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Threshold dynamics of stochastic models with time delays: A case study for Yunnan, China

  • Received: 01 February 2020 Revised: 01 July 2020 Published: 24 August 2020
  • 34F05, 60H10, 92B05

  • In this paper, we provide an effective method for estimating the thresholds of the stochastic models with time delays by using of the nonnegative semimartingale convergence theorem. Firstly, we establish the stochastic delay differential equation models for two diseases, and obtain two thresholds of two diseases and the sufficient conditions for the persistence and extinction of two diseases. Then, numerical simulations for co-infection of HIV/AIDS and Gonorrhea in Yunnan Province, China, are carried out. Finally, we discuss some biological implications and focus on the impact of some key model parameters. One of the most interesting findings is that the stochastic fluctuation and time delays introduced into the deterministic models can suppress the outbreak of the diseases, which can provide some useful control strategies to regulate the dynamics of the diseases, and the numerical simulations verify this phenomenon.

    Citation: Zhimin Li, Tailei Zhang, Xiuqing Li. Threshold dynamics of stochastic models with time delays: A case study for Yunnan, China[J]. Electronic Research Archive, 2021, 29(1): 1661-1679. doi: 10.3934/era.2020085

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  • In this paper, we provide an effective method for estimating the thresholds of the stochastic models with time delays by using of the nonnegative semimartingale convergence theorem. Firstly, we establish the stochastic delay differential equation models for two diseases, and obtain two thresholds of two diseases and the sufficient conditions for the persistence and extinction of two diseases. Then, numerical simulations for co-infection of HIV/AIDS and Gonorrhea in Yunnan Province, China, are carried out. Finally, we discuss some biological implications and focus on the impact of some key model parameters. One of the most interesting findings is that the stochastic fluctuation and time delays introduced into the deterministic models can suppress the outbreak of the diseases, which can provide some useful control strategies to regulate the dynamics of the diseases, and the numerical simulations verify this phenomenon.



    At present, in order to better study the transmission mechanism of infectious diseases, many researchers introduced noises into the deterministic models and studied the effect of noise on the dynamics of the established stochastic epidemic models. Stochastic models could be a more appropriate way of modeling epidemics in many circumstances [11,24]. In particular, Liu et al. [11] established a deterministic model with non-linear incidence rate, and studied the global stability of the model by the basic reproduction number of the model. Then, based on the deterministic model, the stochastic model is established, the dynamics of the stochastic model is proved theoretically, and the properties of these two models are compared. The paper [24] shows that the stochastic models are able to consider randomness of infectious contacts occurring in the latent or infectious periods. The combination of stochastic model and deterministic counterpart can make people understand the epidemic trend of infectious diseases more comprehensively, and make the established theory and prevention strategy more reliable. Many realistic stochastic epidemic models can be derived based on their corresponding deterministic counterparts. Britton [3] gave an excellent survey on stochastic differential equation (SDE) epidemic models which presented the exact and asymptotic properties of a simple stochastic epidemic model, and illustrated by studying effects of vaccination and inference procedures for important parameters such as the basic reproduction number and the critical vaccination coverage. Allen [1] provided a great introduction to the methods of derivation for various types of stochastic models including SDE epidemic models. There are different possible approaches including random effects in the models, both from biological and mathematical perspective [9]. The general stochastic differential equation SIRS model introduced in this paper adopts the modeling approach from Mao et al. [13], which has been pursued in [11,24], and assume that the parameters involved in the model always fluctuate around some average value due to continuous fluctuation in the environment.

    On the other hand, the spread of infectious diseases is not only related to the current state, but also to the historical state (see [25,23]). Therefore, it is more practical to use stochastic differential equation model with time delay to describe the spread of infectious diseases. Recently, many scholars have studied the stochastic infectious disease model with time delay. In particular, Liu et al. [10] proposed and studied the stochastic SEIR epidemic model with infinite distribution delay, and obtained the sufficient conditions for the global asymptotic stability of the endemic equilibrium. Another part of the work is to introduce the disturbance of some parameter variables in the system, which can make the system have a disease-free equilibrium point and give the stability conditions of the disease-free equilibrium point. However, when the parameters of the delay infectious disease model are disturbed randomly, the stochastic model generally does not have disease-free equilibrium and endemic equilibrium. Tornatore et al. [19] proposed a stochastic model with latency and time delay for mosquito transmission, and proposed a strategy for controlling disease transmission. After that, Fan et al. [5] considered the persistence and extinction of a class of stochastic SIR epidemic model with generalized nonlinear incidence and transient immunity and time delay, and obtained the threshold of the model. On the basis of [19,5], Berrhazi et al. [2] considered the stochastic SIR epidemic model with Beddington-DeAngelis incidence and delayed immune loss under Lévy noise disturbance, and studied its persistence, extinction and threshold problems. Considering the effect of vaccination and the incubation period of some diseases (such as tuberculosis, AIDS, measles) after infection, Liu et al. [12] discussed the stochastic SVEIR epidemic model with distribution delay. By constructing appropriate stochastic Lyapunov function, the existence, uniqueness and ergodicity of the positive distribution of the system were obtained.

