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Research article Special Issues

Improved uniform persistence for partially diffusive models of infectious diseases: cases of avian influenza and Ebola virus disease


  • Received: 31 July 2023 Revised: 22 September 2023 Accepted: 19 October 2023 Published: 26 October 2023
  • Past works on partially diffusive models of diseases typically rely on a strong assumption regarding the initial data of their infection-related compartments in order to demonstrate uniform persistence in the case that the basic reproduction number R0 is above 1. Such a model for avian influenza was proposed, and its uniform persistence was proven for the case R0>1 when all of the infected bird population, recovered bird population and virus concentration in water do not initially vanish. Similarly, a work regarding a model of the Ebola virus disease required that the infected human population does not initially vanish to show an analogous result. We introduce a modification on the standard method of proving uniform persistence, extending both of these results by weakening their respective assumptions to requiring that only one (rather than all) infection-related compartment is initially non-vanishing. That is, we show that, given R0>1, if either the infected bird population or the viral concentration are initially nonzero anywhere in the case of avian influenza, or if any of the infected human population, viral concentration or population of deceased individuals who are under care are initially nonzero anywhere in the case of the Ebola virus disease, then their respective models predict uniform persistence. The difficulty which we overcome here is the lack of diffusion, and hence the inability to apply the minimum principle, in the equations of the avian influenza virus concentration in water and of the population of the individuals deceased due to the Ebola virus disease who are still in the process of caring.

    Citation: Ryan Covington, Samuel Patton, Elliott Walker, Kazuo Yamazaki. Improved uniform persistence for partially diffusive models of infectious diseases: cases of avian influenza and Ebola virus disease[J]. Mathematical Biosciences and Engineering, 2023, 20(11): 19686-19709. doi: 10.3934/mbe.2023872

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  • Past works on partially diffusive models of diseases typically rely on a strong assumption regarding the initial data of their infection-related compartments in order to demonstrate uniform persistence in the case that the basic reproduction number R0 is above 1. Such a model for avian influenza was proposed, and its uniform persistence was proven for the case R0>1 when all of the infected bird population, recovered bird population and virus concentration in water do not initially vanish. Similarly, a work regarding a model of the Ebola virus disease required that the infected human population does not initially vanish to show an analogous result. We introduce a modification on the standard method of proving uniform persistence, extending both of these results by weakening their respective assumptions to requiring that only one (rather than all) infection-related compartment is initially non-vanishing. That is, we show that, given R0>1, if either the infected bird population or the viral concentration are initially nonzero anywhere in the case of avian influenza, or if any of the infected human population, viral concentration or population of deceased individuals who are under care are initially nonzero anywhere in the case of the Ebola virus disease, then their respective models predict uniform persistence. The difficulty which we overcome here is the lack of diffusion, and hence the inability to apply the minimum principle, in the equations of the avian influenza virus concentration in water and of the population of the individuals deceased due to the Ebola virus disease who are still in the process of caring.



    In December 2019, COVID-19 (Corona Virus Disease 2019) named by the World Health Organization was first diagnosed in China. Until now, the COVID-19 in China is basically under control, but there are still many infections around the world. WHO Director-General Tedros Adhanom Ghebreyesus said on March 11, 2020 that COVID-19 has pandemic characteristics. The disease has now spread globally, including cases confirmed in 220 Countries. According to the latest real-time statistics of the WHO, as of November 26, 2020, there have been a total of 60,074,174 confirmed cases of COVID-19, and a total of 1,416,292 deaths [1]. The most infected countries distributed in descending order of infected cases are United States of America, India, Brazil, Russian Federation, France, Spain, The United Kingdom, Italy, etc. To defeat the epidemic, scientists in different fields have contributed to COVID-19 [2,3,4,5,6,7,8,9].

