Research article Special Issues

Optimal harvesting strategy for stochastic hybrid delay Lotka-Volterra systems with Lévy noise in a polluted environment


  • This paper concerns the dynamics of two stochastic hybrid delay Lotka-Volterra systems with harvesting and Lévy noise in a polluted environment (i.e., predator-prey system and competitive system). For every system, sufficient and necessary conditions for persistence in mean and extinction of each species are established. Then, sufficient conditions for global attractivity of the systems are obtained. Finally, sufficient and necessary conditions for the existence of optimal harvesting strategy are provided. The accurate expressions for the optimal harvesting effort (OHE) and the maximum of expectation of sustainable yield (MESY) are given. Our results show that the dynamic behaviors and optimal harvesting strategy are closely correlated with both time delays and three types of environmental noises (namely white Gaussian noises, telephone noises and Lévy noises).

    Citation: Sheng Wang, Lijuan Dong, Zeyan Yue. Optimal harvesting strategy for stochastic hybrid delay Lotka-Volterra systems with Lévy noise in a polluted environment[J]. Mathematical Biosciences and Engineering, 2023, 20(4): 6084-6109. doi: 10.3934/mbe.2023263

    Related Papers:

    [1] Yuanpei Xia, Weisong Zhou, Zhichun Yang . Global analysis and optimal harvesting for a hybrid stochastic phytoplankton-zooplankton-fish model with distributed delays. Mathematical Biosciences and Engineering, 2020, 17(5): 6149-6180. doi: 10.3934/mbe.2020326
    [2] B. Spagnolo, D. Valenti, A. Fiasconaro . Noise in ecosystems: A short review. Mathematical Biosciences and Engineering, 2004, 1(1): 185-211. doi: 10.3934/mbe.2004.1.185
    [3] P. Auger, N. H. Du, N. T. Hieu . Evolution of Lotka-Volterra predator-prey systems under telegraph noise. Mathematical Biosciences and Engineering, 2009, 6(4): 683-700. doi: 10.3934/mbe.2009.6.683
    [4] S. Nakaoka, Y. Saito, Y. Takeuchi . Stability, delay, and chaotic behavior in a Lotka-Volterra predator-prey system. Mathematical Biosciences and Engineering, 2006, 3(1): 173-187. doi: 10.3934/mbe.2006.3.173
    [5] Suqing Lin, Zhengyi Lu . Permanence for two-species Lotka-Volterra systems with delays. Mathematical Biosciences and Engineering, 2006, 3(1): 137-144. doi: 10.3934/mbe.2006.3.137
    [6] Mengqing Zhang, Qimin Zhang, Jing Tian, Xining Li . The asymptotic stability of numerical analysis for stochastic age-dependent cooperative Lotka-Volterra system. Mathematical Biosciences and Engineering, 2021, 18(2): 1425-1449. doi: 10.3934/mbe.2021074
    [7] Xiaomeng Ma, Zhanbing Bai, Sujing Sun . Stability and bifurcation control for a fractional-order chemostat model with time delays and incommensurate orders. Mathematical Biosciences and Engineering, 2023, 20(1): 437-455. doi: 10.3934/mbe.2023020
    [8] Guichen Lu, Zhengyi Lu . Permanence for two-species Lotka-Volterra cooperative systems with delays. Mathematical Biosciences and Engineering, 2008, 5(3): 477-484. doi: 10.3934/mbe.2008.5.477
    [9] Yuanshi Wang, Donald L. DeAngelis . A mutualism-parasitism system modeling host and parasite with mutualism at low density. Mathematical Biosciences and Engineering, 2012, 9(2): 431-444. doi: 10.3934/mbe.2012.9.431
    [10] Zeyan Yue, Sheng Wang . Dynamics of a stochastic hybrid delay food chain model with jumps in an impulsive polluted environment. Mathematical Biosciences and Engineering, 2024, 21(1): 186-213. doi: 10.3934/mbe.2024009
  • This paper concerns the dynamics of two stochastic hybrid delay Lotka-Volterra systems with harvesting and Lévy noise in a polluted environment (i.e., predator-prey system and competitive system). For every system, sufficient and necessary conditions for persistence in mean and extinction of each species are established. Then, sufficient conditions for global attractivity of the systems are obtained. Finally, sufficient and necessary conditions for the existence of optimal harvesting strategy are provided. The accurate expressions for the optimal harvesting effort (OHE) and the maximum of expectation of sustainable yield (MESY) are given. Our results show that the dynamic behaviors and optimal harvesting strategy are closely correlated with both time delays and three types of environmental noises (namely white Gaussian noises, telephone noises and Lévy noises).



    Optimal harvesting problem is an important and interesting topic from both biological and mathematical point of view. The classical two-species deterministic Lotka-Volterra system with harvesting under catch-per-unit-effort hypothesis [1] can be expressed as follows:

    {dx1(t)=x1(t)[¯r1¯a11x1(t)¯a12x2(t)]dth1x1(t)dt,dx2(t)=x2(t)[¯r2¯a21x1(t)¯a22x2(t)]dth2x2(t)dt, (1.1)

    where xi(t) represent the population densities of species i at time t. ¯ri and ¯aij are constants. hi0 represents the harvesting effort of xi(t) (i,j=1,2).

    However, the deterministic system has its limitation in mathematical modeling of ecosystems since the parameters involved in the system are unable to capture the influence of environmental noises [2,3]. Hence, it is of enormous importance to study the effects of environmental noises on the dynamics of population systems. Introducing white Gaussian noises into the deterministic system is the most common way to characterize environmental noises [4,5]. Assume that ¯ri are affected by white Gaussian noises, i.e., ¯ri¯ri+σi˙Wi(t), where Wi(t) are standard Wiener processes defined on a complete probability space (Ω,F,P) with a filtration {Ft}t0 satisfying the usual conditions. Then, system (1.1) becomes

    {dx1(t)=x1(t)[¯r1h1¯a11x1(t)¯a12x2(t)]dt+σ1x1(t)dW1(t),dx2(t)=x2(t)[¯r2h2¯a21x1(t)¯a22x2(t)]dt+σ2x2(t)dW2(t). (1.2)

    On the other hand, many academics argue that parameters in ecosystems often switch because of environmental changes, for example, some species have different growth rates at different temperatures, and these changes can be well described by a continuous-time Markov chain ρ(t) with finite-state space, instead of white Gaussian noises [6,7,8,9,10,11,12,13]. System (1.2) under regime switching can be expressed as follows:

    {dx1(t)=x1(t)[¯r1(ρ(t))h1¯a11(ρ(t))x1(t)¯a12(ρ(t))x2(t)]dt+σ1(ρ(t))x1(t)dW1(t),dx2(t)=x2(t)[¯r2(ρ(t))h2¯a21(ρ(t))x1(t)¯a22(ρ(t))x2(t)]dt+σ2(ρ(t))x2(t)dW2(t), (1.3)

    where ρ(t) is a right-continuous Markov chain with finite values S={1,2,...,S}, ¯ri(ρ(t)) and ¯aij(ρ(t)) are functions with finite values. Furthermore, population systems may suffer sudden environmental perturbations, such as earthquake, torrential flood, typhoon and infectious disease. Some scholars claimed that Lévy noise can be used to describe these sudden environmental perturbations [14,15,16,17,18,19]. Introducing Lévy noise into system (1.2) yields

    {dx1(t)=x1(t)[¯r1(ρ(t))h1¯a11(ρ(t))x1(t)¯a12(ρ(t))x2(t)]dt+σ1(ρ(t))x1(t)dW1(t)+Zx1(t)γ1(μ,ρ(t))˜N(dt,dμ),dx2(t)=x2(t)[¯r2(ρ(t))h2¯a21(ρ(t))x1(t)¯a22(ρ(t))x2(t)]dt+σ2(ρ(t))x2(t)dW2(t)+Zx2(t)γ2(μ,ρ(t))˜N(dt,dμ), (1.4)

    where N is a Poisson counting measure with characteristic measure λ on a measurable subset Z[0,+) with λ(Z)<+ and ˜N(dt,dμ)=N(dt,dμ)λ(dμ)dt, γj(μ,ρ(t)) are bounded functions. For the sake of simplicity, we define

    Si(t,ρ(t))=σi(ρ(t))dWi(t)+Zγi(μ,ρ(t))˜N(dt,dμ)(i=1,2). (1.5)

    Hence, system (1.4) can be rewritten into

    {dx1(t)=x1(t){[¯r1(ρ(t))h1¯a11(ρ(t))x1(t)¯a12(ρ(t))x2(t)]dt+S1(t,ρ(t))},dx2(t)=x2(t){[¯r2(ρ(t))h2¯a21(ρ(t))x1(t)¯a22(ρ(t))x2(t)]dt+S2(t,ρ(t))}. (1.6)

    Given the growing importance of environmental noises in the dynamics of complex physical and biological systems, interdisciplinary stochastic systems driven by two different types of environment noises have attracted great attention in the last few decades [20,21,22,23,24,25,26,27,28,29,30,31,32]. Particularly, Giorgio Parisi's Nobel Prize in Physics (2021) expounded on the importance of fluctuations on physics and systems from microscopic to macroscopic physics.