    Motivated by above mentioned papers, we introduce time delays and stochastic into the deterministic differential equations. This paper is organized as follows: In Section 2.1, we give the basic theory and related lemmas. In Section 2.2, we construct a class of stochastic differential equations models with time delays, and give the thresholds and dynamics of the models by using the theorems and lemmas of Section 2.1. In Section 3, we do a case study of the models in Section 2.2. In addition, we carry out some numerical simulations aiming to HIV/AIDS and Gonorrhea transmission in Yunnan by using the models. In Section 4, we summarize the whole paper.

    Firstly, we introduce some lemmas and notations, which will be used in the following parts. Generally speaking, the d-dimensional stochastic differential equation can be expressed as follows:

    dX(t)=f(t,X(t))dt+g(t,X(t))dB(t), (2.1.1)

    where f(t,X(t)) is a function in Rd defined in [t0,+]×Rd and g(t,X(t)) is a d×m matrix, f,g are locally Lipschitz with respect to the second variable. B(t) is an m-dimensional standard Brownian motion defined on the above probability space. The differential operator L of system (2.1.1) is defined by

    L=t+di=1fi(t)xi+12di,j=1[gT(x,t)g(x,t)]ij2xixj. (2.1.2)

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

    LV(x,t)=Vt(x,t)+Vx(x,t)f(x,t)+12trace[gT(x,t)g(x,t)], (2.1.3)

    where Vt(x,t)=Vt,Vx(x,t)=(Vx1,,Vxd),Vxx=(2Vx1xj)d×d. In view of Itô's formula, if x(t)Rd, then dV(x,t)=LV(x,t)dt+Vx(x,t)g(x,t)dB(t).

    Lemma 2.1. [27] Let A(t) and U(t) be two continuous adapted increasing processes on t0 with A(0)=U(0)=0 a.s. Suppose that M(t) is a real-valued continuous local martingale with M(0)=0 a.s. and X(0) a nonnegative F0-measurable random variable with E(X(0))<. Define X(t)=X(0)+A(t)U(t)+M(t) for all t0. If X(t) is nonnegative, then limtA(t)< implies that limtU(t)<,limtX(t)< and <limtM(t)< with probability one.

    Lemma 2.2. [27] Let M(t),t0, be a local martingale vanishing at time 0 and define

    ρM(t):=tod[M,M](s)(1+s)2,t0, (2.1.4)

    where [M,M](t) is Meyers angle bracket process. Then limtM(t)t=0 a.s. provided limtρM(t)< a.s.

    Lemma 2.3. [4] Set fC[[0,]×Ω,(0,)], and x(t)=1tt0x(s)ds. Suppose that there exist positive constants λ0,λ such that

    logf(t)=λtλ0t0f(s)ds+F(t)a.s. (2.1.5)

    for all t0, where FC[[0,]×Ω,(0,)] and limtF(t)t=0a.s. Then

    limtf(t)=λλ0a.s. (2.1.6)

    In real world, a group of people will often be infected with a variety of diseases, especially two of them have the same or similar transmission routes. We discuss a class of models with two infectious diseases as follows.

    In the paper [14], Meng and Zhao formulated a kind of epidemic model with two classes of epidemics as follows

    {dSdt=AdSβ1SI11+a1I1β2SI21+a2I2+r1I1+r2I2,dI1dt=β1SI11+a1I1(d+α1+r1)I1,dI2dt=β2SI21+a2I2(d+α2+r2)I2, (2.2.1)

    where S denotes the number of the population susceptible to the diseases, I1 and I2 are the total population of the infective in terms of two diseases at time t, respectively. The recruitment to the susceptible population is to be considered as a constant A, β1 and β2 are the contact rates, d is natural mortality rate, α1 and α2 are the rates of diseases-related death, r1 and r2 are the treatment cure rates of two diseases, respectively. ai is the parameter that measure the inhibitory effect for Ii. The incidence rate βiSIi1+aiIi(i=1,2) of susceptible individuals through their contacts with infectious. The two thresholds of the model are R1=β1Ad(d+α1+r1) and R2=β2Ad(d+α2+r2), and the four equilibria are E0=(Ad,0,0), E1=(S1,I1,0), E2=(S2,0,I2) and E=(S,I1,I2), respectively. In addition, the dynamic behavior for the model (2.2.1) is described in the following theorem.

    Theorem 2.4. [14] For system (2.2.1), the following conclusions are true.

    (i) If R1<1 and R2<1, then both diseases go extinct and system (2.2.1) has a unique stable diseases-extinction equilibrium E0.

    (ii) If R1>1 and R2<1, then the disease I2 goes extinct and system (2.2.1) has a unique stable equilibrium E1.