    The disease dynamic models continue to play an important role in predicting the development trend of infectious disease epidemics, scientific prevention and control guidance, and provide important data basis and theoretical support for the decision-making of public health managers and the implementation of efficient intervention measures. The SIR model proposed by Kermack and McKendrick [10] has been widely used to study infectious diseases. Differential equations and dynamical system methods are widely used to study the origin, evolution and spread of various diseases. In particular, the dynamic model has achieved fruitful results in rabies [11,12], malaria [13], cholera [14], brucellosis [15] and HFMD(Hand, foot and mouth disease) [16]. There also has been a large amount of literatures using dynamic models to analyze the spread and outbreak of COVID-19 [2,3,8,17,18,19,20,21,22,23,24]. Jiao et al. [2] studied an SEIR with infectivity in incubation period and homestead-isolation on the susceptible. Their research results indicate that governments should strictly implement the isolation system to make every effort to curb the spread of disease during the epidemic. Li et al. [3] revealed the effects of city lock-down date on the final scale of cases and analyzed the impact of the city lock-down date on the final scale of cases by studied the transmission of COVID-19 in Shanxi Province. He et al. [8] proposed an SEIR model for the COVID-19 which is built according to some related factors, such as hospital, quarantine and external input. The particle swarm optimization (PSO) algorithm is applied to estimate the parameters of the system. They show that, for the given parameters, if there exists seasonality and stochastic infection, the system can generate chaos. Bouchnita [17] et al use a multi-scale model of COVID-19 transmission dynamics to quantify the effects of restricting population movement and wearing face masks on disease spread in Morocco. Bardina [19] and Zhang et al. [20] using a stochastic infectious disease model to study COVID-19. This research has shown that the social blockade is very effective in controlling the spread of disease.

    For COVID-19, there is no specific vaccines or antiviral drugs to treatment the disease and it is hard to control the spread of the disease. The best way to control the spread of COVID-19 is social blockade. However, the social blockade will have a serious impact on economic development and the normal lives of the people. Therefore, in order not to affect the normal life of non-infected persons, we proposed the strategy of isolating infected people to study the spread of the disease. Nowadays, there is a kind of infectious patients who have no symptoms, disseminating the infection disease and causing social panic. In 2013, Ma et al. [16] established an SEIIaHR epidemic model to study the spread of HFMD. The SEIIaHR isolates the infected person for treatment, while considering the role of recessive infection in the spread of HFMD. This is the same as our strategy in studying the spread of COVID-19. Therefore, we use the SEIIaHR model to study the impact of asymptomatic patients on the disease.

    This paper is organized as follows: in the next section, we give the SEIIaHR model and describe the each symbol of the system. In section 3, we study the stability analysis of disease-free equilibrium and the persistence of the endemic equilibrium. Next, we take some numerical simulations for the system of (2.1) in section 4. Finally, we give some conclusions about COVID-19.

    From the above discussions, we consider an SEIIaHR model with asymptomatic infected and quarantined on the symptomatic infected as following system

    {˙S(t)=Λβ1S(t)I(t)β2S(t)Ia(t)dS(t),˙E(t)=β1S(t)I(t)+β2S(t)Ia(t)σE(t)dE(t),˙I(t)=σpE(t)(γ1+k+δ1)I(t)dI(t),˙Ia(t)=σ(1p)E(t)γ3Ia(t)dIa(t),˙H(t)=kI(t)(γ2+δ2)H(t)dH(t),˙R(t)=γ1I(t)+γ2H(t)+γ3Ia(t)dR(t). (2.1)

    Here S(t),E(t),I(t),Ia(t),H(t),R(t) represent the numbers of the susceptible, exposed, symptomatic infected, asymptomatic infected, quarantined, recovered population at time t, respectively. Λ>0 describes the annual birth rate, β1,β2 are infection rates, 1σ represents the mean incubation period; p is the fraction of developing infectious cases, and the remaining fraction 1p return to the recessive class; δ1 and δ2 are the disease-induced mortality for the infective and quarantined individuals, respectively; k is the quarantine rate; infective, quarantined and recessive individuals recover at the rate γ1, γ2 and γ3, respectively; d is the human natural mortality rate.

