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Two-Species Competition with High Dispersal: The Winning Strategy

  • This paper is motivated by the following simple question: how does diffusion affect the competition outcomes of two competing species that are identical in all respects other than their strategies on how they spatially distribute their birth rates. This may provide us with insights into how species learn to compete in a relatively stable setting, which in turn may point out species evolution directions. To this end, we formulate some extremely simple two- species competition models that have either continuous or discrete diffusion mechanisms. Our analytical work on these models collectively and strongly suggests the following in a fast diffusion environment: where different species have the same birth rates on average, those that do well are those that have greater spatial variation in their birth rates. We hypothesize that this may be a possible explanation for the evolution of grouping behavior in many species. Our findings are confirmed by extensive numerical simulation work on the models.

    Citation: S.A. Gourley, Yang Kuang. Two-Species Competition with High Dispersal: The Winning Strategy[J]. Mathematical Biosciences and Engineering, 2005, 2(2): 345-362. doi: 10.3934/mbe.2005.2.345

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  • This paper is motivated by the following simple question: how does diffusion affect the competition outcomes of two competing species that are identical in all respects other than their strategies on how they spatially distribute their birth rates. This may provide us with insights into how species learn to compete in a relatively stable setting, which in turn may point out species evolution directions. To this end, we formulate some extremely simple two- species competition models that have either continuous or discrete diffusion mechanisms. Our analytical work on these models collectively and strongly suggests the following in a fast diffusion environment: where different species have the same birth rates on average, those that do well are those that have greater spatial variation in their birth rates. We hypothesize that this may be a possible explanation for the evolution of grouping behavior in many species. Our findings are confirmed by extensive numerical simulation work on the models.


    COVID-19 is an emerging acute infectious disease, which incubation period is 1–14 days, usually 3–7 days. COVID-19 generally have no obvious precursors, the infection will be after the Coronavirus disease early, some patients may also have no obvious symptoms, most common in patients with fever, dry cough, lack of power as the main performance, but beyond that, due to individual differences, the patient also can appear muscle pain, chest tightness, pharyngeal itching, runny nose. The lack of specificity, which can be seen in many diseases and is not unique to COVID-19, makes it difficult for patients to identify infection by symptoms themselves. Some immunity can be acquired after infection or after the cornavirus vaccine, but the duration is unclear.

    The establishing and analyzing of mathematical models play an important role in the control and prevention for disease transmissing. McKendrick first proposed the PDE formulation for the age distribution of a population [1]. Ever since the research results by Kermack and McKendrick [2], Hoppensteadt [3], Iannalli [4] and Webb [5], age structure models have been widely used in the study of transmission dynamics of infectious diseases [6,7,8]. Recently, Bentout Soufiane et al. considered an alcoholism model for age structure and investigated the glabal behavior [9]. In December 2019, some medical institutions of Wuhan reported some cases of pneumonia of unknown cause. On 11 February 2020, the World Health Organization officially named the pneumonia contracted by the Novel Coronavirus as "COVID-19". Recently many scholars have studied on COVID-19, which all proposed and studied the dynamical model which has helped to control infectious diseases. Glenn Webb proposed a model of a COVID-19 epidemic which is developed to predict the effectiveness of vaccination [10]. B. Tang et al. proposed calculation of the basic reproduction number by virtue of mathematical modeling can help decide the potential and severity of an outbreak and provide critical information for identifying the type of disease interventions and intensity [11]. J. Jiao et al. presents an SEIR epidemic model with infectivity in incubation period and homestead-isolation on the susceptible [12]. Besides, deep learning frameworks [13] also can be used for prediction virus spread and a more reliable model incorporating more parameters input into a neural network based virus transmission predictor may be implemented.

    McCluskey assumed that infected individuals can develop disease by either of two pathogenic machanism: fast progression or endogenous reactivation [14]. Generally, acute infectious diseases develop through four stages, among which the incubation period is very important, which refers to the period from pathogen invasion to the onset of clinical symptoms. Take COVID-19 for example which has a certain incubation period. According to current epidemiological statistics, the incubation period is about 1–14 days. Some patients will show symptoms on the day of infection or one or two days later, while some patients will have a longer incubation period of about two weeks. Consequently, it is necessary to consider the factors of fast and slow progress in infection modeling.