    In the natural environment, in addition to being subject to environmental noises, the trends of biological systems depend not only on the present state but also on the past state, such as the growth period from juvenile to adult in the growth model of biological populations. Such phenomena are called time-delay phenomena. "All species should exhibit time delay" in the real world [33] and incorporating time delay into biological systems makes them much more realistic than those without delay, since a species growth rate relies on not only the current state, but also the past state [34,35,36]. As we all know, systems with discrete time delays and those with continuously distributed time delays do not contain each other. However, systems with S-type distributed time delays contain both [37,38].

    Furthermore, with a growing number of toxicant entering into the ecosystem, many species have been extinctive and some of them are on the verge of extinction, environmental pollution has received much attention in international society. Naturally, it is meaningful to estimate environmental toxicity so as to develop optimal harvesting policies.

    In the past few decades, stochastic population systems driven by different types of environment noises have received great attention and have been studied extensively. For example, Abbas et al. [39] studied the effect of stochastic perturbation on a two-species competitive system by constructing a suitable Lyapunov functional. Han et al. [40] investigated two-species Lotka-Volterra delayed stochastic predator-prey systems, with and without pollution. Liu and Chen [41] investigated a stochastic delay predator-prey system with Lévy noise in a polluted environment. Zhao and Yuan [42] considered the optimal harvesting policy of a stochastic two-species competitive model with Lévy noise in a polluted environment. Liu et al. [43] studied the dynamics of a stochastic regime-switching predator-prey system with harvesting and distributed delays.

    However, to the best of our knowledge to date, results about stochastic time-delay population system driven by three different types of environment noises have rarely been report. Hence, in this paper we consider the optimization problems of harvesting for the following two stochastic hybrid delay Lotka-Volterra systems with Lévy noise in a polluted environment:

    {dx1(t)=x1(t)[(r1(ρ(t))h1r11C1(t)D11(x1)(t)D12(x2)(t))dt+S1(t,ρ(t))],dx2(t)=x2(t)[(r2(ρ(t))h2r22C2(t)+D21(x1)(t)D22(x2)(t))dt+S2(t,ρ(t))],dC1(t)=[k1CE(t)(g1+m1)C1(t)]dt,dC2(t)=[k2CE(t)(g2+m2)C2(t)]dt,dCE(t)=[hCE(t)+u(t)]dt, (1.7)

    and

    {dx1(t)=x1(t)[(r1(ρ(t))h1r11C1(t)D11(x1)(t)D12(x2)(t))dt+S1(t,ρ(t))],dx2(t)=x2(t)[(r2(ρ(t))h2r22C2(t)D21(x1)(t)D22(x2)(t))dt+S2(t,ρ(t))],dC1(t)=[k1CE(t)(g1+m1)C1(t)]dt,dC2(t)=[k2CE(t)(g2+m2)C2(t)]dt,dCE(t)=[hCE(t)+u(t)]dt, (1.8)

    where

    Dji(xi)(t)=ajixi(t)+0τjixi(t+θ)dμji(θ)(i,j=1,2),

    0τjixi(t+θ)dμji(θ) are Lebesgue-Stieltjes integrals, τji>0 are time delays, μji(θ), θ[τ,0] are nondecreasing bounded variation functions, τ=max{τji}. For other parameters in systems (1.7) and (1.8), see Table 1.

    Table 1.  Definition of some parameters in system (1.7).
    Parameter Definitions
    Ci(t) the toxicant concentration in the organism of species i at time t
    CE(t) the toxicant concentration in the environment at time t
    rii the dose-response rate of species i to the organismal toxicant
    ki the toxin uptake rate per unit biomass
    gi the organismal net ingestion rate of toxin
    mi the organismal deportation rate of toxin
    h the rate of toxin loss in the environment
    u(t) the exogenous total toxicant input into environment at time t

     | Show Table
    DownLoad: CSV

    As fundamental assumptions, we assume that W1(t), W2(t), ρ(t) and N are independent and ρ(t) is irreducible. Hence, ρ(t) has a unique stationary distribution π=(π1,π2,...,πS). Our aim is, for each system of (1.7) and (1.8), to get the optimal harvesting effort H=(h1,h2)T such that

    ① Both x1(t) and x2(t) are not extinct;

    ② The expectation of sustained yield Y(H)=limt+E[2i=1hixi(t)] is maximal.

    The rest of this paper is arranged as follows. In Section 2, we study the existence and uniqueness of global positive solution to systems (1.7) and (1.8). For every system, sufficient and necessary conditions for persistence in mean and extinction of each species are obtained in Section 3. We discuss the conditions for global attractivity of the systems in Section 4. In Section 5, sufficient and necessary conditions for the existence of optimal harvesting strategy are established. Furthermore, we give the accurate expressions for the OHE and MESY. Finally, some brief conclusions and discussions are shown in Section 6.

    In this paper, we have three fundamental assumptions for systems (1.7) and (1.8).

    Assumption 1. rj(i)>0, ajk(i)>0 and there exist γj(i)γj(i)>1 such that γj(i)γj(μ,i)γj(i) (μZ), iS, j,k=1,2. Hence, for any constant p>0, there exists Cj(p)>0 such that

    maxiS{Z[ln(1+γj(μ,i))]2λ(dμ)}Cj(p)<+. (2.1)

    Remark 1. Assumption 1 implies that the intensity of Lévy noise is not too big to ensure that the solution will not explode in finite time (see, e.g., [42,44,45,46,47]).

    Assumption 2. 0<kigi+mi (i=1,2), suptR+u(t)h.

    Remark 2. Assumption 2 means 0Ci(t)<1 (i=1,2) and 0CE(t)<1, which must be satisfied to be realistic because C1(t), C2(t) and CE(t) are concentrations of the toxicant (see Lemma 2.1 in [48]).

    Assumption 3. The limit of u(t) when t+ exists, i.e., limt+u(t)=uE.

    Lemma 1. (Lemma 4.2 in [49]) If Assumption 3 holds, then

    limt+CE(t)=uEh,limt+t1t0Ci(s)ds=kiuE(gi+mi)hCEi(i=1,2). (2.2)

    To study the long-term dynamics of a stochastic population system, we first study the existence and uniqueness of global positive solution to the system.

    Theorem 1. For any initial condition (ξ1,ξ2)TC([τ,0],R2+), system (1.7) (or system (1.8)) has a unique global solution (x1(t),x2(t))TR2+ on t[τ,+) a.s. Moreover, for any constant p>0, there exists Ki(p)>0 such that

    suptτE[xpi(t)]Ki(p)(i=1,2). (2.3)

    Proof. The proof is standard and hence is omitted (see e.g., [50]).

    Before studying the persistence in mean and extinction of systems (1.7) and (1.8), we first present the following lemma.

    Lemma 2. Denote o(t)={f(t)|limt+f(t)t=0}. Suppose Z(t)C(Ω×[0,+),R+)([51]).

    (i) If there exists constant δ0>0 such that for t1,

    lnZ(t)δtδ0t0Z(s)ds+o(t), (3.1)

    then

    {lim supt+t1t0Z(s)dsδδ0a.s.(δ0);limt+Z(t)=0a.s.(δ<0). (3.2)

    (ii) If there exist constants δ>0 and δ0>0 such that for t1,

    lnZ(t)δtδ0t0Z(s)ds+o(t), (3.3)

    then

    lim inft+t1t0Z(s)dsδδ0a.s. (3.4)

    Denote

    {B1()=r1()σ21()2Z[γ1(μ,)ln(1+γ1(μ,))]λ(dμ),B2()=r2()+σ22()2+Z[γ2(μ,)ln(1+γ2(μ,))]λ(dμ),Aij=aij+0τijdμij(θ)(i,j=1,2),Σ1=Si=1πiB1(i),Σ2=Si=1πiB2(i)+A21A11Σ1,|A|=|A11A12A21A22|,|A1|=|Σ1r11CE1h1A12Σ2A21A11Σ1r22CE2h2A22|,|A2|=|A11Σ1r11CE1h1A21Σ2A21A11Σ1r22CE2h2|,Δ1=|Σ1r11CE1A12Σ2A21A11Σ1r22CE2A22|,Δ2=|A11Σ1r11CE1A21Σ2A21A11Σ1r22CE2|. (3.5)

    To begin with, let us consider the following stochastic auxiliary system:

    {dX1(t)=X1(t)[(r1(ρ(t))h1r11C1(t)D11(X1)(t))dt+S1(t,ρ(t))],dX2(t)=X2(t)[(r2(ρ(t))h2r22C2(t)+D21(X1)(t)D22(X2)(t))dt+S2(t,ρ(t))],dC1(t)=[k1CE(t)(g1+m1)C1(t)]dt,dC2(t)=[k2CE(t)(g2+m2)C2(t)]dt,dCE(t)=[hCE(t)+u(t)]dt. (3.6)

    Lemma 3. For system (3.6):

    (a) If Σ1r11CE1h1<0, then limt+Xi(t)=0 a.s. (i=1,2).