    Define N(t)=S(t)+E(t)+I(t)+Ia(t)+H(t)+R(t), from system (2.1), we know that

    dNdtΛdN,

    it implies that the solutions of system (2.1) are bounded and the region

    X={(S,E,I,Ia,H,R)R6+:S+E+I+Ia+H+RΛd} (3.1)

    is positively invariant for system (2.1). It is easy to see that system (2.1) has a disease-free equilibrium E0=(Λd,0,0,0,0,0). Using the next generation matrix formulated in Diekmam et al. [25] and van den Driessche and Watmough [26], we define the basic reproduction number by

    R0=β1ΛσpdM1M2+β2Λσ(1p)dM1M3, (3.2)

    here we denote M1=σ+d,M2=γ1+k+δ1+d,M3=γ3+d and M4=γ2+δ2+d. Thus we have the following theorem.

    Theorem 3.1. If R0<1, then the disease-free equilibrium E0=(Λd,0,0,0,0) of the system (2.1) is global asymptotically stable.

    Proof. we prove the global stability of the disease-free equilibrium. Define the Lypunov function as V(E,I,Ia)=β1M1M3I+β2M1M2Ia+(β1σpM3+β2σ(1p)M2)E. For all t>0, the derivative of V(t) is

    dVdt=β1M1M3(σpEM2I)+β2M1M2(σ(1p)EM3Ia)+(β1σpM3+β2σ(1p)M2)(β1SI+β2SIaM1E)=β1σpM3S(β1I+β2Ia)+β2σ(1p)M2S(β1I+β2Ia)M1M2M3(β1I+β2Ia)=M2M3M4(β1I+β2Ia)(β1σpSM1M2+β2σ(1p)SM1M31)M2M3M4(β1I+β2Ia)(R01). (3.3)

    Here the relation SΛd has been utilized. If R0<1, we know that dVdt0, and dVdt=0 holds if and only if S=Λd, I=Ia=H=R=0. Using the LaSalle's extension to Lyapunov's method, the limit set of each solution is contained in the largest invariant set in {(S,E,I,Ia,H,R)X|dVdt=0} is the singleton {E0}. This means that the disease-free equilibrium E0 is globally asymptotically stable in X when R0<1.

    Theorem 3.2. If R0>1, then the disease is uniformly persistent, i.e., there is a constant ε>0 such that every positive solution of system (2.1) satisfies

    limtI(t)ε,  limtIa(t)ε. (3.4)

    Proof. Define

    X={x(t)X:E(t)=0},X0=XX.

    In order to prove that the disease is uniformly persistent, we only need to show that X repels uniformly the solutions of system (2.1) in X0. It is easy to verify that X is relatively closed in X and is point dissipative. Let

    X={x(t):x(t)X,t>0}. (3.5)

    We now show that X={(S1,0,0,0,0,0):0<S1Λd}. Assume that x(t)X for all t0, then we have E(t)=0 for all t0. Thus, by the second equation of system (2.1), we have S(t)[β1I1(t)+β2Ia(t)]=0, which implies that I(t)=0,Ia(t)=0 for all t0. Indeed, if I(t)0,Ia(t)0, there is a t00 such that I(t0)>0,Ia(t)>0, form the second equation of system (2.1), we have

    dEdt|t=t0=β1SI(t0)+β2SIa(t0)>0. (3.6)

    It exists a t1>t0 such that E(t1)>0,dIdt|t1=σpE(t1)>0,dIadt|t1=σ(1p)E(t1)>0, it follows that there is a η>0 such that I(t),Ia(t)>0 for t1<t<t1+η. This means that x(t)X for t1<t<t1+η, which contradicts to the assume x(t)X for all t0. Therefore, X={(S1,0,0,0,0,0):0<S1Λd}.

    By analyzing system (2.1), it is clear that E0 is unique equilibrium in X. Next, we will show that E0 repels the solutions of system (2.1) in X0. We analyze the behavior of any solution x(t) of system (2.1) close to E0. We divide the initial data into two cases.