    Besides, the treatment of disease is proportional due to medical resources. Capasso and Serill [15] introducing saturated incidence in the cholera epidemic model, describes the tingible into infected class average relationship g(I)=kI/(1+μ),k,μ>0, which said the disease infection ability, said a crowded or change on the influence of the individual, the increase in the number of infected people, easy to dye more vigilant, lead to easy dyeing behaviour change or when the disease is especially crowded in the environment may be unlimited effective contact.

    Zunyou Wu who is the chief expert of epidemiology at the Chinese Center for Disease Control and Prevention, said there are three possible cases of re-positive symptoms for COVID-19: first, false negative or false positive nucleic acid test; second, the virus is active again; third, reinfection. Zijian Feng who is the deputy director of the Chinese Center for Disease Control and Prevention, said that the re-positive case caused continued transmission is rare and does not play a big role. Recently, some provinces in China have seen new cases of COVID-19 including asymptomatic patients. Therefore an infected individual ows into the exposed class after been treated but not becomes susceptible in our models. Inspired by the above discussions, we consider an SEI epidemic model which introduce the latent age, the nonlinear incidence of reactive unsaturated treatment and the saturation treatment function.

    {dS(t)dt=ΛβSIμS,e(t,a)dt+e(t,a)da=(μ+α(a))e(t,a),dI(t)dt=0α(a)e(t,a)da+(1p)βSIf(I)(d+μ)I, (2.1)

    for boundary and initial values conditions

    e(t,0)=pβSI+f(I),S(0)=S0,e(0,a)=e0(a),I(0)=I0. (2.2)

    where S(t),e(t,a) and I(t) respectively be the population sizes of susceptible, latent and infective classes. We assume that the population size is changeless. β represents susceptible people in contact with an infected person transmit rate, p represents susceptible people contact with an infected person enter slow propagation process called latent stage which denoted by e(t, a) where individuals are infected with disease but are not yet contagious, where a is called the age of latency progression, which is the duration of the incubation period. We denote E(t)=+0e(t,a)da as the latent individuals' total density. 1p represents susceptible people and the onset of contact after rapid development for the onset of ratio, μ and d represent people natural mortality and mortality due to illness. f(x)=γx/(1+mx) represents the saturation treatment function where the γ is cure rate of the disease.

    We define X=R+×L1+(0,+)×R+, equipped with the norm (x1,x2,x3)X=|x1|+0x2(a)da+|x3|. The initial condition of system (2.1) belongs to the positive cone of X, then can be rewritten as x0=(S0,e0(),I0)X. We can get a continuous semi-flow associated with system (2.1), that is, Θ:R+×XX produced be system (2.1) adopts the following form, Θ(t,x0)=(S(t),e(t,),I(t)),t0,x0X, with

    Θ(t,x0)X=|(S(t)|++0|e(t,)|da+|I(t)|. (2.3)

    For simplicity, let ε(s)=u+α(s),θ=0α(a)ea0ε(τ)dτda,K0(a)=ea0ε(τ)dτ. The second equation of system (2.1) is solved along ta=constant

    e(t,a)={(pβS(ta)I(ta)+γI(ta)1+mI(ta))K0(a),t>a0,e0(at)K0(a)K0(at),at0, (2.4)

    Let Ω={(S(t),e(t,),I(t))X, S(t)++0e(t,a)da+I(t)Λμ}. The interior of Ω is ˚Ω. we can easily verify the non-negative and positive invariance set of the system (2.1) with the help of article [5].

    We note that if R0>1, Ω is the positive invariant set for Θ, and it attracts all solutions of the system (2.1) with non-negative initial conditions.

    Firstly, there is a disease-free equilibrium point E0=(S0,0,0) in the system (2.1), where S0=Λμ, and we define the basic reproduction number of the system (2.1) as following

    R0=pβΛθ+γμθ+(1p)βΛ(γ+d+μ)μ

    and it is easily known that if R0>1, system (2.1) has an only positive endemic equilibrium point E(S,e(a),I), where

    S=ΛβI+μ,e(a)=(pβSI+γI1+mI)ea0ε(τ)dτ.