    (b) If Σ1r11CE1h10, Σ2A21A11r11CE1r22CE2A21A11h1h2<0, then

    limt+t1t0X1(s)ds=Σ1r11CE1h1A11,limt+X2(t)=0a.s. (3.7)

    (c) If Σ1r11CE1h10, Σ2A21A11r11CE1r22CE2A21A11h1h20, then

    limt+t1t0X1(s)ds=Σ1r11CE1h1A11,limt+t1t0X2(s)ds=A122(Σ2A21A11r11CE1r22CE2A21A11h1h2)a.s. (3.8)

    Proof. By Itô's formula and the strong law of large numbers, we compute

    {lnX1(t)=(Σ1r11CE1h1)tA11t0X1(s)dsT11(X1)(t)+o(t),lnX2(t)=(Σ2A21A11Σ1r22CE2h2)t+A21t0X1(s)dsA22t0X2(s)ds+T21(X1)(t)T22(X2)(t)+o(t), (3.9)

    where

    Tji(Xi)(t)=0τji0θXi(s)dsdμji(θ)0τjitt+θXi(s)dsdμji(θ). (3.10)

    Case(i): Σ1r11CE1h1<0. Then limt+X1(t)=0 a.s. Hence, for ϵ(0,1) and t1,

    lnX2(t)(Σ2A21A11Σ1r22CE2h2+ϵ)ta22t0X2(s)ds, (3.11)

    which implies limt+X2(t)=0 a.s.

    Case(ii): Σ1r11CE1h10. Consider the following auxiliary function:

    d~X2(t)=~X2(t)[(r2(ρ(t))h2r22C2(t)+D21(X1)(t)a22~X2(t))dt+S2(t,ρ(t))]. (3.12)

    Then X2(t)~X2(t) a.s. By Itô's formula, for ϵ(0,1) and t1,

    {ln~X2(t)(Σ2A21A11r11CE1r22CE2A21A11h1h2+ϵ)ta22t0~X2(s)ds,ln~X2(t)(Σ2A21A11r11CE1r22CE2A21A11h1h2ϵ)ta22t0~X2(s)ds. (3.13)

    Thanks to Lemma 2 and the arbitrariness of ϵ, for arbitrary γ>0,

    limt+t1ttγXi(s)ds=0a.s.(i=1,2). (3.14)

    According to (3.14) and system (3.9), for ϵ(0,1) and t1,

    {lnX2(t)(Σ2A21A11r11CE1r22CE2A21A11h1h2+ϵ)tA22t0X2(s)ds,lnX2(t)(Σ2A21A11r11CE1r22CE2A21A11h1h2ϵ)tA22t0X2(s)ds. (3.15)

    Based on Lemma 2 and the arbitrariness of ϵ, we obtain:

    (1) If Σ1r11CE1h10,Σ2A21A11r11CE1r22CE2A21A11h1h2<0, thenlimt+X2(t)=0a.s.(2) If Σ1r11CE1h10,Σ2A21A11r11CE1r22CE2A21A11h1h20, thenlimt+t1t0X2(s)ds=A122(Σ2A21A11r11CE1r22CE2A21A11h1h2)a.s.

    Lemma 4. For system (1.7), lim supt+t1lnxi(t)0 a.s. (i=1,2).

    Proof. Thanks to Lemma 3 and (3.9), system (3.6) satisfies limt+t1lnXi(t)=0 a.s. (i=1,2). From the stochastic comparison theorem, we obtain the desired assertion.

    Lemma 5. For system (1.7), if limt+x1(t)=0 a.s., then limt+x2(t)=0 a.s.

    Proof. The proof of Lemma 5 is similar to that of Lemma 3 (a) and here is omitted.

    Theorem 2. For system (1.7), define Θ1=Σ1r11CE1h1, Θ2=|A2|A21.

    (i) If Θ2>0, then

    limt+t1t0xi(s)ds=|Ai||A|a.s.(i=1,2). (3.16)

    (ii) If Θ1>0>Θ2, then

    limt+t1t0x1(s)ds=Θ1A11,limt+x2(t)=0a.s. (3.17)

    (iii) If 0>Θ1, then limt+xi(t)=0 a.s. (i=1,2).

    Proof. Clearly, Θ1>Θ2. Thanks to (3.14), for γ>0,

    limt+t1ttγxi(s)ds=0a.s.(i=1,2). (3.18)

    By Itô's formula and (3.18), we deduce

    {lnx1(t)=(Σ1r11CE1h1)tA11t0x1(s)dsA12t0x2(s)ds)+o(t),lnx2(t)=(Σ2A21A11Σ1r22CE2h2)t+A21t0x1(s)dsA22t0x2(s)ds+o(t). (3.19)

    Case(i): Θ2>0. According to system (3.19), we compute

    {limt+t1(A22lnx1(t)A12lnx2(t)+|A|t0x1(s)ds)=|A1|,limt+t1(A21lnx1(t)+A11lnx2(t)+|A|t0x2(s)ds)=|A2|. (3.20)

    Based on Lemma 4, for ϵ(0,1) and t1,

    {A22lnx1(t)(|A1|+ϵ)t|A|t0x1(s)ds,A11lnx2(t)(|A2|ϵ)t|A|t0x2(s)ds. (3.21)

    In view of Lemma 2 and the arbitrariness of ϵ, we obtain

    lim inft+t1t0x2(s)ds|A2||A|a.s. (3.22)

    By (3.22), x2(t) is not extinct. Based on Lemma 5, x1(t) is not extinct either. In view of Lemma 2 and the arbitrariness of ϵ, we obtain

    lim supt+t1t0x1(s)ds|A1||A|a.s. (3.23)

    According to (3.23) and system (3.19), for ϵ(0,1) and t1,

    lnx2(t)(Σ2A21A11Σ1r22CE2h2+A21|A1||A|+ϵ)tA22t0x2(s)ds. (3.24)

    Thanks to Lemma 2 and the arbitrariness of ϵ, we obtain

    lim supt+t1t0x2(s)ds|A2||A|a.s. (3.25)

    Combining (3.22) with (3.25) yields

    limt+t1t0x2(s)ds=|A2||A|a.s. (3.26)

    Combining (3.26) with system (3.19) yields that for ϵ(0,1) and t1,

    {lnx1(t)(Σ1r11CE1h1A12|A2||A|ϵ)tA11t0x1(s)ds,lnx1(t)(Σ1r11CE1h1A12|A2||A|+ϵ)tA11t0x1(s)ds. (3.27)

    Based on Lemma 2 and the arbitrariness of ϵ, we obtain

    limt+t1t0x1(s)ds=|A1||A|a.s. (3.28)

    Case(ii): Θ1>0>Θ2. In view of (3.20), we deduce

    lim supt+t1ln[xA211(t)xA112(t)]|A2|<0a.s. (3.29)

    By Lemma 5, limt+x2(t)=0 a.s. Thus, for ϵ(0,1) and t1,

    {lnx1(t)(Σ1r11CE1h1ϵ)tA11t0x1(s)ds,lnx1(t)(Σ1r11CE1h1+ϵ)tA11t0x1(s)ds. (3.30)

    Thanks to Lemma 2 and the arbitrariness of ϵ, we obtain

    limt+t1t0x1(s)ds=Θ1A11a.s. (3.31)

    Case(iii): 0>Θ1. By system (3.19), for ϵ(0,1) and t1,

    lnx1(t)(Θ1+ϵ)tA11t0x1(s)ds. (3.32)

    So, limt+x1(t)=0 a.s. From Lemma 5, limt+x2(t)=0 a.s.

    Remark 3. If S={1}, hi=0, rii=0, μii(θ) are constant functions defined on [τ,0], aij=0 (ij) and μij(θ) are defined as follows:

    μ12(θ)={a12,τ12θ0,0,τ12θ<τ12,μ21(θ)={a21,τ21θ0,0,τ21θ<τ21,

    then system (1.7) becomes

    {dx1(t)=x1(t)[(r1a11x1(t)a12x2(tτ12))dt+S1(t)],dx2(t)=x2(t)[(r2+a21x1(tτ21)a22x2(t))dt+S2(t)]. (3.33)

    Hence, Theorem 2 contains Theorem 1 in [52] and Theorem 2 in [53] as a special case.