    ● If E(0)=I(0)=Ia(0)=0, then E(t)=I(t)=Ia(t)=0. System (2.1) implies that S(t) goes away from E0 as t.

    ● If E(0),I(0),Ia(0)>0, then E(t),I(t),Ia(t)0 for all t>0. When x(t) stays close to E0, by the system (2.1) there exists a ρ small enough such that

    {dEdt>˜a11E+˜a12I+˜a13Ia,dIdt=˜a21E+˜a22I,dIadt=˜a31E+˜a33Ia. (3.7)

    where ˜a11=(d+σ)ρ, ˜a12=Λβ1dρ, ˜a13=Λβ2dρ, ˜a21=σp, ˜a22=M2, ˜a31=σ1(1p),˜a33=(d+γ3), and largest eigenvalue of the coefficient matrix ˜A(˜aij) of the right hand of (3.7) is positive, since R0>1 [25]. Hence the solutions of the linear quasi-monotonic system

    {dxdt=˜a11x+˜a12y1+˜a13yadydt=˜a21x+˜a22y1dyadt=˜a31x+˜a33ya,

    with y1(0),ya(0)>0 are increasing as t. By the comparison principle, (E,I1,Ia) goes away from (0,0,0,0,0). Therefore, {E0} is an isolated invariant set and acyclic. Using Theorem 4.3 in Freedman [27], system (2.1) is uniformly persistent. Thus, the proof of Theorem 3.2 is completed.

    Biologically speaking, Theorem 3.2 shows that the disease is uniformly persistent if R0>1, and all the solutions of system are ultimately bounded in X, then system has at least one positive solution By Zhao [28]. Therefore, we have the following theorem.

    Theorem 3.3. If R0>1, then the system (2.1) has an endemic equilibrium E=(S,E,I,Ia,H,R).

    Proof. From the third and forth equations of system (2.1), we can conclude that

    σpE=M2I,σ(1p)E=M3Ia,

    then we have

    I=σpEM2,  Ia=σ(1p)EM3.

    We also obtain

    S=ΛM1Ed,  H=kσpEM2M4,  R=1d(σpγ1M2+σ(1p)γ2M3+kσpγ3M2M4)E,

    where M1,M2,M3 and M4 are mentioned in (3.2). Substituting S, I and Ia in the second equation of (2.1) at steady state, we obtain the following equation

    E=M2M3dβ1M3σp+β2M2σ(1p)(R01). (3.8)

    Here we should show the term S is positive, from the above Eq (3.8), we have S=M1M2M3β1M3σp+β2M2σ(1p)>0. From the similar argument, we have I,Ia,H,R>0, i.e., the system has at most one positive solution. Therefore, if R0>1, the system has an endemic equilibrium.

    Since the first case was reported to WHO on 31st December 2019, the COVID-19 has spread rapidly worldwide. As of December 21, 2020 there are 220 countries were infected, and there are many countries still trap in the epidemic. In this section, we consider the study of spread of COVID-19 disease in India. India is observing an increase in the number of patients each day. The accuracy of our proposed model is validated by using the official data of India from[29,30,31].

    The study consider currently infected patients of India from May 1st 2020 to November 15th 2020. The population of India is around N=1386750000[29], thus we assumed that the initial value is S(0)=NE(0)Ia(0)I(0)H(0)R(0), E(0)=315236, Ia=78809, I(0)=236427, H(0)=7880, R(0)=59646. Then we illustrate the source of parameters in following. We can get the value of population input into the susceptible class through birth 77575 per day in India, and the average life expectancy of India is 70.42. Noting that 1/d is the average life expectancy, the value of parameter d can be calculated as d=1/(70.42×365)=3.8904×105. We choose the 1/σ=2.5 which represent the average period of from the susceptible to the exposed. Because the average recovered period of the quarantined about is 14 days, so we choose the parameter γ2=1/14=0.0714. The parameters of system (2.1) are listed in Table 1.