    Define space

    X:=R3×L1((0,+),R),X0:=R2×0×L1((0,+),R),X+:=R3+×L1+((0,+),R),

    and X0+=X+X0. Define operator T:D(T)XX,

    T(SI(0e))=(μ(d+μ)(e(0)e(μ+α(a))e))

    where D(T)=R×R×0×W1,1((0,+),R). Consider nonlinear mapping F:X0X, for

    F(SI(0e))=(ΛβSI0α(a)e(t,a)da+(1p)βSIf(I)(pβSI+f(I)0L1))

    define

    U(t)=(S(t),I(t),(0e(t,)))T

    Therefore systerm (2.1) can be rewritten as an abstract Canchy problem

    dU(t)dt=TU(t)+F(U(t))t0,U(0)=u0X0+. (2.5)

    Draw on the results in Magal [16] and Magal and Thiemel [17], there exists an uniquely deterministic semiflow {U(t)}t0 on X0+ which is bound dissipative and asymptotically smooth, and {U(t)}t0 has a global attractor TX which attracts the bounded sets of X.

    Theorem 2.1. If R01, the disease-free equilibrium E0 is locally asymptotically stable.

    Proof. Let x1(t)=S(t)S0, x2(t)=e(t,a), x3(t)=I(t), linearizing the system (2.1) at E0, and considering the exponential solution x1(t)=x01eλt,x2(t,a)=x02eλt,x3(t)=x03eλt, we can derive

    {(λ+μ)x01+βS0x03=0,dx02(a)da=(λ+μ+α(a))x02(a),x02(0)=pβS0x03+γx03,λx03=0α(a)x02(a)da+(1p)βS0x03(μ+d+γ)x03. (2.6)

    Integrating the second equation of system (2.6) from 0 to a, considering the boundary condition, deduces x02(a)=(pβS0x03+γx03)e(λ+μ)aa0α(s)ds. Substituting x02(a) into the fourth equation of system (2.6), solving it, we get the characteristic equation

    H(λ)=λ+0α(a)(γ+pβΛμ)e(μ+λ)aea0α(τ)dτda+(1p)βΛμ(d+μ+γ).

    easily know H(λ)<0 which implies that H(λ) is a decreasing function, and

    limλ+H(λ)=,limλH(λ)=+,H(0)=(d+μ+γ)(R01).

    Let λ=x+yi is an arbitrary complex root of H(λ)=0, then

    H(x+yi)=x+0α(a)(γ+pβΛμ)e(μ+x)aea0α(τ)dτcos(ya)da+(1p)βΛμ(d+μ+γ)(iy+0α(a)(γ+pβΛμ)e(μ+x)aea0α(τ)dτisin(ya)da)=0.

    be equivalent to

    x+0α(a)(γ+pβΛμ)e(μ+x)aea0α(τ)dτcos(ya)da+(1p)βΛμ(d+μ+γ)=0,y+0α(a)(γ+pβΛμ)e(μ+x)aea0α(τ)dτsin(ya)da=0.

    And because 0=x+0α(a)(γ+pβΛμ)e(μ+x)aea0α(τ)dτcos(ya)da+(1p)βΛμ(d+μ+γ)H(x) then 0=H(λ)H(x) which stands for x<λ, where λ is the unique real root of H(λ)=0. Thus if and only if R01, all the roots of system (2.6) have negative real part.

    Theorem 2.2. If R0>1, the unique endemic equilibrium E is locally asymptotically stable.

    Proof. The perturbation variables are as follows

    y1(t)=S(t)S,y2(t,a)=e(t,a)e(a),y3(t)=I(t)I.