    Remark 4. If S={1}, hi=0, γi(μ,1)=0, μii(θ) are constant functions defined on [τ,0], aij=0 (ij) and μij(θ) are defined as follows:

    μ12(θ)={a12,τ12θ0,0,τ12θ<τ12,μ21(θ)={a21,τ21θ0,0,τ21θ<τ21,

    then system (1.7) becomes

    {dx1(t)=x1(t)[(r1r11C1(t)a11x1(t)a12x2(tτ12))dt+σ1dW1(t)],dx2(t)=x2(t)[(r2r22C2(t)+a21x1(tτ21)a22x2(t))dt+σ2dW2(t)],dC1(t)=[k1CE(t)(g1+m1)C1(t)]dt,dC2(t)=[k2CE(t)(g2+m2)C2(t)]dt,dCE(t)=[hCE(t)+u(t)]dt. (3.34)

    Hence, Theorem 2 contains Theorems 4.1, 4.2, 5.1 and 5.2 in [40] as a special case.

    Denote

    {Bi()=ri()σ2i()2Z[γi(μ,)ln(1+γi(μ,))]λ(dμ),Aij=aij+0τijdμij(θ),Σj=Si=1πiBj(i)rjjCEj,Ξj=Σjhj(i,j=1,2),Δ=|A11A12A21A22|,Δ1=|Ξ1A12Ξ2A22|,Δ2=|A11Ξ1A21Ξ2|,Γ1=|Σ1A12Σ2A22|,Γ2=|A11Σ1A21Σ2|. (3.35)

    To begin with, let us consider the following stochastic auxiliary system:

    { dX1(t)=X1(t)[(r1(ρ(t))h1r11C1(t)D11(X1)(t))dt+S1(t,ρ(t))],dX2(t)=X2(t)[(r2(ρ(t))h2r22C2(t)D21(X1)(t)D22(X2)(t))dt+S2(t,ρ(t))],dC1(t)=[k1CE(t)(g1+m1)C1(t)]dt,dC2(t)=[k2CE(t)(g2+m2)C2(t)]dt,dCE(t)=[hCE(t)+u(t)]dt. (3.36)

    Lemma 6. For system (3.36):

    (1)IfΞ1<0,Ξ2<0,thenlimt+Xi(t)=0a.s.(i=1,2).(2)IfΞ1<0,Ξ20,thenlimt+X1(t)=0,limt+t1t0X2(s)ds=Ξ2A22a.s.(3)IfΞ10,Ξ2A21Ξ1A11<0,thenlimt+t1t0X1(s)ds=Ξ1A11,limt+X2(t)=0a.s.(4)IfΞ10,Ξ2A21Ξ1A110,thenlimt+t1t0X1(s)ds=Ξ1A11,limt+t1t0X2(s)ds=A122(Ξ2A21Ξ1A11)a.s.

    Proof. Thanks to Itô's formula and the strong law of large numbers, we obtain

    {lnX1(t)=Ξ1tA11t0X1(s)dsT11(X1)(t)+o(t),lnX2(t)=Ξ2tA21t0X1(s)dsA22t0X2(s)dsT21(X1)(t)T22(X2)(t)+o(t). (3.37)

    Case(i): Ξ1<0. Then limt+X1(t)=0 a.s. Consider the following auxiliary system:

    d~X2(t)=~X2(t)[(r2(ρ(t))h2r22C2(t)D21(X1)(t)a22~X2(t))dt+S2(t,ρ(t))]. (3.38)

    Then X2(t)~X2(t) a.s. By Itô's formula, we obtain

    ln~X2(t)=Ξ2tA21t0X1(s)dsa22t0~X2(s)dsT21(X1)(t)+o(t). (3.39)

    Therefore, for ϵ(0,1) and t1,

    ln~X2(t)(Ξ2+ϵ)ta22t0~X2(s)ds,ln~X2(t)(Ξ2ϵ)ta22t0~X2(s)ds. (3.40)

    In view of Lemma 2 and the arbitrariness of ϵ, we obtain:

    (1) If Ξ1<0,Ξ2<0, thenlimt+~X2(t)=0a.s.(2) If Ξ1<0,Ξ20, thenlimt+t1t0~X2(s)ds=Ξ2a22a.s.

    So, for γ>0, we have

    limt+t1ttγXi(s)ds=0a.s.(i=1,2). (3.41)

    Combining (3.37) with (3.41) yields that for ϵ(0,1) and t1,

    lnX2(t)(Ξ2+ϵ)tA22t0X2(s)ds,lnX2(t)(Ξ2ϵ)tA22t0X2(s)ds. (3.42)

    Thanks to Lemma 2 and the arbitrariness of ϵ, we obtain:

    (1) If Ξ1<0,Ξ2<0, thenlimt+Xi(t)=0a.s.(i=1,2).(2) If Ξ1<0,Ξ20, thenlimt+X1(t)=0,limt+t1t0X2(s)ds=Ξ2A22a.s.

    Case(ii): Ξ10. Then,

    limt+t1t0X1(s)ds=Ξ1A11a.s. (3.43)

    Combining (3.37) with (3.43) yields that for ϵ(0,1) and t1,

    {ln~X2(t)(Ξ2A21Ξ1A11+ϵ)ta22t0~X2(s)ds,ln~X2(t)(Ξ2A21Ξ1A11ϵ)ta22t0~X2(s)ds. (3.44)

    In view of Lemma 2 and the arbitrariness of ϵ, we obtain:

    (1) If Ξ10,Ξ2A21Ξ1A11<0, thenlimt+~X2(t)=0a.s.(2) If Ξ10,Ξ2A21Ξ1A110, thenlimt+t1t0~X2(s)ds=a122(Ξ2A21Ξ1A11)a.s.

    Hence, for γ>0, (3.41) is true. According to system (3.37) and (3.41), for ϵ(0,1) and t1,

    {lnX2(t)(Ξ2A21Ξ1A11+ϵ)tA22t0X2(s)ds,lnX2(t)(Ξ2A21Ξ1A11ϵ)tA22t0X2(s)ds. (3.45)

    Based on Lemma 2 and the arbitrariness of ϵ, we obtain:

    (1) If Ξ10,Ξ2A21Ξ1A11<0, thenlimt+t1t0X1(s)ds=Ξ1A11,limt+X2(t)=0a.s.(2) If Ξ10,Ξ2A21Ξ1A110, thenlimt+t1t0X1(s)ds=Ξ1A11,limt+t1t0X2(s)ds=A122(Ξ2A21Ξ1A11)a.s.

    Lemma 7. For system (1.8), lim supt+t1lnxi(t)0 a.s. (i=1,2).

    Proof. Thanks to Lemma 6 and (3.37), system (3.36) satisfies limt+t1lnXi(t)=0 a.s. (i=1,2). From the stochastic comparison theorem, we obtain the desired assertion.

    Theorem 3. For system (1.8):

    (1)IfΞ1<0,Ξ2<0;Δ0,Δ1<0,Ξ2<0;Δ0,Δ2<0,Ξ1<0,thenlimt+xi(t)=0a.s.(i=1,2).(2)IfΞ1<0,Ξ20;Δ0,Δ1<0,Ξ20,thenlimt+x1(t)=0,limt+t1t0x2(s)ds=Ξ2A22a.s.(3)IfΞ10,Ξ2<0;Δ0,Δ2<0,Ξ10,thenlimt+t1t0x1(s)ds=Ξ1A11,limt+x2(t)=0a.s.(4)IfΔ>0,Δ1>0,Δ20,thenlimt+t1t0x1(s)ds=Δ1Δa.s.(5)IfΔ>0,Δ10,Δ2>0,thenlimt+t1t0x2(s)ds=Δ2Δa.s.

    Proof. By Itô's formula, we compute

    {lnx1(t)=Ξ1tA11t0x1(s)dsA12t0x2(s)ds+o(t),lnx2(t)=Ξ2tA21t0x1(s)dsA22t0x2(s)ds+o(t). (3.46)

    According to system (3.46) and Lemma 2, we obtain:

    (1) If Ξ1<0,Ξ2<0, then limt+x1(t)=0,limt+x2(t)=0a.s.(2) If Ξ1<0,Ξ20, then limt+x1(t)=0,limt+t1t0x2(s)ds=Ξ2A22a.s.(3) If Ξ10,Ξ2<0, then limt+t1t0x1(s)ds=Ξ1A11,limt+x2(t)=0a.s.

    By system (3.46), we compute

    {A22lnx1(t)A12lnx2(t)=Δ1tΔt0x1(s)ds+o(t),A11lnx2(t)A21lnx1(t)=Δ2tΔt0x2(s)ds+o(t). (3.47)

    By Lemma 7 and (3.47), we obtain that for ϵ(0,1) and t1,

    A22lnx1(t)(Δ1+ϵ)tΔt0x1(s)ds,A11lnx2(t)(Δ2+ϵ)tΔt0x2(s)ds. (3.48)

    Making use of Lemma 2 yields

    {limt+x1(t)=0 a.s.(Δ0,Δ1<0);lim supt+t1t0x1(s)dsΔ1Δ a.s.(Δ>0,Δ10),limt+x2(t)=0 a.s.(Δ0,Δ2<0);lim supt+t1t0x2(s)dsΔ2Δ a.s.(Δ>0,Δ20). (3.49)

    On the one hand, combining system (3.46) with (3.49) yields

    (1) If Δ0,Δ1<0,Ξ2<0, then limt+x1(t)=0,limt+x2(t)=0a.s.(2) If Δ0,Δ1<0,Ξ20, then limt+x1(t)=0,limt+t1t0x2(s)ds=Ξ2A22a.s.(3) If Δ0,Δ2<0,Ξ1<0, then limt+x1(t)=0,limt+x2(t)=0a.s.(4) If Δ0,Δ2<0,Ξ10, then limt+t1t0x1(s)ds=Ξ1A11,limt+x2(t)=0a.s.