    Table 1.  Descriptions and values of parameters.
    Para. Value Unit Interpretation Source
    Λ 7.7575×104 day1 population input [29]
    d 3.8905×105 day1 Natural death rate [29]
    σ 0.33 day The average incubation period [30]
    p 0.25 none The fraction of developing infected cases [30]
    k 0.1 day1 The quarantine rate [31]
    γ1 0.3303 day Recovery rate of the infected [32]
    γ2 0.0714 day Recovery rate of the quarantined [33]
    γ3 0.1398 day Recovery rate of the recessive [32]
    δ1 0.0135 day1 The infected disease-related death rate Estimated
    δ2 0.0328 day1 The quarantined disease-related death rate [32]

     | Show Table
    DownLoad: CSV

    We use the Markov Chain Monte Carlo (MCMC) method to fit the parameters β1, β2 to the data, and adopt an adaptive Metropolis-Hastings (M-H) algorithm to carry out the MCMC procedure. The algorithm is run for 10,000 iterations with a burn-in of the first 6,000 iterations, and the Geweke convergence diagnostic method is employed to assess convergence of chains. In Figure 1, we have plotted the curves between the total number of COVID-19 cases versus days (till November 15, 2020) in India based on the actual data and the proposed model (2.1). The estimation results some parameters are given in Table 2 and Figure 2.

    Figure 1.  COVID spread in India and simulated by MCMC(Days from May 1st 2020).
    Table 2.  The values of β1 and β2 given by MCMC.
    Para. Mean Value Range Unit Interpretation Geweke
    β1 1.3958×109 [1.37,1.42]×109 day Infection rate of the Recessive 0.99942
    β2 1.5155×1011 [1.2,2.0]×1011 day Infection rate of the Infectious 0.99284

     | Show Table
    DownLoad: CSV
    Figure 2.  The distribution of β1 and β2 given by MCMC.

    For the quarantine rate k, we have chosen two different values as a comparison to show the importance of quarantine measures for symptomatic infected to control the spread of disease. Figure 3 shows the relationship between quarantine rate k and basic reproduction number R0. We can see that R0 and k are negatively correlated. After calculation, we get the critical point kc=0.4949, then we have R0 is equal to 1. Figure 4 is the evolution of system (2.1) when k=0.8, 0.01, respectively. If k=0.8, we compute the basic reproduction number R0=0.7741<1, it can be seen that the disease-free equilibrium E0 is globally asymptotically stable (see Figure 4a). If k=0.01, we calculate the basic reproduction number R0=2.1321>1, it can be seen that system (2.1) has a positive equilibrium point and it is is uniformly persistent (see Figure 4b).

    Figure 3.  The relationship between quarantine rate k and R0.
    Figure 4.  The evolution of system (2.1).

    Next, the impact of the treatment period(1/γ2) for quarantined on COVID-19 is analyzed. Figures 5 and 6 show the number of infected (I+Ia+H), quarantined (H), and cumulative deaths (COVID-19 deaths, excluding natural deaths) in different treatment period for R0<1 and R0>1 respectively. When R0<1, the shorter the treatment period, the disease will die out faster, and the fewer people will be isolated. At the same time, the cumulative number of deaths will be lower. When R0>1, the longer the treatment period, the more people will be infected and quarantined. Assuming that there are no individual differences, the treatment period is negatively related to the medical level. That is, the higher the medical level, the shorter the treatment period. This means that improving the level of medical treatment is conductive to the control of COVID-19. Therefore, it is urgent for India and other countries to develop specific drugs against COVID-19.

    Figure 5.  The impact of the treatment period for quarantined on COVID-19: k=0.8,R0=0.7741<1.
    Figure 6.  The impact of the treatment period for quarantined on COVID-19: k=0.01,R0=2.1321>1.