    (iii) If R1<1 and R2>1, then the disease I1 goes extinct and system (2.2.1) has a unique stable equilibrium E2.

    (iv) If R1>1 and R2>1, then E is a unique stable equilibrium, which implies both diseases of system (2.2.1) are permanent.

    Next, we study the stochastic model with time delays corresponding to model (2.2.1).

    {dS=[AdSβ1S(tτ1)I11+a1I1β2S(tτ2)I21+a2I2+r1I1+r2I2]dt+σ3SdB3(t),dI1=[β1S(tτ1)I11+a1I1(d+α1+r1)I1]dt+σ1I1dB1(t),dI2=[β2S(tτ2)I21+a2I2(d+α2+r2)I2]dt+σ2I2dB2(t), (2.2.2)

    where Bi(t) represents a standard Brownian motion with Bi(0)=0 and σ2i>0(i=1,2,3) denotes the intensity of the white noise, τi denotes that S has become the susceptible population of Ii before τi. On the basis of model (2.2.2), we define two thresholds: R1=1d+α1+r1(β1Adσ212) and R2=1d+α2+r2(β2Adσ222), respectively.

    Lemma 2.5. For the solution (S(t),I1(t),I2(t)) of model (2.2.2) with any initial value (S(0),I1(0),I1(0))R3+, we have

    limsupt(S(t)+I1(t)+I2(t))<a.s. (2.2.3)

    Moreover,

    limt+1tt0σ1I1(θ)dB1(θ)=0,limt+1tt0σ2I2(θ)dB2(θ)=0,limt+1tt0σ3S(θ)dB3(θ)=0,limt+1tt0σidBi(θ)=0,(i=1,2,3)a.s. (2.2.4)

    Proof. From (2.2.2), we get

    d(S+I1+I2)=[Ad(S+I1+I2)α1I1α2I2]dt+σ3SdB3(t)+σ1I1dB1(t)+σ2I2dB2(t). (2.2.5)

    This equation has the solution

    S(t)+I1(t)+I2(t)=Ad+[(S(0)+I1(0)+I2(0))Ad]edtα1t0ed(ts)I1(s)dsα2t0ed(ts)I2(s)ds+M(t)Ad+[(S(0)+I1(0)+I2(0))Ad]edt+M(t), (2.2.6)

    where

    M(t)=σ3t0ed(ts)S(s)dB3(s)+σ1t0ed(ts)I1(s)dB1(s)+σ2t0ed(ts)I2(s)dB2(s)

    is a continuous local martingale with M(0)=0 a.s. Define

    X(t)=X(0)+A(t)U(t)+M(t), (2.2.7)

    with X(0)=(S(0)+I1(0)+I2(0)),A(t)=Ad(1edt) and U(t)=(S(0)+I1(0)+I2(0))(1edt) for all t0. Due to the stochastic comparison theorem, S(t)+I1(t)+I2(t)X(t) a.s. It is easy to check that A(t) and U(t) are continuous adapted increasing processes for t0 with A(0)=U(t)=0. By using Lemma 2.1, we have limtX(t)< a.s. This completes the proof of (2.2.3).

    For convenience, we denote

    M1(t)=σ1t0I1(s)dB1(s),M2(t)=σ2t0I2(s)dB2(s),M3(t)=σ3t0S(s)dB3(s),M4(t)=σ1t0dB1(s),M5(t)=σ2t0dB2(s),M6(t)=σ3t0dB3(s). (2.2.8)

    Computing [M1,M1](t)=σ21t0I21(s)ds, by Lemma 2.2 and (2.2.3), we obtain

    limtρ1(t)=limtt0σ21I21(s)ds(1+s)2σ21supt0{I21(t)}<. (2.2.9)

    Then, by Lemma 2.2, limt1tt0σ1I1(s)dB1(s)=0. The left can be proved similarly. This completes the proof.

    Lemma 2.6. For the solution (S(t),I1(t),I2(t)) of model (2.2.2) with any initial value (S(0),I1(0),I1(0))R3+, we have

    limsuptS(t)+I1(t)+I2(t)<Ada.s. (2.2.10)

    Proof. We set

    Ma(t)=t0S(s)dB3(s),Ma(t)=t0ed(ts)S(s)dB3(s),Mb(t)=t0I1(s)dB1(s),Mb(t)=t0ed(ts)I1(s)dB1(s),Mc(t)=t0I2(s)dB2(s),Mc(t)=t0ed(ts)I2(s)dB2(s). (2.2.11)

    By Lemma 2.5, we have

    limt1tMa(t)=0,limt1tMa(t)=0,limt1tMb(t)=0,limt1tMb(t)=0,limt1tMc(t)=0,limt1tMc(t)=0a.s. (2.2.12)

    From (2.2.6), since

    M(t)=σ3tt0s0ed(su)S(u)dB3(u)ds+σ1tt0s0ed(su)I1(u)dB1(u)ds+σ2tt0s0ed(su)I2(u)dB2(u)ds=σ3t(t0S(u)dB3(u)t0ed(tu)S(u)dB3(u))+σ1t(t0I1(u)dB1(u)t0ed(tu)I1(u)dB1(u))+σ2t(t0I2(u)dB2(u)t0ed(tu)I2(u)dB2(u)), (2.2.13)

    by (2.2.12), we obtain limtM(t)=0. From (2.2.6), we get

    limt1tt0[S(0)+I1(0)+I2(0)Ad]edsds=limt1dt{[S(0)+I1(0)+I2(0)Ad](1edt)}=0. (2.2.14)

    By (2.2.6), (2.2.13) and (2.2.14), we obtain

    limsuptS(t)+I1(t)+I2(t)<Ada.s.

