ+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
LV≤−Θ2r2(88√(β1−β2)β3β4Λ21Λ24(1+α3V)−1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+Θ(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)≤−Θ2r2(88√(β1−β2)β3β4Λ21Λ24(1+αϵ)−1)+2d1+μ+γ+β1α1+β3α2+β4α3+σ21+σ232+Θ(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)≤−Θ2r2(88√(β1−β2)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
LV≤2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)≤d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)1ϵ2+B−12(d−(θ+1)σ22)(1ϵ)θ+2≤H+Θ1(α2d2β4)1ϵ2−12(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
LV≤2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)MI+B−12(d−(θ+1)σ22)(Sθ+2+Iθ+2+Mθ+2+Vθ+2)≤2d1+μ+γ+β1α1+β4α3+β3α2+σ21+σ232+Θ1(α2d2β4)1ϵ2+B−12(d−(θ+1)σ22)(1ϵ)θ+2≤H+Θ1(α2d2β4)1ϵ2−12(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+(Λ1−d1Si−(β1−β2Iim+Ii)SiIi1+α1Ii−β3SiVi1+α2Vi)Δt+Si(σ1√Δtζ1i+σ12Si(ζ21i−1)Δt),Ii+1=Ii+((β1−β2Iim+Ii)SiIi1+α1Ii+β3SiVi1+α2Vi−(d1+μ+γ)Ii)Δt+Ii(σ2√Δtζ2i+σ222Ii(ζ22i−1)Δt),Mi+1=Mi+(Λ2−β4MiIi1+α3Ii−d2Mi)Δt+Mi(σ3√Δtζ3i+σ232Mi(ζ23i−1)Δt),Vi+1=Vi+(β4MiIi1+α3Ii−d2Vi)Δt+Vi(σ4√Δtζ4i+σ242Vi(ζ24i−1)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.
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=99√Λ21Λ2d21d2(β1−β2)β3β4+12(σ21+σ22+σ23+σ24)4d1+3d2+μ+γ≈3.555>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.
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√(β1−β2)β3β4Λ21Λ24/(σ212+σ222+σ232+σ242+2d1+3d2+(μ+γ)+β1α1+β3α2+β4α3), |
RS4=88√(β1−β2)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.
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.
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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