    Then, we show the relationship between parameters k,β2 and R0. From Figure 7a, we know that the parameters k and R0 are negatively correlated, and the parameters β2 and R0 are positively correlated. When β2=2.0×1011, the quarantine rate k has the maximum threshold k=0.5411>kc. When β2=0, the quarantine rate k has the minimum threshold k=0.3519<kc. Figure 7b, 7c show the relationship between β2 and R0 when k=0.01,0.8, respectively. When k=0.01, the disease is uniformly persistent, even the the parameter β2=0. If we select k=0.8, only when β2>3.6639×1011 can affect the spread of the disease. Therefore, we deduce that when k>0.5411, asymptomatic infections do not affect the spread of the disease; when 0.3519<k<0.5411, it is related to the infection rate of asymptomatic people whether the disease persists. In general, the higher the quarantine rate of people with symptoms, the easier it is to control the spread of the disease.

    Figure 7.  The relationship between parameters k,β2 and R0.

    In this paper, we consider an SEIIaHR epidemic model with asymptomatic infection and isolation. First, We have proved that the disease-free equilibrium E0 is globally asymptotically stable if and only if R0<1 and the system (2.1) is uniformly persistent if R0>1. Our numerical simulation results are consistent with theoretical analysis. Second, we showed the impact of the treatment period(1/γ2) for quarantined on COVID-19. The better the medical treatment, the COVID-19 is more likely to die out or be controlled at a lower level. Therefore, it is urgent for India and other countries around the world to develop specific drugs against COVID-19. Third, we deduced that the parameters k and R0 are negatively correlated, and the parameters β2 and R0 are positively correlated. At the same time, we found that asymptomatic infections will affect the spread of the disease when the quarantine rate is within the range of [0.3519,0.5411] and isolating people with symptoms is very important to control and eliminate the disease in India and other countries.

    The authors would like to thank the referees for helpful comments which resulted in much improvement of the paper. Project Supported by National Nature Science Foundation of China (Grant No. 12071445, 12001501), Fund for Shanxi 1331KIRT, Shanxi Natural Science Foundation (Grant No. 201901D211216) and the outstanding youth fund of North University of China.

    The authors declare that they have no conflict of interest.