    This completes the proof.

    Lemma 2.7. For any given initial value (S(0),I1(0),I1(0))R3+, there exists a unique positive solution (S(t),I1(t),I2(t)) to system (2.2.2) on t0 and the solution will remain in R3+ with probability one, that is to say, (S(t),I1(t),I2(t))R3+ for all t0 almost surely.

    Proof. Since the coefficients of system (2.2.2) are locally Lipschitz continuous, for any given initial value (S(0),I1(0),I1(0))R3+, there exists a unique local solution (S(t),I1(t),I2(t)) on t[0,τe), where τe denotes the explosion time (see [3]). To verify that this solution is global, we only need to prove τe=+ a.s.

    Let k0>0 be enough large such that each component of (S(0),I1(0),I1(0)) is no large than k0. For each integer k>k0, define the stopping time

    τk=inf{t[0,τe):S(t)k,I1(t)k,I2(t)k},

    where throughout this paper we set inf=+. Obviously, τk is increasing as k. Set τ=limkτk, then we can get ττe a.s.

    Define a C2-function V:R3+R+ by

    V(X)=S+I1+I2.

    By Itô's formula, we get

    dV(X)=[AdSdI1dI2α1I1α2I2]dt+σ3SdB3(t)+σ1I1dB1(t)+σ2I2dB2(t)LVdt+σ3SdB3(t)+σ1I1dB1(t)+σ2I2dB2(t),

    where

    LV=AdSdI1dI2α1I1α2I2A.

    For any kk0, there exists T>0 such that τk(0,Tτk]. By the generalized Itô's formula, for any t(0,Tτk], we have

    EV(X(Tτk))=EV(X(S(0),I1(0),I2(0)))+ETτk0LV(X(s))dsEV(X(S(0),I1(0),I2(0)))+AT,

    where E is the expectation of the function. Let k, then t, it follows that limkP(τkT)=0, therefore P(τT)=0. Since T>0 is arbitrary, it results in

    P(τ<)=0,P(τ=)=1.

    This completes the proof.

    Theorem 2.8. Let (S(t),I1(t),I2(t)) be the positive solution of model (2.2.2) with initial value (S(0),I1(0),I2(0))R3+. Then as Ri<1, two infectious diseases of model (2.2.2) go extinct almost surely, i.e. limtIi(t)=0,i=1,2. Moreover, limtS(t)=Ad a.s.

    Proof. Define a function V=lnIi(t). By Itô's formula, we obtain

    dlnIi(t)=(βiS(tτi)1+aiIi(d+αi+ri)12σ2i)dt+σidBi(t). (2.2.15)

    Integrating (2.2.15) from 0 to t gives

    lnIi(t)=βit0S(rτi)1+aiIidr(d+αi+ri)t12σ2it+σiBi(t)σiBi(0)+lnIi(0)βit0S(rτi)dr(d+αi+ri)t12σ2it+σiBi(t)σiBi(0)+lnIi(0)=βit0S(r)dr+βi0τiS(r)drβittτiS(r)dr(d+αi+ri)t12σ2it++σiBi(t)σiBi(0)+lnIi(0)βit0S(r)dr(d+αi+ri)t12σ2it+P(t), (2.2.16)

    where

    P(t)=βi0τiS(r)drβittτiS(r)dr+σiBi(t)σiBi(0)+lnIi(0).

    Dividing both sides of (2.2.16) by t, we have

    lnIi(t)tβiS(d+αi+ri)12σ2i+P(t)t. (2.2.17)

    By integrating the model (2.2.2) and dividing the two sides by t, we conclude that

    {S(t)S(0)t=AdSβ1tt0S(rτ1)I11+a1I1drβ2tt0S(rτ2)I21+a2I2dr+r1I1+r2I2+σ3tt0S(r)dB3(r),Ii(t)Ii(0)t=βitt0S(rτi)Ii1+aiIidr(d+αi+ri)Ii+σitt0Ii(r)dBi(r). (2.2.18)

    Calculating the sum of (2.2.18), we can assert that

    S(t)S(0)t+I1(t)I1(0)t+I2(t)I2(0)t=AdS+r1I1+r2I2(d+α1+r1)I1(d+α2+r2)I2+σ3tt0S(r)dB3(r)+σ1tt0I1(r)dB1(r)+σ2tt0I2(r)dB2(r)AdS(d+α1)I1(d+α2)I2+Wt, (2.2.19)

    where

    Wt=σ3tt0S(r)dB3(r)+σ1tt0I1(r)dB1(r)+σ2tt0I2(r)dB2(r).

    According to (2.2.19), we have

    dS=A(d+α1)I1(d+α2)I2+WtS(t)S(0)tI1(t)I1(0)tI2(t)I2(0)t. (2.2.20)

    Putting (2.2.20) into (2.2.17), we obtain

    lnIi(t)tβi(Ad(d+α1)dI1(d+α2)dI2+WtdS(t)S(0)tdI1(t)I1(0)tdI2(t)I2(0)td)(d+αi+ri)12σ2i+P(t)t. (2.2.21)

    By Lemma 2.5 and Lemma 2.6, we get

    limtlnIi(t)tβiAd(d+αi+ri)12σ2iβi(d+α1)dlimtI1βi(d+α2)dlimtI2βiAd(d+αi+ri)12σ2i. (2.2.22)

    That is, when Ri=1d+αi+ri(βiAdσ2i2)<1, there obviously holds limsuptlnIi(t)t<0, which implies limtIi(t)=0,limtS(t)=Ad=S0. This completes the proof.

    Theorem 2.9. Let (S(t),I1(t),I2(t)) be any positive solution of model (2.2.2) with initial value (S(0),I1(0),I2(0))R3+, then we have the following results.

    (i) If R1>1 and R2<1, then the disease I2 goes extinct and the disease I1 is permanent on average. Moreover, I1 satisfies

    liminftI1(t)=1a1+β1(d+α1)d(d+α1+r1)(R11)>0.

    (ii) If R2>1 and R1<1, then the disease I1 goes extinct and the disease I2 is permanent on average. Moreover, I2 satisfies

    liminftI2(t)=1a2+β2(d+α2)d(d+α2+r2)(R21)>0.

    (iii) If R1>1 and R2>1, then the two infections diseases I1 and I2 are permanent on average. Moreover, I1 and I2 satisfy

    liminfta2I1(t)+a1I2(t)1max{m1,m2}{a2(R11)+a1(R21)}>0,

    where

    m1a1(d+α1)+β1d(d+α1)+a1β2(d+α1)a2d+a1r1,m2a2(d+α2)+β2d(d+α2)+a2β1(d+α2)a1d+a2r2.

    Proof. Firstly, we prove (ⅰ). From model (2.2.2), we obtain

    dS=[AdSβ1S(tτ1)I11+a1I1β2S(tτ2)I21+a2I2+r1I1+r2I2]dt+σ3SdB3(t)=[AdSβ1a1S(tτ1)+1a1β1S(tτ1)1+a1I1β2S(tτ2)I21+a2I2+r1I1+r2I2]dt+σ3SdB3(t). (2.2.23)

    Integrating (2.2.23) and dividing the two sides by t, we may assert that limtI2(t)=0 as R2<1. From Theorem 2.8, we obtain

    S(t)S(0)t=AdS[β1a1tt0S(r)dr+β1a1t0τ1S(r)drβ1a1tttτ1S(r)dr]+1a1tt0β1S(rτ1)1+a1I1dr1tt0β2S(rτ2)I21+a2I2dr+r1I1+r2I2+σ3tt0S(r)dB3(r)=AdSβ1a1tt0S(r)dr+1a1tt0β1S(rτ1)1+a1I1dr+r1I1+r2I21tt0β2S(rτ2)I21+a2I2drβ1a1t0τ1S(r)dr+β1a1tttτ1S(r)drA(d+β1a1)S+1a1tt0β1S(rτ1)1+a1I1dr+r1I1+Qt, (2.2.24)

    where

    Qt=1tt0β2S(rτ2)I21+a2I2drβ1a1t0τ1S(r)dr+β1a1tttτ1S(r)dr.

    By (2.2.24), we deduce

    A(d+β1a1)S+1a1tt0β1S(rτ1)1+a1I1dr+r1I1=S(t)S(0)tQtΦt. (2.2.25)

    From model (2.2.2), we also obtain

    AdS(d+α1)I1(d+α2)I2Θt, (2.2.26)

    where

    Θt=S(t)S(0)+I1(t)I1(0)+I2(t)I2(0)M1(t)M2(t)M3(t)t.