    Linearizing system (2.1) at E and assuming the form of solution is as follows

    y1(t)=y01eλt,y2(t,a)=y02(a)eλt,y3(t)=y03eλt, (2.7)

    where y01,y02(a),y03 will be determined. we get

    {0=(λ+βI+μ)y01+βSy03,dy02(a)da=(λ+μ+α(a))y02(a),y02(0)=pβy01I+pβy03S+γ(1+mI)2y03,λy03=0α(a)y02(a)da+(1p)β(y01I+y03S)γ(1+mI)2y03(d+μ)y03. (2.8)

    By calculating, we can get the following eqution

    [λ+γ(1+mI)2+(d+μ)(1p)βS]y03(1p)βIy01=pβIy01W(λ)+(pβS+γ(1+mI)2)y03W(λ), (2.9)

    where W(λ)=0α(a)e(λ+μ)a0α(τ)dτda satisfies the following properties

    W(0)=θ,limλW(λ)=+,limλ+W(λ)=0α(a)da.

    From the first equation of system (2.8) and the Eq (2.9), we obtain the following characteristic equation

    (λ+μ+βI)(λ+μ+d)=(λ+μ+βI){(W(λ)1)γ(1+mI)2+[(1p)β+pβW(λ)]ΛβI+μ}βΛβI+μ[(p1)βIpβIW(λ)] (2.10)

    Note M is the right side of the Eq (2.10). Assuming λ>0, M satisfies the following inequality

    M∣≤R0(λ+βI+μ+1)(γ+d+μ). (2.11)

    which is equivalent to

    h(λ)=λ2+Pλ+Q0.

    where

    P=βI+2μ+dR0(γ+d+μ),Q=(βI+μ)(d+μ)R0(βI+μ+1)(γ+d+μ).

    Since λ>0, therefore

    (βI+μ)(d+μ)(βI+μ+1)(γ+d+μ)>R0.

    Let A=(βI+μ)(d+μ)(βI+μ+1)(γ+d+μ), easily know A<1, i.e. R0<1 which is contradict with R0>1. then we can get λ<0.

    Theorem 2.3. If R0>1, there exists ε>0, such that for each yM0, limt+infd(U(t)y,M0)ε.Furthermore, there exists a compact subset H0M0 which is a global attractor for {U(t)}t0 in M0.

    Proof. Define M0={(S,I,0,e)TX0+:T(t)=I+0e(a)da>0}, and M0=X0+M0. Firstly, let (S0,I0,0,e0)M0, we can get T(t)max{d+μ,μ+αmax}T(t), where αmax=esssupa(0,)α(a), easily know U(t)M0M0. Secondly, if (S0,I0,0,e0)M0, with the help of system (2.4), we know if t0, we get I(t)=0 and 0e(t,a)da0, for t+. Therefore U(t)M0M0. Let (S0,I0,0,e0)M0, we get

    {dI(t)dt=0α(a)e(t,a)da+(1p)βSIf(I)(d+μ)I,e(t,a)dt+e(t,a)da=(μ+α(a))e(t,a),e(t,0)=pβSI+f(I),I(0)=I0,e(0,a)=e0(a)

    Since S(t)S0 as t+, we get I(t)˜I(t),e(t,a)˜e(t,a), where

    {d˜I(t)dt=0α(a)˜e(t,a)da+(1p)βS0˜Iγ˜I(d+μ)˜I,˜e(t,a)dt+˜e(t,a)da=(μ+α(a))˜e(t,a),˜e(t,0)=pβS0˜I+γ˜I,˜I(0)=˜I0,˜e(0,a)=˜e0(a) (2.12)

    By the system (2.4), we have

    ˜e(t,a)={(pβS0˜I(ta)+γ˜I(ta))K0(a),t>a0,˜e0(at)K0(a)K0(at),at0, (2.13)

    where K0(a)=ea0ε(τ)dτ. Substituting system (2.13) into system (2.12), we obtain

    {d˜I(t)dt=T1+T2+(1p)βS0˜Iγ˜I(d+μ)˜I˜I(0)=0 (2.14)

    where

    T1=t0α(a)(pβS0˜I(ta)+γ˜I(ta))K0(a)da,T2=+tα(a)˜e0(at)K0(a)K0(at)da.

    It's simple to know that if T2=0, we get that system (2.14) has an only solution ˜I(t)=0. From the system (2.13), we can get ˜e(t,0)=0,t+. Through comparison, we get (I(t),e(t,a))(0,0) for t+.