    On the other hand, in view of systems (3.46) and (3.49), we deduce that if Δ>0, Δ10 and Δ20, then for ϵ(0,1) and t1,

    {lnx1(t)(Ξ1A12Δ2Δϵ)tA11t0x1(s)ds,lnx2(t)(Ξ2A21Δ1Δϵ)tA22t0x2(s)ds. (3.50)

    According to Lemma 2 and the arbitrariness of ϵ, we obtain

    {lim inft+t1t0x1(s)dsΔ1Δa.s.(Δ>0,Δ1>0,Δ20);lim inft+t1t0x2(s)dsΔ2Δa.s.(Δ>0,Δ10,Δ2>0). (3.51)

    Thus, Theorem 3 (4)–(5) follows from combining (3.49) with (3.51).

    Remark 5. If S={1}, hi=0, rii=0 and μij(θ) are constant functions defined on [τ,0], then system (1.8) becomes

    {dx1(t)=x1(t)[(r1a11x1(t)a12x2(t))dt+S1(t)],dx2(t)=x2(t)[(r2a21x1(t)a22x2(t))dt+S2(t)]. (3.52)

    Hence, Theorem 3 contains Theorem 4 in [17] as a special case.

    Remark 6. If S={1}, hi=0, rii=0, μii(θ) are constant functions defined on [τ,0], aij=0 (ij) and μij(θ) are defined as follows:

    μ12(θ)={a12,τ12θ0,0,τ12θ<τ12,μ21(θ)={a21,τ21θ0,0,τ21θ<τ21,

    then system (1.8) becomes

    {dx1(t)=x1(t)[(r1a11x1(t)a12x2(tτ12))dt+S1(t)],dx2(t)=x2(t)[(r2a21x1(tτ21)a22x2(t))dt+S2(t)]. (3.53)

    Hence, Theorem 3 contains Theorem 1 in [53] as a special case.

    Assumption 4. 2ajj>2i=1Aij (j=1,2).

    Theorem 4. Under Assumption 4, system (1.7) (or system (1.8)) is globally attractive.

    Proof. Let (x1(t;ϕ),x2(t;ϕ))T and (x1(t;ϕ),x2(t;ϕ))T be, respectively, the solution to system (1.7) (or system (1.8)) with ϕ and ϕC([τ,0],R2+), we only need to show

    limt+E|xi(t;ϕ)xi(t;ϕ)|=0(i=1,2). (4.1)

    Define

    W(t;ϕ,ϕ)=2i=1|ln(xi(t;ϕ)xi(t;ϕ))|+2i,j=10τjitt+θ|xi(s;ϕ)xi(s;ϕ)|dsdμji(θ). (4.2)

    By Itô's formula, we derive

    L[W(t;ϕ,ϕ)]2j=1(2ajj2i=1Aij)|xj(t;ϕ)xj(t;ϕ)|. (4.3)

    Based on (4.3), we obtain

    E[W(t;ϕ,ϕ)]E[W(0;ϕ,ϕ)]2j=1(2ajj2i=1Aij)t0E[|xj(s;ϕ)xj(s;ϕ)|]ds. (4.4)

    By (4.4), we deduce

    +0E[|xj(t;ϕ)xj(t;ϕ)|]dtE[W(0;ϕ,ϕ)]2ajj2i=1Aij(j=1,2). (4.5)

    Define Hi(t)=E[|xi(t;ϕ)xi(t;ϕ)|] (i=1,2). Then for any t1,t2[0,+),

    |Hi(t2)Hi(t1)|E[|xi(t2;ϕ)xi(t1;ϕ)|]+E[|xi(t2;ϕ)xi(t1;ϕ)|]. (4.6)

    Denote maxiSrj(i)=rj, maxiS|σj(i)|=σj, supsτCj(s)=Cj, maxiSsupμZ|γj(μ,i)|=γj. Based on Hölder's inequality, for t2>t1 and p>1, we deduce

    (E[|xj(t2)xj(t1)|])pE[|xj(t2)xj(t1)|p]3p1E[(t2t1xj(s)(rj+hj+rjjCj+2i=1Dji(xi)(s))ds)p]+3p1E[|t2t1σj(ρ(s))xj(s)dWj(s)|p]+3p1E[|t2t1Zxj(s)γj(μ,ρ(s))˜N(ds,dμ)|p]3p1Υ1+3p1Υ2+3p1Υ3(j=1,2). (4.7)

    In view of Theorem 7.1 in [54], for p2, we obtain

    Υ2(σj)p(p(p1)2)p2(t2t1)p22t2t1E[xpj(s)]ds. (4.8)

    From Hölder's inequality, we derive

    Υ17p1(rj)p(t2t1)p1t2t1E[xpj(s)]ds+7p1hpj(t2t1)p1t2t1E[xpj(s)]ds+7p1(rjjCj)p(t2t1)p1t2t1E[xpj(s)]ds+7p12i=1apji(t2t1)p1t2t1E[xpi(s)xpj(s)]ds+7p12i=1(t2t1)p1E[t2t1|0τjixi(s+θ)xj(s)dμji(θ)|pds]. (4.9)

    According to Hölder's inequality, we get

    E[t2t1(0τjixj(s)xi(s+θ)dμji(θ))pds]12(0τjidμji(θ))pt2t1E[x2pj(s)]ds+12(0τjidμji(θ))p1t2t10τjiE[x2pi(s+θ)]dμji(θ)ds. (4.10)

    According to the Kunita's first inequality in [55], for p>2, we get

    Υ3D(p){E[(t2t1Z|xj(s)γj(μ,ρ(s))|2λ(dμ)ds)p2]+E[t2t1Z|xj(s)γj(μ,ρ(s))|pλ(dμ)ds]}D(p){E[(γj)p(t2t1Zx2j(s)λ(dμ)ds)p2]+E[(γj)pt2t1Zxpj(s)λ(dμ)ds]}D(p){(γj)p(Zλ(dμ))p2|t2t1|p22t2t1E[xpj(s)]ds+(γj)pZλ(dμ)t2t1E[xpj(s)]ds}. (4.11)

    By Theorem 1 and (4.7)–(4.11), we deduce that for p>2 and |t2t1|12,

    (E[|xj(t2)xj(t1)|])pM|t2t1|, (4.12)

    where

    M1=21p1{(rj)pKj(p)+hpjKj(p)+(rjjCj)pKj(p)+2i=1[apji2+12(0τjidμji(θ))p][Ki(2p)+Kj(2p)]};M2=3p1(σj)p(p(p1)2)p2Kj(p)+3p1D(p)(γj)p(Zλ(dμ))p2Kj(p);M3=3p1D(p)(γj)pZλ(dμ)Kj(p);M=M1(12)p1+M2(12)p22+M3. (4.13)

    Combining (4.7) with (4.12) yields

    |Hj(t2)Hj(t1)|2(M|t2t1|)1p. (4.14)

    Then, for any ϵ>0, there exists δ(ϵ)=min{ϵp2pM,12} such that for any t2>t1 satisfying |t2t1|<δ(ϵ), we have |Hj(t2)Hj(t1)|<ϵ. Therefore, (4.1) follows from (4.5), (4.14) and Barbalat's conclusion in [56].

    Now, let consider the optimal harvesting problem of systems (1.7) and (1.8).

    Theorem 5. For system (1.7), define

    h1=2A11Δ1+(A12A21)Δ24A11A22(A12A21)2,h2=(A12A21)Δ1+2A22Δ24A11A22(A12A21)2,Y(H)=A22h21+(A12A21)h1h2A11h22+Δ1h1+Δ2h2. (5.1)

    (i) If

    {Θ2|h1=h10,h2=h20>0,4A11A22(A12A21)2>0, (5.2)

    then the optimal harvesting strategy exist. Moreover, H=(h1,h2)T and

    MESY=Y(H)|A|. (5.3)

    (ii) If one of the following conditions holds, then the optimal harvesting strategy does not exist:

    (a) Θ1|h1=h1<0;

    (b) Θ1|h1=h1>0>Θ2|h1=h1,h2=h2;

    (c) h1<0 or h2<0;

    (d) 4A11A22(A12A21)2<0.