    [1] P. van den Driessche, J. Watmough, Reproduction numbers and sub-threshold endemic equilibria for compartmental models of disease transmission, Math. Biosci., 180 (2002), 29–48. https://doi.org/10.1016/S0025-5564(02)00108-6 doi: 10.1016/S0025-5564(02)00108-6
    [2] H. R. Thieme, Spectral bound and reproduction number for infinite-dimensional population structure and time heterogeneity, SIAM J. Appl. Math., 70 (2009), 188–211. https://doi.org/10.1137/080732870 doi: 10.1137/080732870
    [3] W. Wang, X. Q. Zhao, Basic reproduction numbers for reaction-diffusion epidemic models, SIAM J. Appl. Dyn. Syst., 11 (2012), 1652–1673. https://doi.org/10.1137/120872942 doi: 10.1137/120872942
    [4] K. Yamazaki, Global well-posedness of infectious disease models without life-time immunity: the cases of cholera and avian influenza, Math. Med. Biol., 35 (2018), 427–445. https://doi.org/10.1093/imammb/dqx016 doi: 10.1093/imammb/dqx016
    [5] H. M. Yin, On a reaction-diffusion system modelling infectious diseases without lifetime immunity, Eur. J. Appl. Math., 33 (2021), 803–827. https://doi.org/10.1017/S0956792521000231 doi: 10.1017/S0956792521000231
    [6] W. Wang, X. Q. Zhao, A nonlocal and time-delayed reaction-diffusion model of dengue transmission, SIAM J. Appl. Math., 71 (2011), 147–168. https://doi.org/10.1137/090775890 doi: 10.1137/090775890
    [7] Y. Lou, X. Q. Zhao, A reaction-diffusion malaria model with incubation period in the vector population, J. Math. Biol., 62 (2011), 543–568. https://doi.org/10.1007/s00285-010-0346-8 doi: 10.1007/s00285-010-0346-8
    [8] X. Q. Zhao, Global dynamics of a reaction and diffusion model for Lyme disease, J. Math. Biol., 65 (2012), 787–808. https://doi.org/10.1007/s00285-011-0482-9 doi: 10.1007/s00285-011-0482-9
    [9] K. Yamazaki, X. Wang, Global well-posedness and asymptotic behavior of solutions to a reaction-convection-diffusion cholera epidemic model, Discrete Contin. Dyn. Syst. Ser. -B, 21 (2016), 1297–1316. https://doi.org/10.3934/dcdsb.2016.21.1297 doi: 10.3934/dcdsb.2016.21.1297
    [10] K. Yamazaki, X. Wang, Global stability and uniform persistence of the reaction-convection-diffusion cholera epidemic model, Math. Biosci. Eng., 14 (2017), 559–579. https://doi.org/10.3934/mbe.2017033 doi: 10.3934/mbe.2017033
    [11] K. Yamazaki, Zika virus dynamics partial differential equations model with sexual transmission route, Nonlinear Anal. Real World Appl., 50 (2019), 290–315. https://doi.org/10.1016/j.nonrwa.2019.05.003 doi: 10.1016/j.nonrwa.2019.05.003
    [12] S. B. Hsu, J. Jiang, F. B. Wang, On a system of reaction-diffusion equations arising from competition with internal storage in an unstirred chemostat, J. Differ. Equations, 248 (2010), 2470–2496. https://doi.org/10.1016/j.jde.2009.12.014 doi: 10.1016/j.jde.2009.12.014
    [13] S. B. Hsu, F. B. Wang, X. Q. Zhao, Dynamics of a periodically pulsed bio-reactor model with a hydraulic storage zone, J. Dyn. Differ. Equations, 23 (2011), 817–842. https://doi.org/10.1007/s10884-011-9224-3 doi: 10.1007/s10884-011-9224-3
    [14] J. P. Grover, S. B. Hsu, F. B. Wang, Competition and coexistence in flowing habitats with a hydraulic storage zone, Math. Biosci., 222 (2009), 42–52. https://doi.org/10.1016/j.mbs.2009.08.006 doi: 10.1016/j.mbs.2009.08.006
    [15] S. B. Hsu, F. B. Wang, X. Q. Zhao, Global dynamics of zooplankton and harmful algae in flowing habitats, J. Differ. Equations, 255 (2013), 265–297. https://doi.org/10.1016/j.jde.2013.04.006 doi: 10.1016/j.jde.2013.04.006
    [16] X. Q. Zhao, Dynamical Systems in Population Biology, Springer-Verlag, New York, Inc., 2003. https://doi.org/10.1007/978-0-387-21761-1
    [17] N. K. Vaidya, F. B. Wang, X. Zou, Avian influenza dynamics in wild birds with bird mobility and spatial heterogeneous environment, Discrete Contin. Dyn. Syst. Ser. -B, 17 (2012), 2829–2848. https://doi.org/10.3934/dcdsb.2012.17.2829 doi: 10.3934/dcdsb.2012.17.2829
    [18] K. Yamazaki, Threshold dynamics of reaction-diffusion partial differential equations model of Ebola virus disease, Int. J. Biomath., 11 (2018), 1850108. https://doi.org/10.1142/S1793524518501085 doi: 10.1142/S1793524518501085