    Define function V=lnI1(t). By using Itô's formula and combining with (2.2.17), we obtain

    lnI1(t)t=1tt0β1S(rτ1)1+a1I1dr(d+α1+r1)12σ21+P(t)t. (2.2.27)

    Putting (2.2.25) and (2.2.26) into (2.2.27), we obtain

    lnI1(t)t=a1[A+(d+β1a1)Sr1I1](d+α1+r1)12σ21+P(t)t+a1Φt=a1A+(a1d+β1)Sa1r1I1(d+α1+r1)12σ21+P(t)t+a1Φt=a1A+(a1d+β1)[Ad(d+α1)dI1(d+α2)dI2Θdt]a1r1I1(d+α1+r1)12σ21+P(t)t+a1Φt=[Aβ1d(d+α1+r1)12σ21][a1d+a1α1+β1(d+α1)d+a1r1]I1(a1d+β1)(d+α2)dI2(a1d+β1)Θdt+P(t)t+a1Φt. (2.2.28)

    According to Lemma 2.3, Lemma 2.5 and Lemma 2.6, when R1>1 and R2<1, we have

    limtI1=λλ0=Aβ1d(d+α1+r1)12σ21a1d+a1α1+β1(d+α1)d+a1r1=1a1+β1(d+α1)d(d+α1+r1)(R11)>0.

    This completes the proof of (ⅰ).

    (ii) The proof of (ⅱ) is similar to that of (ⅰ).

    (iii) From model (2.2.2), we get

    dS=[AdSβ1S(tτ1)I11+a1I1β2S(tτ2)I21+a2I2+r1I1+r2I2]dt+σ3SdB3(t)=[AdSβ1a1S(tτ1)+1a1β1S(tτ1)1+a1I1β2a2S(tτ2)+1a2β2S(tτ2)1+a2I2+r1I1+r2I2]dt+σ3SdB3(t). (2.2.29)

    Similar to (2.2.23)-(2.2.25), integrating (2.2.29) yields

    A(d+β1a1+β2a2)S+1a1tt0β1S(rτ1)1+a1I1dr+1a2tt0β2S(rτ2)1+a2I2dr+r1I1+r2I2=S(t)S(0)tQtΨt. (2.2.30)

    From model (2.2.2), we also get

    AdS(d+α1)I1(d+α2)I2Θt, (2.2.31)

    where

    Θt=S(t)S(0)+I1(t)I1(0)+I2(t)I2(0)M1(t)M2(t)M3(t)t.

    Define the function V=ln(a2I1(t)+a1I2(t)). Similar to (ⅰ), using Itô's formula, we get

    ln(a2I1(t)+a1I2(t))t=a2tt0β1S(rτ1)1+a1I1dr+a1tt0β2S(rτ2)1+a2I2dra2(d+α1+r1)a1(d+α2+r2)12a2σ2112a1σ22+a2M1(t)t+a1M2(t)t. (2.2.32)

    Substituting (2.2.30) and (2.2.31) into (2.2.32), we get

    ln(a2I1(t)+a1I2(t))t=a1a2A+a1a2(d+β1a1+β2a2)Sa1a2r1I1a1a2r2I2+a1a2Ψta2(d+α1+r1)a1(d+α2+r2)12a2σ2112a1σ22+a2M1(t)t+a1M2(t)ta1a2Aa2(d+α1+r1)a1(d+α2+r2)12a2σ2112a1σ22+(a1a2d+a2β1+a1β2)Sa1a2r1I1a1a2r2I2+Υt=a1a2Aa2(d+α1+r1)a1(d+α2+r2)12a2σ2112a1σ22+(a1a2d+a2β1+a1β2)[Ad(d+α1)dI1(d+α2)dI2Θdt]a1a2r1I1a1a2r2I2+Υt=[Ad(a2β1+a1β2)a2(d+α1+r1)a1(d+α2+r2)12a2σ2112a1σ22][(a1a2d+a2β1+a1β2)(d+α1)d+a1a2r1]I1[(a1a2d+a2β1+a1β2)(d+α2)d+a1a2r2]I2(a1a2d+a2β1+a1β2)Θdt+Υt. (2.2.33)

    Then we obtain

    ln(a2I1(t)+a1I2(t))t[Ad(a2β1+a1β2)a2(d+α1+r1)a1(d+α2+r2)12a2σ2112a1σ22]max{m1,m2}[a2I1+a1I2](a1a2d+a2β1+a1β2)Θdt+Υt, (2.2.34)

    where

    m1a1(d+α1)+β1d(d+α1)+a1β2(d+α1)a2d+a1r1,m2a2(d+α2)+β2d(d+α2)+a2β1(d+α2)a1d+a2r2.

    By Lemma 2.3, Lemma 2.5 and Lemma 2.6, we take the limit on both sides of (2.2.34) to get

    liminfta2I1(t)+a1I2(t)λλ0=Ad(a2β1+a1β2)a2(d+α1+r1)a1(d+α2+r2)12a2σ2112a1σ22max{m1,m2}=1max{m1,m2}{a2(R11)+a1(R21)}>0.

    This completes the proof.

    From Theorem 2.8 and Theorem 2.9, we can claim that the thresholds Ri(i=1,2) of the model (2.3.2) can describe the persistence and extinction of two diseases. In other words, if R1<1 and R2<1, then the two infections diseases I1 and I2 of model (2.3.2) go extinct; if R1>1 and R2<1, then the disease I2 goes extinct and the disease I1 is permanent on average; if R2>1 and R1<1, then the disease I1 goes extinct and the disease I2 is permanent on average; if R1>1 and R2>1, then the two infections diseases I1 and I2 are permanent on average.

    In this section, basing on the model (2.2.1) and (2.2.2), we do a case study for HIV/AIDS and Gonorrhea in Yunnan Province, China. The transmission routes of these two kinds of diseases are close to those of the main infected population. The main transmission modes are as follows: sexual transmission, blood transmission, mother to child transmission. According to the report data [26]: The cumulative number HIV positives reported at the end of September 2018 was 850,000, including 260,000 recorded deaths in China, and the estimated number living with HIV/AIDS was 36.9 million around the world. At present, there are many papers about the spread of HIV/AIDS. The basic mathematical models of HIV/AIDS in-host has been developed to describe interactions between immune system and viruses [21]. In [7] and [16], a class of HIV/AIDS model with time delay and a class of HIV/AIDS model with age structure are studied respectively. In [15], a cell-to-cell transmission model of HIV/AIDS is studied. There are few literatures about Gonorrhea, the way of transmission is similar to AIDS, and its harm is not as serious as AIDS. Gonorrhea is a purulent inflammatory disease of genitourinary system caused by Neisseria gonorrhoeae. It is also because the transmission route and AIDS are similar, so it is necessary to study the co-infection model of these two infectious diseases. Yunnan is located in southwest of China, bordering the countries of Myanmar, Laos and Vietnam. According to the sixth national census in 2011 [17], there are 45,596,000 people in Yunnan. From the cumulative number of HIV/AIDS infections in Yunnan Province in 2007 [26], combining with the number of newly increased infections and deaths of HIV/AIDS from 2007 to 2016 [18], the cumulative number of HIV/AIDS infections in Yunnan Province from 2007 to 2016 is obtained (see Table 1). In addition, the number of Gonorrhea infections increased annually from 2007 to 2016 in Yunnan Province [18] is shown in Table 1.

    Table 1.  Cumulative total of reported HIV/AIDS cases and the number of Gonorrhea infections increased annually from 2007 to 2016 in Yunnan Province, China (see [26,18]).
    Year 2007 2008 2009 2010 2011
    HIV/AIDS 57325 64460 71852 78613 85999
    Gonorrhea 2358 2230 1818 1819 1720
    Year 2012 2013 2014 2015 2016
    HIV/AIDS 92666 98555 104903 111351 117817
    Gonorrhea 1893 1643 2104 3028 4098

     | Show Table
    DownLoad: CSV

    Using Eviews 7.0, we will test the stationarity of the data for the number of people infected with HIV/AIDS and Gonorrhea from 2007 to 2016 in Yunnan Province, respectively. The autocorrelation and partial correlation coefficients of the test results show that the data series is stable and the statistics are good. Next, the parameters of the model (2.2.2) are further determined for fitting. The specific idea is that part of the parameters are based on the known literatures and some biological values, and then, based on the data in Table 1 and the parameters obtained, the least square method is used to fit the model to estimate the remaining parameters. For the natural mortality of people in Yunnan Province, we choose d=167=0.0149 where 67 is the average life of people in Yunnan [6]. For HIV/AIDS and Gonorrhea patients' death rate αi(i=1,2) in Yunnan, we know that 1eαit is the death probability of HIV/AIDS and Gonorrhea patients. We can take α1=0.7114 (see [7]) and detailed parameters values are shown in Table 2. We take 2007 as the initial time t=0, according to the cumulative number of HIV/AIDS infections in Yunnan Province in 2007 [26], so we take I1(0)=57325, and the other two initial values S(0) and I2(0) are obtained by estimation, as shown in Table 2. The number of susceptible persons, the population infected with HIV/AIDS and the population infected with Gonorrhea are obtained by numerical fitting using the parameters of Table 2, as shown in Fig. 1, including the comparison of fitting data and statistical data.

    Table 2.  Parameters and numerical values chosen for the simulation.
    Parameters Definition Value Source
    A Recruitment rate for the susceptible population 92136 Estimated
    d Natural mortality rate 0.0149 [6]
    α1 Death rate for HIV/AIDS 0.7114 [26]
    α2 Death rate for Gonorrhea 0.3 Estimated
    r1 Cure rate for HIV/AIDS 0.79 Estimated
    r2 Cure rate for Gonorrhea 0.99994 Estimated
    β1 Infection rate for HIV/AIDS 0.9 Estimated
    β2 Infection rate for Gonorrhea 0.25 Estimated
    a1 Inhibition rate of HIV/AIDS on transmission 0.9 Estimated
    a2 Inhibition rate of Gonorrhea on transmission 1 Estimated
    τ1 Incubation period of AIDS 8 year [26]
    τ2 Incubation period of Gonorrhea 0 [18]
    S(0) Initial value of susceptible population 80000 Estimated
    I1(0) Initial value of HIV/AIDS patients 57325 [26]
    I2(0) Initial value of Gonorrhea patients 12358 Estimated

     | Show Table
    DownLoad: CSV
    Figure 1.  The model (2.2.2) is simulated by the parameters values in Table 2, and compared with the HIV/AIDS and Gonorrhea data in Yunnan Province from 2007 to 2016.

    When the parameters in Table 2 are substituted into the two thresholds of the model (2.2.1), they are both greater than unity, that is, both diseases are persistent. To illustrate the significance of model (2.2.2) in disease control, we first describe the dependence of each parameter in thresholds Ri(i=1,2) of model (2.2.2), namely the partial rank correlation coefficients (PRCCs). As shown in Fig. 2. Considering the objective conditions of medical equipment and human life span, combining with the results of PRCC, we can adopt four ways to control the two diseases: (1) improving the recovery rate of diseases ri; (2) reducing the infections rate of infectious diseases βi; (3) reducing the number of imports to susceptible persons A and (4) using big noises σi(i=1,2).

    Figure 2.  Partial rank correlation coefficients(PRCCs) results for the dependence of Ri on each parameter.

    According to the results of PRCC, we take the following values: A = 400, r1 = 0.75, r2 = 0.2,d = 0.0149, β1 = 0.00007, β2 = 0.00002, α1 = 0.7114, α2 = 0.1, a1 = 0.0001, a2 = 0.0001, σ1 = 0.95, σ2 = 0.9, σ3 = 0.2, τ1=τ2=0.5. It follows that R1=1.2729>1>R1=0.9672,R2=1.7050>1>R2=0.4189. Under these conditions, the two diseases of the deterministic model (2.2.1) will be persistent, whereas the two diseases described by the model (2.2.2) will be extinct (see Fig. 3 and Fig. 4).

    Figure 3.  When R1=1.2729>1>R1=0.9672, model (2.2.1) describes HIV/AIDS infection I1 will be persistent, but stochastic differential equation with time delay model (2.2.2) describes HIV/AIDS infection I1 will be extinct.
    Figure 4.  When R2=1.7050>1>R2=0.4189, model (2.2.1) describes Gonorrhea infection I2 will be persistent, but stochastic differential equation with time delay model (2.2.2) describes Gonorrhea infection I2 will be extinct.

    The fluctuation of natural environment will bring variability to biological system [20]. And environmental changes have a vital impact on the development of epidemics. Variability of temperature and rainfall may cause significant fluctuations in the dynamics of pathogenic fungi [22,8]. In terms of human disease, the nature of epidemic spread and growth is inherently random due to the unpredictability of person-to-person contacts [11,24]. Therefore, the variability and randomness of the environment are introduced into the epidemic model [20]. In general, the threshold of the model is a very important quantity for theoretical analysis of differential equation models describing infectious diseases. That is to say, the relationship between the threshold and 1 is used to analyze whether the disease is extinct or not. Therefore, in this paper, we discuss two classes of differential equations models. Specifically in each class of models, considering the introduction of randomness and time-delays, the change of infection rate, the existence of immunity loss and so on, then we theoretically analyze the thresholds changes in each class. We obtain the sufficient conditions for the extinction and persistence of diseases. In addition, we do a case study of (2.2.1) and (2.2.2), and we also carry out some numerical simulations aiming to HIV/AIDS and Gonorrhea transmission in Yunnan by using the models.

    Through the case study, the results of numerical simulation and theoretical analysis are consistent, i.e., when Ri>1(i=1,2), the diseases will be persistent; when Ri<1(i=1,2), the diseases will be extinct. By comparing the thresholds of model (2.2.1) and model (2.2.2), and combining with the numerical simulations results, its are found that there are always Ri>Ri(i=1,2). Therefore, we are mostly concerned about the situations Ri>1>Ri(i=1,2), which are the significances of stochastic differential equations in controlling infectious diseases. Finally, we discuss some biological implications and focus on the impact of some key model parameters, the strategies of controlling HIV/AIDS and Gonorrhea are given, i.e., controlling the spread of infectious diseases by improving the recovery rate of diseases ri, reducing the infections rate of infectious diseases βi, declining the number of imports to susceptible people A and using big noises σi(i=1,2).

    Another possible and important extension for future work is that there is a class of stochastic model and its corresponding deterministic model, and the threshold of the stochastic model is larger than that of the deterministic model. That is, when the threshold of the stochastic model is greater than 1 and then greater than the threshold of the deterministic model, the disease of the deterministic model will be extinct, but the disease of the stochastic model will be persistent. This is the risk of introducing random noises into the deterministic models for the infectious diseases models, but for the population models, this can maintain the growth of the population, so it is very meaningful to study this problem. All the aforementioned possible extensions are interesting, biologically important but yet mathematically challenging, and we have to leave them for future research projects.

    We are grateful to reviewers for their valuable comments and suggestions, which greatly improved the presentation of this paper.



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