
In this study, considering the effect of environment perturbation which is usually embodied by the alteration of contact infection rate, we formulate a stochastic epidemic mathematical model in which two different kinds of infectious diseases that spread simultaneously through both horizontal and vertical transmission are described. To indicate our model is well-posed and of biological significance, we prove the existence and uniqueness of positive solution at the beginning. By constructing suitable Lyapunov functions (which can be used to prove the stability of a certain fixed point in a dynamical system or autonomous differential equation) and applying Itˆo's formula as well as Chebyshev's inequality, we also establish the sufficient conditions for stochastic ultimate boundedness. Furthermore, when some main parameters and all the stochastically perturbed intensities satisfy a certain relationship, we finally prove the stochastic permanence. Our results show that the perturbed intensities should be no greater than a certain positive number which is up-bounded by some parameters in the system, otherwise, the system will be surely extinct. The reliability of theoretical results are further illustrated by numerical simulations. Finally, in the discussion section, we put forward two important and interesting questions left for further investigation.
Citation: Xunyang Wang, Canyun Huang, Yixin Hao, Qihong Shi. A stochastic mathematical model of two different infectious epidemic under vertical transmission[J]. Mathematical Biosciences and Engineering, 2022, 19(3): 2179-2192. doi: 10.3934/mbe.2022101
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In this study, considering the effect of environment perturbation which is usually embodied by the alteration of contact infection rate, we formulate a stochastic epidemic mathematical model in which two different kinds of infectious diseases that spread simultaneously through both horizontal and vertical transmission are described. To indicate our model is well-posed and of biological significance, we prove the existence and uniqueness of positive solution at the beginning. By constructing suitable Lyapunov functions (which can be used to prove the stability of a certain fixed point in a dynamical system or autonomous differential equation) and applying Itˆo's formula as well as Chebyshev's inequality, we also establish the sufficient conditions for stochastic ultimate boundedness. Furthermore, when some main parameters and all the stochastically perturbed intensities satisfy a certain relationship, we finally prove the stochastic permanence. Our results show that the perturbed intensities should be no greater than a certain positive number which is up-bounded by some parameters in the system, otherwise, the system will be surely extinct. The reliability of theoretical results are further illustrated by numerical simulations. Finally, in the discussion section, we put forward two important and interesting questions left for further investigation.
In all periods of the development of human society, there are arduous struggles against various infectious diseases [1]. What makes matters worse is multiple infectious diseases often exist on human individuals at the same time, and the coordinated and cross-infection between infectious diseases makes the course of the disease more complicated and difficult to deal with. We often refer to this situation as the parallel development of multiple infectious diseases [2]. The probability of several infectious diseases in a patient at the same time is related to the environment, susceptible population and human immunity. If the sanitary environment is poor, and there are sewage, excreta, animal and plant residues, mosquitoes and mice everywhere, the probability of N kinds of infectious diseases taking place in parallel will be very high. If people with bad living habits, sanitation workers, medical staff in the infection department and other personnel are frequently exposed to a large number of pathogenic microorganisms, the probability of suffering from N kinds of infection rate is also very high. In addition, people with immune system defects or injuries have a high rate of N infectious diseases [3]. Therefore, it is very common for multiple infectious diseases to occur in the same individual. For example, patients with advanced AIDS have a 100% chance of contracting N diversified infectious diseases when exposed to other infection environment besides AIDS [4,5].
Recently, the researches on modelling two types of infectious diseases have drawn many applied mathematicians' attention [6,7,8,9,10,11]. In [6], the authors discussed an epidemic model with double hypothesis combined two different transmission mechanisms. In [7], a stochastic SIRS epidemic model with two different viruses is built to study the effect of intensities from white noise on each individual, and further discussed the dynamics of threshold around disease-free equilibrium as well as endemic equilibrium. In [8], they proposed a new mathematical model with nonlinear incidence rate and two fundamental epidemic hypothesis.