    Proof. Thanks to (2.3), there exists C=2i=1Ki(p)>0 such that

    t1t0E[xp1(s)+xp2(s)]dsC. (5.4)

    By Theorem 3.1.1 in [57], (x1(t),x2(t),ρ(t))T has an invariant measure ν(×)R2+×S. From Theorem 3.1 in [58], ν(×) is unique. Thanks to Theorem 3.2.6 in [59], ν(×) is ergodic. Hence, we have

    Sk=1R2+θiν(dθ1,dθ2,k)=limt+t1t0xi(s)dsa.s.(i=1,2). (5.5)

    Let

    U={H=(h1,h2)TR2|Θ2>0,h10,h20}. (5.6)

    On the one hand, from Theorem 2 (i), for every HU, we obtain

    limt+t1t0xi(s)ds=|Ai||A|. (5.7)

    On the other hand, if the OHE H exists, then HU.

    Proof of (i). Based on the first condition of (5.2), we obtain that U is not empty. According to (5.7), for H=(h1,h2)TU, we have

    limt+t1t0HTx(s)ds=2i=1hilimt+t1t0xi(s)ds=Y(H)|A|. (5.8)

    Let ϱ(×) be the stationary probability density of system (1.7), then we get

    Y(H)=limt+E[HTx(t)]=Sk=1R2+HTθϱ(θ,k)dθ. (5.9)

    Noting that system (1.7) has a unique ergodic invariant measure ν(×) and that there exists a one-to-one correspondence between ϱ(×) and ν(×), we deduce

    Sk=1R2+HTθϱ(θ,k)dθ=Sk=1R2+HTθν(dθ,k). (5.10)

    In view of Eqs (5.5), (5.8), (5.9) and (5.10), we deduce

    Y(H)=Y(H)|A|. (5.11)

    Solving Y(H)h1=Y(H)h2=0 yields

    {h1=2A11Δ1+(A12A21)Δ24A11A22(A12A21)2,h2=(A12A21)Δ1+2A22Δ24A11A22(A12A21)2. (5.12)

    Define the Hessian matrix Λ as follows:

    Λ=(2A22A12A21A12A212A11). (5.13)

    Thanks to 2A22<0 and 4A11A22(A12A21)2>0, Λ is negative definite. Thus, Y(H) has a unique maximum, and the unique maximum value point of Y(H) is H=(h1,h2)T. Hence, (5.3) follows from (5.11).

    Proof of (ii). First, from Theorem 2 (iii), under condition (a), the optimal harvesting strategy does not exist. Next, let us show that the optimal harvesting strategy does not exist, provided that either (b) or (c) holds. The proof is by contradiction. Suppose that the OHE is ~H=(~h1,~h2)T. Then ~HU. In other words, we have

    Θ2|h1=~h1,h2=~h2>0,~h10,~h20. (5.14)

    On the other hand, since ~H=(~h1,~h2)TU is the OHE, then (~h1,~h2)T must be the unique solution to system Y(H)h1=Y(H)h2=0. Hence, (h1,h2)T=(~h1,~h2)T. Therefore, the Eq (5.14) becomes

    Θ2|h1=h1,h2=h2>0,h10,h20, (5.15)

    which contradicts with both (b) and (c).

    Now we are in the position to prove that if the following condition holds, then the optimal harvesting strategy does not exist (i.e., prove (d)):

    {Θ2|h1=h10,h2=h20>0,4A11A22(A12A21)2<0. (5.16)

    From the first condition of (5.16), we obtain that U is not empty. Hence (5.11) is true. 2A22<0 implies that Λ is not positive semidefinite. The second condition of (5.16) indicates that Λ is not negative semidefinite. Namely, Λ is indefinite. Thus, Y(H) does not exist extreme point. So the OHE does not exist.

    The proof is complete.

    Remark 7. If S={1}, rii=0, γi(μ,1)=0, μii(θ) are constant functions defined on [τ,0], aij=0 (ij) and μij(θ) are defined as follows:

    μ12(θ)={a12,τ12θ0,0,τ12θ<τ12,μ21(θ)={a21,τ21θ0,0,τ21θ<τ21,

    then system (1.7) becomes

    {dx1(t)=x1(t)[(r1h1a11x1(t)a12x2(tτ12))dt+σ1dW1(t)],dx2(t)=x2(t)[(r2h2+a21x1(tτ21)a22x2(t))dt+σ2dW2(t)]. (5.17)

    Hence, Theorem 5 contains Theorem 1 in [60] as a special case.

    Remark 8. If rii=0, γi(μ,ρ(t))=0, μii(θ) are constant functions defined on [τ,0] and aij=0 (ij), then system (1.7) becomes

    {dx1(t)=x1(t)[(r1(ρ(t))h1a11x1(t)0τ12x2(t+θ)dμ12(θ))dt+σ1(ρ(t))dW1(t)],dx2(t)=x2(t)[(r2(ρ(t))h2+0τ21x1(t+θ)dμ21(θ)a22x2(t))dt+σ2(ρ(t))dW2(t)]. (5.18)

    Therefore, Theorem 2 and Theorem 5 contains, respectively, Theorem 1 and Theorem 2 in [12] as a special case.

    Theorem 6. For system (1.8), define

    h1=2A11Γ1+(A12+A21)Γ24A11A22(A12+A21)2,h2=(A12+A21)Γ1+2A22Γ24A11A22(A12+A21)2,Y(H)=A22h21+(A12+A21)h1h2A11h22+Γ1h1+Γ2h2. (5.19)

    (A1) If

    4A11A22(A12+A21)2>0,Δi|h1=h10,h2=h20>0(i=1,2), (5.20)

    then the optimal harvesting strategy exists. Moreover, H=(h1,h2)T and

    MESY=Y(H)Δ. (5.21)

    (A2) If one of the following conditions holds, then the optimal harvesting strategy does not exist:

    (B1) Ξ1|h1=h1<0, Ξ2|h2=h2<0;

    (B2) Ξ1|h1=h1<0, Ξ2|h2=h20;

    (B3) Ξ1|h1=h10, Ξ2|h2=h2<0;

    (B4) Δ0, Δ1|h1=h1,h2=h2<0, Ξ2|h2=h2<0;

    (B5) Δ0, Δ2|h1=h1,h2=h2<0, Ξ1|h1=h1<0;

    (B6) Δ0, Δ1|h1=h1,h2=h2<0, Ξ2|h2=h20;

    (B7) Δ0, Δ2|h1=h1,h2=h2<0, Ξ1|h1=h10;

    (B8) h1<0 or h2<0;

    (B9) 4A11A22(A12+A21)2<0.

    Proof. The proof of Theorem 6 is similar to that of Theorem 5 and hence is omitted.

    Remark 9. If S={1}, rii=0, μii(θ) are constant functions defined on [τ,0], aij=0 (ij) and μij(θ) are defined as follows:

    μ12(θ)={a12,τ12θ0,0,τ12θ<τ12,μ21(θ)={a21,τ21θ0,0,τ21θ<τ21,

    then system (1.8) becomes

    {dx1(t)=x1(t)[(r1h1a11x1(t)a12x2(tτ12))dt+S1(t)],dx2(t)=x2(t)[(r2h2a21x1(tτ21)a22x2(t))dt+S2(t)]. (5.22)

    Hence, Theorem 3 and Theorem 6 contain, respectively, Lemma 2.3 and Theorem 4.1 in [47] as a special case.

    In this paper, we study the stochastic dynamics of two hybrid delay Lotka-Volterra systems with harvesting and jumps in a polluted environment. The main results include five theorems. Theorem 2 and Theorem 3 establish sufficient and necessary conditions for persistence in mean and extinction of each species. In Theorem 4, sufficient conditions for global attractivity of the systems are obtained. Theorems 5 and 6 provide sufficient and necessary conditions for the existence of optimal harvesting strategy. Furthermore, we obtain the accurate expressions for the OHE and MESY in Theorems 5 and 6. Our results show that the dynamic behaviors and optimal harvesting strategy are closely correlated with both time delays and environmental noises.

    Some interesting questions deserve further investigation. On the one hand, it would be interesting to consider the stochastic hybrid delay food chain model with harvesting and jumps in a polluted environment. On the other hand, it is interesting to investigate the influences of impulsive perturbations on the systems. One may also propose some more realistic systems, such as considering the generalized functional response. We will leave these investigations for future work.

    This work is supported by National Natural Science Foundation of China (No. 11901166).

    The authors declare that there are no conflicts of interest.