    [19] Z. J. Cheng, J. Shan, Novel coronavirus: where we are and what we know, Infection, 48 (2020), 155–163. https://doi.org/10.1007/s15010-020-01401-y doi: 10.1007/s15010-020-01401-y
    [20] C. Yang, J. Wang, A mathematical model for the novel coronavirus epidemic in Wuhan, China, Math. Biosci. Eng., 17 (2020), 2708–2724. https://doi.org/10.3934/mbe.2020148 doi: 10.3934/mbe.2020148
    [21] J. D. Brown, G. Goekjian, R. Poulson, S. Valeika, D. E. Stallknecht, Avian influenza virus in water: Infectivity is dependent on pH, salinity and temperature, Vet. Microbiol., 136 (2009), 20–26. https://doi.org/10.1016/j.vetmic.2008.10.027 doi: 10.1016/j.vetmic.2008.10.027
    [22] V. S. Hinshaw, R. G. Webster, B. Turner, The perpetuation of orthomyxoviruses and paramyxoviruses in Canadian waterfowl, Can. J. Microbiol., 26 (1980), 622–629. https://doi.org/10.1139/m80-108 doi: 10.1139/m80-108
    [23] R. G. Webster, M. Yakhno, V. S. Hinshaw, W. J. Bean, K. G. Murti, Intestinal influenza: replication and characterization of influenza viruses in ducks, Virology, 84 (1978), 268–278. https://doi.org/10.1016/0042-6822(78)90247-7 doi: 10.1016/0042-6822(78)90247-7
    [24] World Health Organization, Ebola virus disease, 2023. Available from: https://www.who.int/news-room/fact-sheets/detail/ebola-virus-disease.
    [25] L. Evans, Partial Differential Equations, American Mathematics Society, Providence, Rhode Island, 1998.
    [26] R. Covington, S. Patton, E. Walker, K. Yamazaki, Stability analysis on a partially diffusive model of the coronavirus disease of 2019, submitted.
    [27] W. Puryear, K. Sawatzki, N. Hill, A. Foss, J. J. Stone, L. Doughty, et al., Pathogenic Avian Influenza A(H5N1) virus outbreak in New England Seals, United States, Emerging Infect. Dis., 29 (2023), 786–791. https://doi.org/10.3201/eid2904.221538 doi: 10.3201/eid2904.221538
    [28] T. Berge, J. M. S. Luburma, G. M. Moremedi, N. Morris, R. Kondera-Shava, A simple mathematical model for Ebola in Africa, J. Biol. Dyn., 11 (2017), 42–74. https://doi.org/10.1080/17513758.2016.1229817 doi: 10.1080/17513758.2016.1229817
    [29] World Health Organization, Ebola disease caused by Sudan ebolavirus - Uganda, 2023. Available from: https://www.who.int/emergencies/disease-outbreak-news/item/2023-DON433.
    [30] C. Freeman, Meet the world's bravest undertakers - Liberia's Ebola burial squad, The Telegraph, 2014. Available from: https://www.telegraph.co.uk/news/worldnews/ebola/11024042/Meet-the-worlds-bravest-undertakers-Liberias-Ebola-burial-squad.html.
    [31] H. L. Smith, X. Q. Zhao, Robust persistence for semidynamical systems, Nonlinear Anal. Theory Methods Appl., 47 (2001), 6169–6179. https://doi.org/10.1016/S0362-546X(01)00678-2 doi: 10.1016/S0362-546X(01)00678-2
    [32] H. L. Smith, Monotone Dynamical Systems: An Introduction to the Theory of Competitive and Cooperative Systems, Mathematical Surveys and Monographs, American Mathematical Society, Providence, Rhode Island, 41 (1995).
    [33] H. R. Thieme, Convergence results and a Poincarˊe-Bendixson trichotomy for asymptotically autonomous differential equations, J. Math. Biol., 30 (1992), 755–763. https://doi.org/10.1007/BF00173267 doi: 10.1007/BF00173267
    [34] P. Magal, X. Q. Zhao, Global attractors and steady states for uniformly persistent dynamical systems, SIAM J. Math. Anal., 37 (2005), 251–275. https://doi.org/10.1137/S0036141003439173 doi: 10.1137/S0036141003439173
    [35] K. Deimling, Nonlinear Functional Analysis, Dover Publications, Inc., Mineola, New York, 1985. https://doi.org/10.1007/978-3-662-00547-7
    [36] J. K. Hale, Asymptotic Behavior of Dissipative Systems, Mathematical Surveys and Monographs, American Mathematics Society, Providence, Rhode Island, 1988. https://doi.org/10.1090/surv/025
    [37] J. Wang, C. Yang, K. Yamazaki, A partially diffusive cholera model based on a general second-order differential operator, J. Math. Anal. Appl., 501 (2021), 125181. https://doi.org/10.1016/j.jmaa.2021.125181 doi: 10.1016/j.jmaa.2021.125181
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