Besides, some researchers have also noticed the phenomena of infectious diseases under vertical transmission and they feel interested in modelling the epidemic with this phenomena [11,12,13,14,15]. For instance, Ackleh A.S. et al. studied the epidemic model with multi-disease and vertical transmission [10,11]. What is vertical transmission infection? It refers to the phenomenon that some infectious diseases pass from the infected mother to the offspring through the blood system and reproductive system, so that the child becomes an infectious disease patient at birth [15].
Although the literatures above-mentioned studied the very important phenomenon of multiple infectious diseases taking place in parallel with vertical infection, we note that most of them established deterministic models and did not take into account the impact of various stochastic factors on the dynamic behavior of the system, which is not objective enough. In view of this, stochastic models and stochastic analysis methods are necessary to describe a large number of biological and social phenomena [16,17,18,19]. In the process of infectious disease modeling, the contact infection incidence of infectious disease is the most noteworthy for two reasons, one is that it can describe the rate at which susceptible becomes infectious, i.e., the incidence can outline the transmission intensity of infectious diseases to some extent; the other is that it can be easily affected by many subjective and objective factors, such as weather, mood, habits and so on. Therefore, it is more objective to establish a stochastic model to describe the infection process of some infectious diseases. In recent decades, many applied mathematicians and epidemiologists have established a series of stochastic epidemic models and achieved great results by introducing random perturbation into deterministic model [16,17,18,19,20,21,22,23,24,25]. Among these stochastic modeling and analysis literatures, Hattaf K. and coauthors investigated stochastic model with specific functional response and temporary immunity in [20], and proposed a delayed stochastic SIR epidemic model with a general incidence rate in [21]. Din A. and his coauthors recently also carried out a lot of research on dengue [24] and hepatitis B epidemic [22,25] as well as some social behaviours including drinking alcohol [23] by constructing corresponding stochastic models, they studied the stochastic dynamics such as stationary distribution of extinction and persistence [22,23,24,25] and also considered the optimal control on hepatitis B epidemic stochastic model [22].
The reference [11] have discussed the dynamic properties of the system under some different parameters and initial values, on this basis as well as the foregoing mentioned reasons and also motivated by related references mentioned before, in this paper, we will study a stochastic epidemic model with two types of infectious diseases and vertical transmission. By constructing suitable Lyapunov function and using Itˆo's formula and Chebyshev's inequality, the dynamic behaviors of our model is analyzed. Next, numerical simulations are carried out to testify our obtained theoretical conclusions. Finally, we propose two interesting related problems to be discussed and further studied in the last section.
In reference [11], the authors studied the following differential equations:
{dSdt=Λ−(β1I11+I1+β2I2)S+(γ−p2)I2−μS−p1I1+ηR,dI1dt=β1SI11+I1−(μ+α1+δ−p1)I1,dI2dt=β2SI2−(μ+α2+γ−p2)I2,dRdt=δI1−(η+μ)R, | (2.1) |