    [1] X. Zou, K. Wang, Optimal harvesting for a stochastic regime-switching logistic diffusion system with jumps, Nonlinear Anal. Hybrid Syst., 13 (2014), 32–44. https://doi.org/10.1016/j.nahs.2014.01.001 doi: 10.1016/j.nahs.2014.01.001
    [2] J. Roy, D. Barman, S. Alam, Role of fear in a predator-prey system with ratio-dependent functional response in deterministic and stochastic environment, Biosystems, 197 (2020), 104176. https://doi.org/10.1016/j.biosystems.2020.104176 doi: 10.1016/j.biosystems.2020.104176
    [3] Q. Liu, D. Jiang, Influence of the fear factor on the dynamics of a stochastic predator-prey model, Appl. Math. Lett., 112 (2021), 106756. https://doi.org/10.1016/j.aml.2020.106756 doi: 10.1016/j.aml.2020.106756
    [4] Q. Yang, X. Zhang, D. Jiang, Dynamical behaviors of a stochastic food chain system with Ornstein-Uhlenbeck process, J. Nonlinear Sci., 32 (2022), 1–40. https://doi.org/10.1007/s00332-021-09760-y doi: 10.1007/s00332-021-09760-y
    [5] L. Wang, D. Jiang, Ergodicity and threshold behaviors of a predator-prey model in stochastic chemostat driven by regime switching, Math. Meth. Appl. Sci., 44 (2021), 325–344. https://doi.org/10.1002/mma.6738 doi: 10.1002/mma.6738
    [6] Q. Luo, X. Mao, Stochastic population dynamics under regime switching, J. Math. Anal. Appl., 334 (2007), 69–84. https://doi.org/10.1016/j.jmaa.2006.12.032 doi: 10.1016/j.jmaa.2006.12.032
    [7] Q. Luo, X. Mao, Stochastic population dynamics under regime switching Ⅱ, J. Math. Anal. Appl., 355 (2009), 577–593. https://doi.org/10.1016/j.jmaa.2009.02.010 doi: 10.1016/j.jmaa.2009.02.010
    [8] C. Zhu, G. Yin, On hybrid competitive Lotka-Volterra ecosystems, Nonlinear Anal., 71 (2009), 1370–1379. https://doi.org/10.1016/j.na.2009.01.166 doi: 10.1016/j.na.2009.01.166
    [9] X. Li, A. Gray, D. Jiang, X. Mao, Sufficient and necessary conditions of stochastic permanence and extinction for stochastic logistic populations under regime switching, J. Math. Anal. Appl., 376 (2011), 11–28. https://doi.org/10.1016/j.jmaa.2010.10.053 doi: 10.1016/j.jmaa.2010.10.053
    [10] M. Ouyang, X. Li, Permanence and asymptotical behavior of stochastic prey-predator system with Markovian switching, Appl. Math. Comput., 266 (2015), 539–559. https://doi.org/10.1016/j.amc.2015.05.083 doi: 10.1016/j.amc.2015.05.083
    [11] J. Bao, J. Shao, Permanence and extinction of regime-switching predator-prey models, SIAM J. Math. Anal., 48 (2016), 725–739. https://doi.org/10.1137/15M1024512 doi: 10.1137/15M1024512
    [12] M. Liu, X. He, J. Yu, Dynamics of a stochastic regime-switching predator-prey model with harvesting and distributed delays, Nonlinear Anal. Hybrid Syst., 28 (2018), 87–104. https://doi.org/10.1016/j.nahs.2017.10.004 doi: 10.1016/j.nahs.2017.10.004
    [13] Y. Cai, S. Cai, X. Mao, Stochastic delay foraging arena predator-prey system with Markov switching, Stoch. Anal. Appl., 38 (2020), 191–212. https://doi.org/10.1080/07362994.2019.1679645 doi: 10.1080/07362994.2019.1679645
    [14] J. Bao, X. Mao, G. Yin, C. Yuan, Competitive Lotka-Volterra population dynamics with jumps, Nonlinear Anal., 74 (2011), 6601–6616. https://doi.org/10.1016/j.na.2011.06.043 doi: 10.1016/j.na.2011.06.043
    [15] J. Bao, C. Yuan, Stochastic population dynamics driven by Lévy noise, J. Math. Anal. Appl., 391 (2012), 363–375. https://doi.org/10.1016/j.jmaa.2012.02.043 doi: 10.1016/j.jmaa.2012.02.043
    [16] M. Liu, K. Wang, Dynamics of a Leslie-Gower Holling-type Ⅱ predator-prey system with Lévy jumps, Nonlinear Anal., 85 (2013), 204–213. https://doi.org/10.1016/j.na.2013.02.018 doi: 10.1016/j.na.2013.02.018
    [17] M. Liu, K. Wang, Stochastic Lotka-Volterra systems with Lévy noise, J. Math. Anal. Appl., 410 (2014), 750–763. https://doi.org/10.1016/j.jmaa.2013.07.078 doi: 10.1016/j.jmaa.2013.07.078
    [18] M. Liu, M. Deng, B. Du, Analysis of a stochastic logistic model with diffusion, Appl. Math. Comput., 266 (2015), 169–182. https://doi.org/10.1016/j.amc.2015.05.050 doi: 10.1016/j.amc.2015.05.050
    [19] X. Zhang, W. Li, M. Liu, K. Wang, Dynamics of a stochastic Holling Ⅱ one-predator two-prey system with jumps, Phys. A, 421 (2015), 571–582. https://doi.org/10.1016/j.physa.2014.11.060 doi: 10.1016/j.physa.2014.11.060
    [20] D. Valenti, G. Denaro, A. Cognata, B. La Spagnolo, A. Bonanno, G. Basilone, et al., Picophytoplankton dynamics in noisy marine environment, Acta Phys. Pol. B, 43 (2012), 1227–1240. https://doi.org/10.5506/APhysPolB.43.1227 doi: 10.5506/APhysPolB.43.1227
    [21] C. Guarcello, D. Valenti, G. Augello, B. Spagnolo, The role of non-Gaussian sources in the transient dynamics of long Josephson junctions, Acta Phys. Pol. B, 44 (2013), 997–1005. https://doi.org/10.5506/APhysPolB.44.997 doi: 10.5506/APhysPolB.44.997
    [22] C. Guarcello, D. Valenti, B. Spagnolo, V. Pierro, G. Filatrella, Josephson-based threshold detector for Lévy-distributed current fluctuations, Phys. Rev. Appl., 11 (2019), 044078. https://doi.org/10.1103/PhysRevApplied.11.044078 doi: 10.1103/PhysRevApplied.11.044078
    [23] A. A. Dubkov, A. La Cognata, B. Spagnolo, The problem of analytical calculation of barrier crossing characteristics for Lévy flights, J. Stat. Mech. Theory Exp., 2009 (2019), P01002. https://doi.org/10.1088/1742-5468/2009/01/P01002 doi: 10.1088/1742-5468/2009/01/P01002
    [24] B. Lisowski, D. Valenti, B. Spagnolo, M. Bier, E. Gudowska-Nowak, Stepping molecular motor amid Lévy white noise, Phys. Rev. E, 91 (2015), 042713. https://doi.org/10.1103/PhysRevE.91.042713 doi: 10.1103/PhysRevE.91.042713
    [25] I. A. Surazhevsky, V. A. Demin, A. I. Ilyasov, A. V. Emelyanov, K. E. Nikiruy, V. V. Rylkov, et al., Noise-assisted persistence and recovery of memory state in a memristive spiking neuromorphic network, Chaos Solitons Fractals, 146 (2021), 110890. https://doi.org/10.1016/j.chaos.2021.110890 doi: 10.1016/j.chaos.2021.110890
    [26] A. N. Mikhaylov, D. V. Guseinov, A. I. Belov, D. S. Korolev, V. A. Shishmakova, M. N. Koryazhkina, et al., Stochastic resonance in a metal-oxide memristive device, Chaos Solitons Fractal, 144 (2021), 110723. https://doi.org/10.1016/j.chaos.2021.110723 doi: 10.1016/j.chaos.2021.110723
    [27] Y. V. Ushakov, A. A. Dubkov, B. Spagnolo, Spike train statistics for consonant and dissonant musical accords in a simple auditory sensory model, Phys. Rev. E, 81 (2010), 041911. https://doi.org/10.1103/PhysRevE.81.041911 doi: 10.1103/PhysRevE.81.041911
    [28] N. V. Agudov, A. V. Safonov, A. V. Krichigin, A. A. Kharcheva, A. A. Dubkov, D. Valenti, et al., Nonstationary distributions and relaxation times in a stochastic model of memristor, J. Stat. Mech. Theory Exp., 2020 (2020), 024003. https://doi.org/10.1088/1742-5468/ab684a doi: 10.1088/1742-5468/ab684a
    [29] D. O. Filatov, D. V. Vrzheshch, O. V. Tabakov, A. S. Novikov, A. I. Belov, I. N. Antonov, et al., Noise-induced resistive switching in a memristor based on ZrO2(Y)/Ta2O5 stack, J. Stat. Mech. Theory Exp., 2019 (2019), 124026. https://doi.org/10.1088/1742-5468/ab5704 doi: 10.1088/1742-5468/ab5704
    [30] A. Carollo, B. Spagnolo, A. A. Dubkov, D. Valenti, On quantumness in multi-parameter quantum estimation, J. Stat. Mech. Theory Exp., 2019 (2019), 094010. https://doi.org/10.1088/1742-5468/ab3ccb doi: 10.1088/1742-5468/ab3ccb