    Since E0=(S0,0,0,0L1) is globally asymptotically stable in M0, next we only need to proof that Ws(E0)M0=Θ, where Ws(E0)={zX0+,limt+U(t)z=E0}. Assume there exists zWs(E0)M0, it follows that there exists t0>0 such that I(t0)+0e(t0,a)da>0. Using the method in [18], we have e(t,a)>0 for (t,a)[0,)×[0,), I(t)>0 for t0. By means of the method of Braueretal [19], the following function is defined

    H(a)=aα(s)esaε(τ)dτds

    for a>0, H(a)0, and H(0)=θ. Furthermore, for a0,H(a)=α(a)+ε(a)H(a). Let

    Φ(t)=I(t)+0H(a)e(t,a)da

    which satisfies

    dΦ(t)dt=I(d+μ)1+mI((θp+1p)βS(1+mI)+(θ1)γ(d+μ)1).

    If R0>1, there exists t0>0 such that Φ(t)Φ(t0) for all tt0. Since Φ(t0)>0, this prevents that (I(t),e(t,a))(0,0L1,0L1), which is contradiction with S(t) converges to S0 and I(t) converges to 0, for t. We get the semiflow {U(t)}t0 is uniformly persistent with respect to the pair (M0,M0). Besides, there exists a compact subset H0M0 which is a global attractor for {U(t)}t0 in M0.

    Theorem 2.4. Assume α(a) is an bounded function, if R0<1, the infection-free equilibrium E0 is globally asymptotically stable. Note ˉα=lima[0,+)supα(a).

    Proof. Consider systems (2.1)(2.4) we get

    0α(a)e(t,a)dat0α(a)[pβS(ta)I(ta)+γI(ta)]K0(a)da+ˉαeL1eμt (2.15)

    where eL1=+0e0(a)da. Take the limit of both sides of the inequality (Eq 2.15), since SΛμ and limt+eμt=0, we get

    limt+sup0α(a)e(t,a)da+0α(a)pβΛμK0(a)dalimt+supI(t)+0γα(a)K0(a)dalimt+supI(t). (2.16)

    With the help of Taylor's formula and the third equation of system (2.1), we get

    dI(t)dt0α(a)e(t,a)da+(1p)βIΛμ(γ+d+μ)I. (2.17)

    By solving inequality (Eq 2.17) and taking the limit of both sides, we can get

    limt+supI(t)R0limt+supI(t)

    Therefore, when R0<1, limt+supI(t)=0. By using inequality (Eq 2.16) and system (2.1) respectively, we get limt+supe(t,a)=0 and limt+supS(t)=Λμ. Therefore, if R0<1, the disease-free equilibrium point E0 is global attraction. Further, with the help of Theorem 2.1, we have the disease-free equilibrium point is global asymptotically stable.

    Theorem 2.5. If R0>1, the unique endemic equilibrium E is globally asymptotically stable.

    Proof. The Lyapunov functional V(t) is constructed

    V(t)=WS+We+WI, (2.18)

    where

    WS(t)=(1p)Sg(SS),We(t)=0W(a)e(a)g(e(t,a)e(a))da,WI(t)=Ig(II).

    for W(a)=+aα(s)esa(μ+α(τ))dτ,g(x)=1+xlnx, de(a)da=ε(a)e(a). Calculating the derivative of the V(t) along with the solutions of system (2.18), yields

    dV(t)dt=(1p)μS(2SSSS)+(1p)βSI(1SSSISI+II)W(a)e(a)g(e(t,a)e(a))|+θe(0)g(e(t,0)e(0))0α(a)e(a)g(e(t,a)e(a))+0α(a)e(a)(1IIIe(t,a)Ie(a)+e(t,a)e(a))da+(1p)βSI(1SS+SISIII)=(1p)μS(2SSSS)+(1p)βSI(2SSSS)W(a)e(a)g(e(t,a)e(a))|+0α(a)e(a)(1IIIe(t,a)Ie(a)+e(t,a)e(a)+1e(t,a)e(a)+lne(t,a)e(a))da+θe(0)g(e(t,0)e(0))=(1p)μS(2SSSS)+(1p)βSI(2SSSS)W(a)e(a)g(e(t,a)e(a))|0α(a)e(a)(g(II)+g(Ie(t,a)Ie(a))da+θe(0)g(e(t,0)e(0))

    if II>1 and SS>1, or 0<II<1 and 0<SS<1, we have

    θe(0)g(e(t,0)e(0))=0α(a)e(a)g(e(t,0)e(0))0α(a)e(a)g(II)da

    Hence,

    dV(t)dt==(1p)μS(2SSSS)+(1p)βSI(2SSSS)W(a)e(a)g(e(t,a)e(a))|0α(a)e(a)(g(II)+g(Ie(t,a)Ie(a))da+0α(a)e(a)g(II)da=(1p)μS(2SSSS)+(1p)βSI(2SSSS)W(a)e(a)g(e(t,a)e(a))|0α(a)e(a)g(Ie(t,a)Ie(a))da

    For g(x)0,xR, therefore dV(t)dt0 is always true, furthermore the strict equality holds if and only if S=S,e(t,a)=e(a),I=I. Therefore when R0>1 the endemic equilibrium E is globally asymptotically stable.

    In the work, an age structure epidemic SEI model with fast and slow progression is considered. The basic reproduction number R0 is obtained as R0=pβΛθ+γμθ+(1p)βΛ(γ+d+μ)μ. We have proved the globally asymptotically stable for disease-free and endemic equilibrium respectively. In the following, we also give some numerical simulations to illustrate the global stability. Let Λ=1;β=0.055;γ=0.7;μ=0.063;d=0.04;p=0.8;m=0.02;S(0)=30,e(0,a)=6e0.4a,I(0)=10. and

    α(a)={0.4,aτ0,τa0.

    In Figure 1, we choose τ=12, then R0<1, it can be seen that E0 is globally asymptotically stable. While in Figure 2, we choose τ=1, then R0>1, it can be seen that E is globally asymptotically stable. The figures show the series of S(t) and I(t) which converge to their equilibrium values, in addition the age distribution of e(t,a).

    Figure 1.  The time series of S(t) and I(t), and the age distributions of e(t,a) when τ=12.
    Figure 2.  The time series of S(t) and I(t), and the age distributions of e(t,a) when τ=1.

    COVID-19 has spread rapidly around the world since 2020 with a high fatality rate. Today the epidemic in some countries is still unable to be effectively controlled, and social and economic life has been greatly disrupted. COVID-19 trend prediction has become a major research focus. Current trend prediction methods include epidemic disease prediction model, COVID-19 trend prediction model based on deep learning, etc. These models have effectively assisted medical experts and scientific research institutions to efficiently predict COVID-19. The countermeasures and suggestions for strengthening epidemic prevention and control are put forward, which have a good guiding role for accurate epidemic prevention and control.

    The large-scale epidemic of COVID-19 in China has basically ended, but there are still occasional imported cases or local outbreaks caused by cold chain pollution which prevention and control enters a new phase of normalization. Since the outbreak of COVID-19, a large number of researchers have conducted extensive studies on infectious disease dynamics and prevention and control measures through various models and data analysis methods. Many scholars have built traditional dynamics models based on warehouses to explore the development trend of COVID-19 and provide scientific basis for epidemic prevention and control.

    According to transmission characteristics of infectious diseases, the paper proposed the methods of fast and slow transmission, which more effectively reveals the transmission mechanism for infectious diseases. The global asymptotic stability of the system has analyzed with the help of the principle of dynamics, and abtained the threshold of infectious disease control. The greater the rate of slow progression of an infectious disease, the fewer the threshold results. The world is now being vaccinated which cannot provide lifelong immunity, but can reduce the mortality of those infected. By vaccinating, the rate of patients entering slow progression increases and the threshold is correspondingly reduced. Therefore, vaccination can effectively control the transmission of Coronavirus.

    This research is supported by Guizhou Province Science and Technology Support Plan Project ([2020]4Y167), the National Natural Science Foundation of China (N0.12001417), Doctoral Foundation of Guizhou Education University (2018BS001), First-class University Construction Project of Guizhou Education University ([2019]35).

    The authors declare there is no conflict of interest.

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