where S(t) represents the number of susceptible units at time t; I1(t) and I2(t) that represents the number of infected units at time t and R(t) that represents the number of recovered units at time t, the initial condition is noted as S(0)>0,I1(0)>0,I2(0)>0,R(0)>0, the total population is thus N(t)=S(t)+I1(t)+I2(t)+R(t). It is assumed that there is a constant quantity of populations entering to the deterministic model with recruitment rate Λ>0. There is a vertical transmission of both the two diseases; specifically, the infectious individual gives new birth to a infected individual at the rates 0≤p1≤1 and 0≤p2≤1 for the disease I1 and I2, respectively. Consequently, p1I1 and p2I2 units will enter into infected compartments I1 and I2, respectively, and the same quantities are removing from recruitment in the susceptible compartment. The diseases are both transmitted by contact between the individuals in the S compartment and those in Ii(i=1,2) compartments with nonlinear incidence rate for I1 that is described by β1SI11+I1, where β1>0 represents the infection power rate, and linear incidence rate for I2 that is similarly described by β2SI2, in which β2>0 represents the infection rate. The units in the I1 compartment are experiencing death because of the disease at infection death rate α1≥0. They will also recover from the disease and get immunity at a recovered rate δ>0. The units in the I2 compartment are also confronting death for the disease at infection death rate α2≥0. They will also recover from the disease and return back to be susceptible at recovery rate γ>0. Furthermore, the individuals in the R compartment will lose immunity rate 0≤η<1. There is a natural death rate μ>0 for every member in the total population. A particularly noteworthy assumption is that both the two diseases cannot be transmitted to the same individual at the same time. Moreover, to insure that the recruitment Λ in the susceptible compartment is always positive, the following hypotheses are assumed to be hold always:
δ≥p1,γ≥p2. |
The model (2.1) can usually be applied in the environment where the people will probably suffer from two different infectious epidemic, but the same individual will not suffer from these two diseases at the same time, because in one way people around are highly alert to the patients with these two diseases, in another way patients themselves will consciously minimize contact with the outside world. The environment where the two infectious diseases coexist is quite complex. There are some uncertain factors in the process of disease infection and transmission. These factors often play a key role in the dynamics of infectious disease infection and transmission, which can not be ignored. Therefore, in this paper, taking the effect of stochastically fluctuating environment into account, we can embody the fluctuations from the environment in the parameter β1,β2 as follows
β1→β1+σ1˙B1(t),β2→β2+σ2˙B2(t). | (2.2) |
where Bi(t)(i=1,2) is standard Brownian motions with B(0)=0, and with intensity of white noise σ2i>0(i=1,2). Therefore, based on deterministic model (2.1), we can derive the corresponding stochastic model which takes the following form:
{dS=[Λ−(β1I11+I1+β2I2)S+(γ−p2)I2−μS−p1I1+ηR]dt−σ1SI11+I1dB1(t)−σ2SI2dB2(t),dI1=[β1SI11+I1−(μ+α1+δ−p1)I1]dt+σ1SI11+I1dB1(t),dI2=[β2SI2−(μ+α2+γ−p2)I2]dt+σ2SI2dB2(t),dR=[δI1−(η+μ)R]dt. | (2.3) |
Next, we introduce some fundamental theory in stochastic differential equation (please see [16]).
Let (Ω,F,P) be a complete probability space with a filtration {Ft}t≥0 which satisfies the usual conditions(i.e., it is right continuous and F0 contains all P−null sets). Let B(t) be an n-dimensional standard Brownian motion defined on this space.
We consider the n-dimensional stochastic differential equation of Itˆo type
dx(t)=f(x(t),t)dt+g(x(t),t)dB(t),t≥t0, | (2.4) |
with initial value x(t0)=x0∈Rn+={x∈Rn+:xi>0,1≤i≤n}. And then we define the differential operator L along with system (2.4) as
L=∂∂t+n∑i=1fi(x,t)∂∂xi+12n∑i,j=1[gτ(x,t)g(x,t)]i,j∂2∂xi∂xj. |
We act the operator L on a function V∈C2,1(Rn×R+;R+), thus
LV(x,t)=Vt(x,t)+Vx(x,t)f(x,t)+12trace[gτ(x,t)Vxx(x,t)g(x,t)], |
where
Vt=∂V∂t,Vx=(∂V∂x1,⋯,∂V∂xn),Vxx=(∂2V∂xi∂xj)n×n. |
Lemma 1. (Itˆ0′sformula) ([20]) Assume x(t) to be an Itˆo process on t≥0 of system (2.4), V∈C2,1(Rn×R+;R+), then the function V(x(t),t) is still an Itˆo process with the stochastic differential given by
dV(x(t),t)=LV(x(t),t)dt+Vx(x(t),t)g(x(t),t)dB(t). |
Lemma 2. (Chebyshev′sinequality) ([16])
E(|X|≥c)≤c−pE|X|p,p>1. |
In this part, in order to show our model is well-posed, by using the Lyapunov analysis method and Itˆo′s formula, we will prove that there is a unique global positive solution of system (2.3).
Theorem 3.1. For any initial value (S(0),I1(0),I2(0),R(0))∈R4+, there exists a unique solution (S(t),I1(t),I2(t),R(t)) of system (2.3) for t≥0, and the solution will remain in R4+ with probability 1, i.e., (S(t),I1(t),I2(t),R(t))∈R4+ for all t≥0 almost surely.
proof. It can be easily found that the coefficients of the system (2.3) are locally Lipschitz continuous (which means for SDE dXt=b(t,Xt)dt+σ(t,Xt)dBt, b(t,Xt) and σ(t,Xt) satisfy |b(t,x)−b(t,y)|+|σ(t,x)−σ(t,y)|≤D|x−y| for ∀x,y and t>0, here D>0 is a constant [20]) for all given initial values (S(0),I1(0),I2(0),R(0))∈R4+, therefore, there must exist a unique local solution (S(t),I1(t),I2(t),R(t)) on t∈[0,τe), where τe is called explosion time [19]. Next, in order to show this solution is global, we need to prove that τe=∞ a.s.. Let k0≥0 be sufficiently large so that all the initial values S(0),I1(0),I2(0) and R(0) can lie within the interval [1k0,k0]. For each integer k≥k0, we define the stopping time
τk=inf{t∈[0,τe):S(t)∉(1k,k)orI1(t)∉(1k,k)orI2(t)∉(1k,k)orR(t)∉(1k,k)}, |
and then we set inf∅=∞(as usual ∅ denotes the empty set). Obviously, τk is increasing when k→∞. We set τ∞=limk→∞τk, hence τ∞≤τe a.s.. To finish the proof, we need to show that τ∞=∞ a.s. in the end. We select the proof by contradiction. If this statement is not ture, then there exist two constants T>0 and ε∈(0,1) such that
P{τ∞≤T}>ε. |
Hence, there is an integer k1≥k0 such that for any k≥k1
P{τk≤T}≥ε. | (3.1) |
We define a C2-function V: R4+→R+ by
V(S,I1,I2,R)=(S−1−lnS)+(I1−1−lnI1)+(I2−1−lnI2)+(R−1−lnR). |
The nonnegativity of this function can be easily derived from u−1−lnu≥0,u>0.
Let k≥k0 and T>0 be arbitrary. By virtue of the Itˆo′s formula, we obtain
dV(S,I1,I2,R)=LVdt+σ11+I1(I1−S)dB1(t)+σ2(I2−S)dB2(t), | (3.2) |
where
LV=[Λ−μ(S+I1+I2+R)−α1I1−α2I2]−Λ+(γ−p2)I2−p1I1+ηRS |
−β1(S−I1)1+I1−β2(S−I2)−δI1R+(4μ+α1+α2+δ+γ+η−p1−p2) |
+σ21(S2+I21)2(1+I1)2+12σ22(S2+I22) |
≤Λ+4μ+α1+α2+δ+γ+η+σ21(S2+I21)2(1+I1)2+12σ22(S2+I22)≜H, |
where H is obviously a positive constant. Hence,
dV(S,I1,I2,R)≤Hdt+σ1(I2−S)1+I1dB1(t)+σ2(I2−S)dB2(t). |
We integrate both sides of the above inequality from 0 to τk∧T, then we can derive
∫τk∧T0dV(S(s),I1(s),I2(s),R(s))≤∫τk∧T0Hds |
+∫τk∧T0[σ1(I1(s)−S(s))1+I1(s)dB1(s)+σ2(I2(s)−S(s))dB2(s)], |
where T∧τk=min{τk,T}. And then we take the expectations along the two sides of the above equality, we derive the further relation equality as
EV(S(τk∧T),I1(τk∧T),I2(τk∧T),R(τk∧T))≤V(S(0),I1(0),I2(0),R(0))+HT. |
Let Ωk={τk≤T} for k≥k1 and from Eq (3.1), we have P(Ωk)≥ε. For every ν∈Ωk, S(τk,ν), I1(τk,ν), I2(τk,ν), R(τk,ν) equals either k or 1k; hence V(S(τk,ν), I1(τk,ν), I2(τk,ν), R(τk,ν)) is no less than min{k−1−lnk,1k−1−ln1k}.
Then we obtain
V(S(0),I1(0),I2(0),R(0))+HT≥E[1Ωk(ν)V(S(τk),I1(τk),I2(τk),R(τk))] |
≥εmin{k−1−lnk,1k−1−ln1k}, |
where 1Ωk(ν) is the indicator function of Ωk.
Taking limit process n→∞, the contradiction ∞=V(S(0),I1(0),I2(0),R(0))+HT<∞ appears.
Thus, we complete the proof.
In this section, we will study the stochastic permanence of system (2.3).
Definition 4.1. ([20]) The solution X(t)=(S(t),I1(t),I2(t),R(t)) of system (2.3) is called stochastically permanent, if for all ε∈(0,1) and all initial value (S(0),I1(0),I2(0),R(0))∈R4+, two positive constants λ=λ(ε) and χ=χ(ε) can be found to make the solution of system (2.3) X(t) satisfies the properties
lim inft→∞P{|X(t)|≤χ}≥1−ε,lim inft→∞P{|X(t)|≥λ}≥1−ε. |
Theorem 4.1. For any initial value (S(0),I1(0),I2(0),R(0))∈R4+, the solution X(t)=(S(t),I1(t),I2(t),R(t)) satisfies
lim supt→∞E(|X(t)|−ϑ)≤Q, | (4.1) |
where ϑ is an arbitrary positive constant satisfying
ϑ+12(μ+max{1,α1,α2}+2max{σ21,σ22})<Λ, | (4.2) |
Q=4ϑ(4kϑΛ+C2)4kϑΛmax{1,(2ϑΛ+C+√4kϑΛ+C22ϑΛ)ϑ−1}, | (4.3) |
in which
0<k<ϑ[2Λ−(μ+max{1,α1,α2}+2max{σ21,σ22})], | (4.4) |
C=k+ϑ(μ+max{1,α1,α2}+2max{σ21,σ22}). | (4.5) |
proof. Firstly, we define a function V(S,I1,I2,R)=1S+I1+I2+R, (S(t),I1(t),I2(t),R(t))∈R4+; applying Itˆo′s formula, we get
dV(S,I1,I2,R)=[μV+V2(α1I1+α2I2−Λ)+2V3(σ21S2I21(1+I1)2+σ22S2I22)]dt. |
Selecting a positive constant ϑ that satisfies Eq (4.2) and using Itˆo′s formula, we can obtain
L(1+V)ϑ=ϑ(1+V)ϑ−1[μV+V2(α1I1+α2I2−Λ)+2V3(σ21S2I21(1+I1)2+σ22S2I22)]=ϑ(1+V)ϑ−1G, |
where G=μV+V2(α1I1+α2I2−Λ)+2V3(σ21S2I21(1+I1)2+σ22S2I22).
Since
V2(α1I1+α2I2)<V2(S+α1I1+α2I2+R) |
<V2max{1,α1,α2}(S+I1+I2+R)=Vmax{1,α1,α2}, |
2V3(σ21S2I21(1+I1)2+σ22S2I22)<2V3max{σ21,σ22}(S2+S2I22)<2Vmax{σ21,σ22}, |
Therefore,
G<(μ+max{1,α1,α2}+2max{σ21,σ22})V−ΛV2. |
Let k>0 be small enough and satisfy Eq (4.4), by virtue of Itˆo's formula
L(ekt(1+V)ϑ)=kekt(1+V)ϑ+ektL(1+V)ϑ |
<ekt(1+V)ϑ−1[k(1+V)+ϑ(μ+max{1,α1,α2}+2max{σ21,σ22})V−ϑΛV2] |
=ekt(1+V)ϑ−1[k+CV−ϑΛV2]≤ektW, |
where
W=4kϑΛ+C24kϑΛmax{1,(2ϑΛ+C+√4kϑΛ+C22ϑΛ)ϑ−1}, |
and the definition of C can be found in the statement of the theorem.
Consequently,
d(ekt(1+V)ϑ)≤Wektdt. |
We again integrate both sides of the above inequality from 0 to t, and then we can get
ekt(1+V)ϑ≤(1+V(0))ϑ+Wk(ekt−1)≤(1+V(0))ϑ+Wkekt. |
⇒(1+V)ϑ≤Wk+(1+V(0))ϑe−kt |
⇒E(1+V)ϑ≤Wk+(1+V(0))ϑe−kt. |
Hence, in the end, we obtain
lim supt→∞E(V(t))ϑ≤lim supt→∞E(1+V)ϑ≤Wk. |
For (S,I1,I2,R)∈R4+, we know that
(S+I1+I2+R)ϑ≤4ϑ(S2+I21+I22+R2)ϑ2≤4ϑ|X(t)|ϑ; |
Thus, we come to the final conclusion
lim supt→∞E(1|X(t)|ϑ)≤4ϑlim supt→∞E(V(t))ϑ≤4ϑWk=Q, |
which completes the proof.
Theorem 4.2. The solutions of system (2.3) are stochastically permanent on condition that
max{σ21,σ22}<Λ−μ+max{1,α1,α2}2. |
proof. From Theorem 4.1, we have P{|X(t)|>χ}<ε which implies P{|X(t)|≤χ}≤1−ε. This follows that lim inft→∞P{|X(t)|≤χ}≥1−ε.
By Theorem 4.1, we get lim supt→∞E(1|X(t)|ϑ)≤Q.
For any ε>0, let λ=ε1ϑQ1ϑ; and then by virtue of Chebyshev's inequality,
P{|X(t)|<λ}=P{1|X(t)|>1λ}≤λϑE(|X(t)|−ϑ). |
Hence,
lim supt→∞P{|X(t)|<λ}≤εQ⋅Q=ε, |
which means the following assertion is correct.
lim inft→∞P{|X(t)|≥λ}≥1−ε. |
The proof is thus completed.
Compared with the existence, uniqueness and boundedness of positive solutions, the stochastic permanence condition of the model solution is much more stringent. Specifically, some main parameters, i.e., the recrument rate Λ, disease-related mortality α1,α2, natural mortality μ and all the perturbed intensities σ1,σ2 should satisfy max{σ21,σ22}<Λ−μ+max{1,α1,α2}2. From a biological point of view, stochastic permanence means that after a long enough time, the probability of population size of all compartment in model (2.3) being too large or too small is very low. Stochastic permanence is equivalent to both random upper bounded and random lower bounded. It implies that the population size in all compartments is relatively stable. It should be further pointed out that when the conditions of the theorem cannot be met, the model will die out, that is, part of the compartments population will eventually die out.
In this part, we will use the Milstein method proposed in Higham [21] to illustrate our main assertions for the stochastic system (2.3). The Milstein method has been developed from the deterministic Euler method with strong order of convergence γ=12. By adding a correction to the stochastic increment to raise the strong order of Euler method to 1, making Milstein¡¯s method. Therefore, the order of convergence of Milstein method in this paper is 1.
To begin with, let we consider the following discretization equations:
{Sk+1=Sk+[Λ−(β1I1k1+I1k+β2I2k)Sk+(γ−p2)I2k−μSk−p1I1k+ηRk]Δt−σ1SkI1k1+I1k√Δtξk−σ2SkI2k√Δtξk+σ212(SkI1k1+I1k)2(ξ2k−1)Δt+σ222S2kI22k(ξ2k−1)Δt,I1k+1=I1k+[β1SkI1k1+I1k−(μ+α1+δ−p1)I1k]Δt+σ1SkI1k1+I1k√Δtξk+σ212(SkI1k1+I1k)2(ξ2k−1)Δt,I2k+1=I2k+[β2SkI2k−(μ+α2+γ−p2)I2k]Δt+σ2SkI2k√Δtξk+σ222S2I22k(ξ2k−1)Δt,Rk+1=Rk+[δI1k−(η+μ)Rk]Δt, | (5.1) |
where ξk(k=1,⋯,n) is called the Guassian random variables which Obey Gaussian distribution N(0,1).
To testify our main results in this paper, according to the biological meanings of relative parameters and initial values, we select the rational parameters values as Λ=2,β1=0.75,β2=0.3,γ=0.75,p1=0.01,p2=0.05,μ=0.3,η=0.5,δ=0.7,α1=0.1,α2=0.6, and also proper initial value (S(0),I1(0), I2(0),R(0)) = (5, 4, 2, 3). Then the related pathwise estimation of the solutions of system (2.3) are presented in Figure 1. Since the intensity of white noise σ1 and σ2 are both difficult to measure in actual situations, therefore, we estimate the values of them according to the conditions presented in our theorems with the method in [22]. Let σ1=0.04,σ2=0.06, the solutions of system (2.3) are stochastically permanent(Figure 1(a)). Let σ1=0.2,σ2=0.1 and the condition of Theorem 4.2 is satisfied, we can see that the larger intensity of the white noise will weaken the stability of the system (Figure 1(b)).
When σ1=σ2=0.0, system (2.3) will be deterministic and its time-series plots shown by Figure 2(a). We select σ1=1.0,σ2=1.3 not to satisfy the condition of Theorem 4.2, then the noise can make the population become largely fluctuating. In this condition, the solutions of system (2.3) are not stochastically permanent(please see Figure 2(b)).
In this paper, in order to investigate the effect of stochastic perturbation from the environment on dynamical behaviours of two different infectious epidemic with vertical transmission, we derived a stochastic model based on the deterministic model from literature [11]. For the established stochastic model, using the methods and techniques of stochastic analysis, we systematically study the existence and uniqueness of positive solutions, stochastic ultimate boundedness, stochastic persistence and other related issues of the system. We draw the following conclusions:
1) No matter which positive number the initial value takes and independent on the selection of parameters, stochastic system (2.3) always exists a unique positive solution and never explode(i.e., the positive solution is ultimate bounded). It shows our stochastic model is well-posed and biologically significant.
2) Further, when the intensities of stochastic perturbation from environment σ21,σ22 are both not rather large with a upper bound described by max{σ21,σ22}<Λ−μ+max{1,α1,α2}2, in any limited time, the population of all compartments in the model will not be very large or very small, that is, it will maintain the so-called stochastic permanence. This means that when the stochastic disturbance intensity is large enough, for example, they are both greater than the population recruitment rate Λ, the population of at least one compartment will become extinct.
3) Compared to the corresponding deterministic model in [11], which showed that both the two disease-free equilibrium and endemic equilibrium point are not only locally asymptotically stable but also global asymptotically stable provided that the parameters in the model satisfied some quantitative relationships, the stochastic model no longer has stability, we can only discuss rather weaker properties, such as permanence and boundedness. This also shows the destructive impact from stochastic disturbance on the properties of the system.
In this paper, although we prove the existence and uniqueness, ultimate boundedness and stochastic persistence of the positive solution to the established stochastic model, there are still some more detailed and interesting problems that have not been solved. We will discuss them here in order to stimulate readers' interest, or we will continue to study them in the near future.
In the process of proof, we find that the system satisfies stochastic permanence only when the random disturbance intensity of the system is small enough, in other words, when the random disturbance intensity is large enough, the system will go to extinct. A very important and interesting question is how to control the random disturbance intensity or clarify the relationship between disturbance intensity and system parameters to make the populations in the two disease compartment be extinct while other compartments be stochastic permanent? If this problem can be solved, it will provide a valuable control strategy for effectively controlling infectious diseases in the model.
On the other hand, we also noticed a very interesting phenomenon that individuals will acquire knowledge about this disease when a disease spreads within a community, these knowledge or cognition will form memory and have a subtle impact on people's behavior. Therefore, it will be interesting to study the memory effect on the dynamics of our model by using the new generalized fractional derivative method that we can refer to the document [29], where the author put forward a novel definition of fractional derivative taking non-singular kernel in the sense of Caputo. The new generalized fractional derivative method is recently rather popular, we can also refer to the publications [30,31,32], using the methods and skills in them, we are sure to depict the memory effect in our model.
We would like to thank the funding support from the Natural Science Foundation of Gansu Province, China (No.21JR7RA217, No.20JR5RA460), and National Natural Science Foundation of China (No. 1216053). Besides, we are also very grateful to the two anonymous reviewers since their professional opinions help us improve the quality of the manuscript.
We declare that there is no conflict of interest.
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