    [31] R. Stassi, S. Savasta, L. Garziano, B. Spagnolo, F. Nori, Output field-quadrature measurements and squeezing in ultrastrong cavity-QED, New J. Phys., 18 (2016), 123005. https://doi.org/10.1088/1367-2630/18/12/123005 doi: 10.1088/1367-2630/18/12/123005
    [32] S. Ciuchi, F. De Pasquale, B. Spagnolo, Nonlinear relaxation in the presence of an absorbing barrier, Phys. Rev. E, 47 (1993), 3915. https://doi.org/10.1103/PhysRevE.47.3915 doi: 10.1103/PhysRevE.47.3915
    [33] Y. Kuang, Delay Differential Equations: With Applications in Population Dynamics, Academic Press, Boston, 1993.
    [34] W. Zuo, D. Jiang, X. Sun, T. Hayat, A. Alsaedi, Long-time behaviors of a stochastic cooperative Lotka-Volterra system with distributed delay, Phys. A, 506 (2018), 542–559. https://doi.org/10.1016/j.physa.2018.03.071 doi: 10.1016/j.physa.2018.03.071
    [35] F. A. Rihan, H. J. Alsakaji, Stochastic delay differential equations of three-species prey-predator system with cooperation among prey species, Discret. Contin. Dyn. Syst. Ser. S, 15 (2020), 245. https://doi.org/10.3934/dcdss.2020468 doi: 10.3934/dcdss.2020468
    [36] H. J. Alsakaji, S. Kundu, F. A. Rihan, Delay differential model of one-predator two-prey system with Monod-Haldane and holling type Ⅱ functional responses, Appl. Math. Comput., 397 (2021), 125919. https://doi.org/10.1016/j.amc.2020.125919 doi: 10.1016/j.amc.2020.125919
    [37] L. Wang, R. Zhang, Y. Wang, Global exponential stability of reaction-diffusion cellular neural networks with S-type distributed time delays, Nonlinear Anal., 10 (2009), 1101–1113. https://doi.org/10.1016/j.nonrwa.2007.12.002 doi: 10.1016/j.nonrwa.2007.12.002
    [38] L. Wang, D. Xu, Global asymptotic stability of bidirectional associative memory neural networks with S-type distributed delays, Int. J. Syst. Sci., 338 (2002), 869–877. https://doi.org/10.1080/00207720210161777 doi: 10.1080/00207720210161777
    [39] S. Abbas, D. Bahuguna, M. Banerjee, Effect of stochastic perturbation on a two species competitive model, Nonlinear Anal. Hybrid Syst., 3 (2009), 195–206. https://doi.org/10.1016/j.nahs.2009.01.001 doi: 10.1016/j.nahs.2009.01.001
    [40] Q. Han, D. Jiang, C. Ji, Analysis of a delayed stochastic predator-prey model in a polluted environment, Appl. Math. Model., 38 (2014), 3067–3080. https://doi.org/10.1016/j.apm.2013.11.014 doi: 10.1016/j.apm.2013.11.014
    [41] Q. Liu, Q. Chen, Analysis of a stochastic delay predator-prey system with jumps in a polluted environment, Appl. Math. Comput., 242 (2014), 90–100. https://doi.org/10.1016/j.amc.2014.05.033 doi: 10.1016/j.amc.2014.05.033
    [42] Y. Zhao, S. Yuan, Optimal harvesting policy of a stochastic two-species competitive model with Lévy noise in a polluted environment, Phys. A, 477 (2017), 20–33. https://doi.org/10.1016/j.physa.2017.02.019 doi: 10.1016/j.physa.2017.02.019
    [43] M. Liu, X. He, J. Yu, Dynamics of a stochastic regime-switching predator-prey model with harvesting and distributed delays, Nonlinear Anal. Hybrid Syst., 28 (2018), 87–104. https://doi.org/10.1016/j.nahs.2017.10.004 doi: 10.1016/j.nahs.2017.10.004
    [44] M. Liu, C. Bai, Dynamics of a stochastic one-prey two-predator model with Lévy jumps, Appl. Math. Comput., 284 (2016), 308–321. https://doi.org/10.1016/j.amc.2016.02.033 doi: 10.1016/j.amc.2016.02.033
    [45] Y. Zhao, L. You, D. Burkow, S. Yuan, Optimal harvesting strategy of a stochastic inshore-offshore hairtail fishery model driven by Lévy jumps in a polluted environment, Nonlinear Dyn., 95 (2019), 1529–1548. https://doi.org/10.1007/s11071-018-4642-y doi: 10.1007/s11071-018-4642-y
    [46] Q. Liu, D. Jiang, N. Shi, T. Hayat, A. Alsaedi, Stochastic mutualism model with Lévy jumps, Commun. Nonlinear Sci. Numer. Simul., 43 (2017), 78–90. https://doi.org/10.1016/j.cnsns.2016.05.003 doi: 10.1016/j.cnsns.2016.05.003
    [47] H. Qiu, W. Deng, Optimal harvesting of a stochastic delay competitive Lotka-Volterra model with Lévy jumps, Appl. Math. Comput., 317 (2018), 210–222. https://doi.org/10.1016/j.amc.2017.08.044 doi: 10.1016/j.amc.2017.08.044
    [48] M. Liu, K. Wang, Survival analysis of stochastic single-species population models in polluted environments, Ecol. Model., 220 (2009), 1347–1357. https://doi.org/10.1016/j.ecolmodel.2009.03.001 doi: 10.1016/j.ecolmodel.2009.03.001
    [49] G. Liu, X. Meng, Optimal harvesting strategy for a stochastic mutualism system in a polluted environment with regime switching, Phys. A, 536 (2019), 120893. https://doi.org/10.1016/j.physa.2019.04.129 doi: 10.1016/j.physa.2019.04.129
    [50] S. Wang, L. Wang, T. Wei, Optimal harvesting for a stochastic logistic model with S-type distributed time delay, J. Differ. Equation Appl., 23 (2017), 618–632. https://doi.org/10.1080/10236198.2016.1269761 doi: 10.1080/10236198.2016.1269761
    [51] M. Liu, K. Wang, Q. Wu, Survival analysis of stochastic competitive models in a polluted environment and stochastic competitive exclusion principle, Bull. Math. Biol., 73 (2011), 1969–2012. https://doi.org/10.1007/s11538-010-9569-5 doi: 10.1007/s11538-010-9569-5
    [52] M. Liu, C. Bai, On a stochastic delayed predator-prey model with Lévy jumps, Appl. Math. Comput., 228 (2014), 563–570. https://doi.org/10.1016/j.amc.2013.12.026 doi: 10.1016/j.amc.2013.12.026
    [53] Q. Liu, Q. Chen, Z. Liu, Analysis on stochastic delay Lotka-Volterra systems driven by Lévy noise, Appl. Math. Comput., 235 (2014), 261–271. https://doi.org/10.1016/j.amc.2014.03.011 doi: 10.1016/j.amc.2014.03.011
    [54] X. Mao, Stochastic Differential Equations and Applications, Horwood Publishing Limited, 2007. https://doi.org/10.1533/9780857099402
    [55] D. Applebaum, Lévy Processes and Stochastic Calculus, Cambridge University Press, 2009. https://doi.org/10.1017/CBO9780511809781
    [56] I. Barbalat, Systems dequations differentielles d'osci d'oscillations, Rev. Roumaine Math. Pures Appl., 4 (1959), 267–270.
    [57] M. Kinnally, R. Williams, On existence and uniqueness of stationary distributions for stochastic delay differential equations with positivity constraints, Electron. J. Probab., 15 (2010), 409–451. https://doi.org/10.1214/EJP.v15-756 doi: 10.1214/EJP.v15-756
    [58] M. Hairer, J. C. Mattingly, M. Scheutzow, Asymptotic coupling and a general form of Harris' theorem with applications to stochastic delay equations, Probab. Theory Related Fields, 149 (2011), 223–259. https://doi.org/10.1007/s00440-009-0250-6 doi: 10.1007/s00440-009-0250-6
    [59] G. Prato, J. Zabczyk, Ergodicity for Infinite Dimensional Systems, Cambridge University Press, 1996.
    [60] M. Liu, Optimal harvesting policy of a stochastic predator-prey model with time delay, Appl. Math. Lett., 48 (2015), 102–108. https://doi.org/10.1016/j.aml.2014.10.007 doi: 10.1016/j.aml.2014.10.007
  • This article has been cited by:

    1. Liwen He, Zilin Cong, Yanjing Cai, Analyzing Lamprey Population Growth and Sex Ratio Evolution Through Cellular Automata and Impact of Predation Efficiency and Sex Ratio on Lamprey Populations, 2024, 4, 2960-2319, 222, 10.62051/4wbwpw76
  • Reader Comments
  • © 2023 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(1777) PDF downloads(120) Cited by(1)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog