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Research article

Stochastic persistence and global attractivity of a two-predator one-prey system with S-type distributed time delays

  • Received: 14 October 2022 Revised: 25 November 2022 Accepted: 07 December 2022 Published: 27 December 2022
  • In this paper, well-posedness and asymptotic behaviors of a stochastic two-predator one-prey system with S-type distributed time delays are studied by using stochastic analytical techniques. First, the existence and uniqueness of global positive solution with positive initial condition is proved. Second, sufficient conditions for persistence in mean and extinction of each species are obtained. Then, sufficient conditions for global attractivity are established. Finally, some numerical simulations are provided to support the analytical results.

    Citation: Zeyan Yue, Lijuan Dong, Sheng Wang. Stochastic persistence and global attractivity of a two-predator one-prey system with S-type distributed time delays[J]. Mathematical Modelling and Control, 2022, 2(4): 272-281. doi: 10.3934/mmc.2022026

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  • In this paper, well-posedness and asymptotic behaviors of a stochastic two-predator one-prey system with S-type distributed time delays are studied by using stochastic analytical techniques. First, the existence and uniqueness of global positive solution with positive initial condition is proved. Second, sufficient conditions for persistence in mean and extinction of each species are obtained. Then, sufficient conditions for global attractivity are established. Finally, some numerical simulations are provided to support the analytical results.



    In 1977 and 1984, Freedman and Waltman ([1,2]) studied the following two-predator one-prey system:

    {dx1(t)dt=x1(t)[r1a11x1(t)a12x2(t)a13x3(t)],dx2(t)dt=x2(t)[r2+a21x1(t)a22x2(t)a23x3(t)],dx3(t)dt=x3(t)[r3+a31x1(t)a32x2(t)a33x3(t)], (1.1)

    where xi(t) stands for the size of the ith population and all the parameters are positive constants.

    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 [3,4,5]. Therefore, it is of enormous importance to study the effects of environmental noises on the dynamics of population systems. Assume that the parameters ri are affected by white noises, i.e., r1r1+σ1˙B1(t), r2r2+σ2˙B2(t), r3r3+σ3˙B3(t), where Bi(t) are mutually independent standard Wiener processes defined on a complete probability space (Ω,F,P) with a filtration {Ft}t0 satisfying the usual conditions. Then, the stochastic two-predator one-prey system with white noises can be expressed as follows:

    {dx1(t)=x1(t)[r1a11x1(t)a12x2(t)a13x3(t)]dt+σ1x1(t)dB1(t),dx2(t)=x2(t)[r2+a21x1(t)a22x2(t)a23x3(t)]dt+σ2x2(t)dB2(t),dx3(t)=x3(t)[r3+a31x1(t)a32x2(t)a33x3(t)]dt+σ3x3(t)dB3(t). (1.2)

    On the other hand, "all species should exhibit time delay" in the real world, and incorporating time delays in biological systems makes the systems much more realistic than those without time delays ([6,7,8,9,10]). Hence, in this paper we concern the dynamics of the following stochastic two-predator one-prey system with S-type distributed time delays:

    {dx1(t)=x1(t)[r1D11(x1)(t)D12(x2)(t)D13(x3)(t)]dt+σ1x1(t)dB1(t),dx2(t)=x2(t)[r2+D21(x1)(t)D22(x2)(t)D23(x3)(t)]dt+σ2x2(t)dB2(t),dx3(t)=x3(t)[r3+D31(x1)(t)D32(x2)(t)D33(x3)(t)]dt+σ3x3(t)dB3(t), (1.3)

    where Dji(xi)(t)=ajixi(t)+0τjixi(t+θ)dμji(θ), 0τjixi(t+θ)dμji(θ) are Lebesgue-Stieltjes integrals, τji>0 are time delays, μji(θ) are nondecreasing bounded variation functions defined on [τ,0], τ=maxi,j=1,2,3{τji}.

    Denote Aij=aij+0τijdμij(θ), D1=r1σ212, Di=ri+σ2i2 (i=2,3) and

    {Θ=|A11A12A13A21A22A23A31A32A33|,Θ1=|D1A12A13D2A22A23D3A32A33|,Θ2=|A11D1A13A21D2A23A31D3A33|,Θ3=|A11A12D1A21A22D2A31A32D3|.

    Assume that Θ>0. For the matrix corresponding to Θ (respectively, Θk), denote by MΘij (respectively, MΘkij) the complement minor of the element at the i-th row and the j-th column (i,j,k=1,2,3).

    Theorem 2.1. For any (ξ1,ξ2,ξ3)TC([τ,0],R3+), system (1.3) has a unique global solution (x1(t),x2(t),x3(t))TR3+ on t[0,+) a.s. Moreover, for any constant p>0, there are Ki(p)>0 such that

    supt0E[xpi(t)]Ki(p)(i=1,2,3). (2.1)

    Proof. The proof is rather standard and here is omitted (see, e.g., [11] and [12]).

    Lemma 2.1. ([13]) Suppose Z(t)C(Ω×[0,+),R+) and limt+o(t)t=0.

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

    lnZ(t)δtδ0t0Z(s)ds+o(t), (2.2)

    then

    {lim supt+t1t0Z(s)dsδδ0a.s.(δ0);limt+Z(t)=0a.s.(δ<0). (2.3)

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

    lnZ(t)δtδ0t0Z(s)ds+o(t), (2.4)

    then

    lim inft+t1t0Z(s)dsδδ0a.s. (2.5)

    Lemma 2.2. Consider the following auxiliary system:

    {dX1(t)=X1(t)[r1D11(X1)(t)]dt+σ1X1(t)dB1(t),dXi(t)=Xi(t)[ri+Di1(X1)(t)Dii(Xi)(t)]dt+σiXi(t)dBi(t),(i=2,3). (2.6)

    (a) If D1<0, then limt+Xi(t)=0 a.s. (i=1,2,3).

    (b) If D10, Di+Ai1D1A11<0, then

    limt+t1t0X1(s)ds=D1A11,limt+Xi(t)=0a.s.(i=2,3).

    (c) If D10, Di+Ai1D1A110, then

    limt+t1t0X1(s)ds=D1A11,limt+t1t0Xi(s)ds=A1ii(Di+Ai1D1A11)a.s.(i=2,3).

    Proof. By Itô's formula, we have

    {lnX1(t)=D1tA11t0X1(s)dsT11(X1)(t)+o(t),lnXi(t)=Dit+Ai1t0X1(s)dsAiit0Xi(s)ds+Ti1(X1)(t)Tii(Xi)(t)+o(t),(i=2,3), (2.7)

    where

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

    Case(i): D1<0. Then limt+X1(t)=0 a.s. Hence, for ϵ(0,Di2) and t1,

    lnXi(t)(Di+ϵ)taiit0Xi(s)ds,(i=2,3). (2.8)

    So, limt+Xi(t)=0 a.s. (i=2,3).

    Case(ii): D10. Then,

    limt+t1t0X1(s)ds=D1A11a.s. (2.9)

    Consider the following SDDE:

    d~Xi(t)=~Xi(t)(ri+Di1(X1)(t)aii~Xi(t))dt+σi~Xi(t)dBi(t),(i=2,3).

    Then, Xi(t)~Xi(t) a.s. (i=2,3). By Itô's formula,

    ln~Xi(t)=(Di+Ai1D1A11)taiit0~Xi(s)ds+o(t).

    In view of Lemma 2.1, we obtain:

    (1) If D10, Di+Ai1D1A11<0, then limt+~Xi(t)=0 a.s. (i=2,3).

    (2) If D10, Di+Ai1D1A110, then

    limt+t1t0~Xi(s)ds=a1ii(Di+Ai1D1A11)a.s.(i=2,3).

    Therefore, for arbitrary constant γ>0,

    limt+t1ttγXi(s)ds=0a.s.(i=1,2,3). (2.10)

    Based on (2.10) and system (2.7), for i=2,3,

    lnXi(t)=(Di+Ai1D1A11)tAiit0Xi(s)ds+o(t).

    Thanks to Lemma 2.1, we obtain:

    (1) If D10, Di+Ai1D1A11<0, then limt+Xi(t)=0 a.s. (i=2,3).

    (2) If D10, Di+Ai1D1A110, then

    limt+t1t0Xi(s)ds=A1ii(Di+Ai1D1A11)a.s.(i=2,3).

    Therefore, the desired assertion (b) follows from combining (2.9) with (1), and (c) follows from combining (2.9) with (2).

    Lemma 2.3. For system (1.3), lim supt+t1lnxi(t)0 a.s. (i=1,2,3).

    Proof. Thanks to Lemma 2.2 and (2.7), system (2.6) satisfies limt+t1lnXi(t)=0 a.s. (i=1,2,3). From the stochastic comparison theorem, we obtain the desired assertion.

    Theorem 2.2. For system (1.3):

    (i) If D1<0, then limt+xi(t)=0 a.s. (i=1,2,3).

    (ii) If D10, MΘ233<0, MΘ322<0, then

    limt+t1t0x1(s)ds=D1A11,limt+xi(t)=0a.s.(i=2,3).

    (iii) If D10, MΘ130, Θ3<0, MΘ233>0, then

    limt+t1t0xi(s)ds=MΘi33MΘ33,limt+x3(t)=0a.s.(i=1,2).

    (iv) If Θ1>0, Θ2>0, Θ3>0, MΘ11>0, then

    limt+t1t0xi(s)ds=ΘiΘa.s.(i=1,2,3).

    (v) If D10, MΘ120, Θ2<0, MΘ322<0, then

    limt+t1t0x1(s)ds=D1A11,limt+xi(t)=0a.s.(i=2,3).

    (vi) If D10, MΘ120, Θ2<0, MΘ3220, then

    limt+t1t0xi(s)ds=MΘi22MΘ22,limt+x2(t)=0a.s.(i=1,3).

    Proof. According to (2.10), for arbitrary constant γ>0,

    limt+t1ttγxi(s)ds=0a.s.(i=1,2,3). (2.11)

    By Itô's formula and (2.11), we derive

    {lnx1(t)=D1tA11t0x1(s)dsA12t0x2(s)dsA13t0x3(s)ds+o(t),lnx2(t)=D2t+A21t0x1(s)dsA22t0x2(s)dsA23t0x3(s)ds+o(t),lnx3(t)=D3t+A31t0x1(s)dsA32t0x2(s)dsA33t0x3(s)ds+o(t). (2.12)

    Case(i): D1<0. From Lemma 2.2 (a), limt+xi(t)=0 a.s. (i=1,2,3).

    Case(ii): D10, MΘ233<0, MΘ322<0. Based on system (2.12), for ϵ(0,1) and t1,

    lnx1(t)(D1+ϵ)tA11t0x1(s)ds. (2.13)

    By Lemma 2.1 and the arbitrariness of ϵ, we obtain

    lim supt+t1t0x1(s)dsD1A11a.s. (2.14)

    Hence, for ϵ(0,1) and t1,

    {lnx2(t)(MΘ233A11+ϵ)tA22t0x2(s)ds,lnx3(t)(MΘ322A11+ϵ)tA33t0x3(s)ds. (2.15)

    According to Lemma 2.1 and the arbitrariness of ϵ, we have

    limt+xi(t)=0a.s.(i=2,3). (2.16)

    Based on (2.16) and system (2.12), for ϵ(0,1) and t1,

    {lnx1(t)(D1+ϵ)tA11t0x1(s)ds,lnx1(t)(D1ϵ)tA11t0x1(s)ds. (2.17)

    In view of Lemma 2.1 and the arbitrariness of ϵ, we obtain

    limt+t1t0x1(s)ds=D1A11a.s. (2.18)

    Case(iii): D10, MΘ130, Θ3<0, MΘ233>0. Compute

    MΘ13lnx1(t)MΘ23lnx2(t)+MΘ33lnx3(t)=Θ3tΘt0x3(s)ds+o(t).

    By Lemma 2.3, for ϵ(0,1) and t1,

    MΘ33lnx3(t)(Θ3+ϵ)tΘt0x3(s)ds. (2.19)

    From Lemma 2.1 and the arbitrariness of ϵ, we deduce

    limt+x3(t)=0a.s. (2.20)

    By (2.20) and system (2.12), for ϵ(0,1) and t1,

    {lnx1(t)(D1+ϵ)tA11t0x1(s)dsA12t0x2(s)ds,lnx1(t)(D1ϵ)tA11t0x1(s)dsA12t0x2(s)ds,lnx2(t)(D2+ϵ)t+A21t0x1(s)dsA22t0x2(s)ds,lnx2(t)(D2ϵ)t+A21t0x1(s)dsA22t0x2(s)ds. (2.21)

    According to (2.21), for ϵ(0,1) and t1,

    A21lnx1(t)+A11lnx2(t)[MΘ233(A11+A21)ϵ]tMΘ33t0x2(s)ds,A22lnx1(t)A12lnx2(t)[MΘ133+(A12+A22)ϵ]tMΘ33t0x1(s)ds.

    Thanks to Lemma 2.3, for ϵ(0,1) and t1,

    A11lnx2(t)[MΘ233(A11+2A21)ϵ]tMΘ33t0x2(s)ds,A22lnx1(t)[MΘ133+(2A12+A22)ϵ]tMΘ33t0x1(s)ds.

    In view of Lemma 2.1 and the arbitrariness of ϵ, we obtain

    lim inft+t1t0x2(s)dsMΘ233MΘ33a.s. (2.22a)
    lim supt+t1t0x1(s)dsMΘ133MΘ33a.s. (2.22b)

    Thanks to (2.21) and (2.22b), for ϵ(0,1) and t1,

    lnx2(t)(A22MΘ233MΘ33+2ϵ)tA22t0x2(s)ds. (2.23)

    Based on Lemma 2.1 and the arbitrariness of ϵ, we obtain

    lim supt+t1t0x2(s)dsMΘ233MΘ33a.s. (2.24)

    Combining (2.22-1) with (2.24) yields

    limt+t1t0x2(s)ds=MΘ233MΘ33a.s. (2.25)

    From (2.21) and (2.25), for ϵ(0,1) and t1,

    lnx1(t)(A11MΘ133MΘ332ϵ)tA11t0x1(s)ds. (2.26)

    Thanks to Lemma 2.1 and the arbitrariness of ϵ, we have

    lim inft+t1t0x1(s)dsMΘ133MΘ33a.s. (2.27)

    Combining (2.22-2) with (2.27) yields

    limt+t1t0x1(s)ds=MΘ133MΘ33a.s. (2.28)

    Case(iv): Θ1>0, Θ2>0, Θ3>0, MΘ11>0. According to Lemma 2.1, (2.19) and the arbitrariness of ϵ, we obtain

    lim supt+t1t0x3(s)dsΘ3Θa.s. (2.29)

    In view of system (2.12), we compute

    MΘ11lnx1(t)MΘ21lnx2(t)+MΘ31lnx3(t)=Θ1tΘt0x1(s)ds+o(t).MΘ12lnx1(t)+MΘ22lnx2(t)MΘ32lnx3(t)=Θ2tΘt0x2(s)ds+o(t).

    Then, for ϵ(0,1) and t1,

    MΘ11lnx1(t)(Θ1+ϵ)tΘt0x1(s)ds,MΘ22lnx2(t)(Θ2+ϵ)tΘt0x2(s)ds.

    According to Lemma 2.1 and the arbitrariness of ϵ, we deduce

    lim supt+t1t0x1(s)dsΘ1Θa.s. (2.30a)
    lim supt+t1t0x2(s)dsΘ2Θa.s. (2.30b)

    Therefore, for ϵ(0,1) and t1,

    t1t0xi(s)dsΘiΘ+ϵa.s.(i=1,2,3). (2.31)

    Based on (2.31) and system (2.12), for ϵ(0,1) and t1,

    lnx1(t)(A11Θ1Θ3i=1A1iϵ)tA11t0x1(s)ds. (2.32)

    Thanks to Lemma 2.1 and the arbitrariness of ϵ, we obtain

    lim inft+t1t0x1(s)dsΘ1Θa.s. (2.33)

    Combining (2.30-1) with (2.33) yields

    limt+t1t0x1(s)ds=Θ1Θa.s. (2.34)

    According to (2.31), (2.33) and system (2.12), for ϵ(0,1) and t1,

    lnx2(t)(A22Θ2Θ3i=1A2iϵ)tA22t0x2(s)ds. (2.35)

    From Lemma 2.1 and the arbitrariness of ϵ, we have

    lim inft+t1t0x2(s)dsΘ2Θa.s. (2.36)

    Combining (2.30-2) with (2.36) yields

    limt+t1t0x2(s)ds=Θ2Θa.s. (2.37)

    Similarly, for ϵ(0,1) and t1,

    lnx3(t)(A33Θ3Θ3i=1A3iϵ)tA33t0x3(s)ds. (2.38)

    Thanks to Lemma 2.1 and the arbitrariness of ϵ, we obtain

    lim inft+t1t0x3(s)dsΘ3Θa.s. (2.39)

    Combining (2.29) with (2.39) yields

    limt+t1t0x3(s)ds=Θ3Θa.s. (2.40)

    Case(v): D10, MΘ120, Θ2<0, MΘ322<0. By Lemma 2.1, (2.30) and the arbitrariness of ϵ, we have

    limt+x2(t)=0a.s. (2.41)

    Hence, for ϵ(0,1) and t1,

    {lnx1(t)(D1+ϵ)tA11t0x1(s)dsA13t0x3(s)ds,lnx1(t)(D1ϵ)tA11t0x1(s)dsA13t0x3(s)ds,lnx3(t)(D3+ϵ)t+A31t0x1(s)dsA33t0x3(s)ds,lnx3(t)(D3ϵ)t+A31t0x1(s)dsA33t0x3(s)ds. (2.42)

    Based on (2.42), we deduce

    A33lnx1(t)A13lnx3(t)[MΘ122+(A13+A33)ϵ]tMΘ22t0x1(s)ds. (2.43)

    Therefore, for ϵ(0,1) and t1,

    A33lnx1(t)[MΘ122+(2A13+A33)ϵ]tMΘ22t0x1(s)ds. (2.44)

    In view of Lemma 2.1 and the arbitrariness of ϵ, we deduce

    lim supt+t1t0x1(s)dsMΘ122MΘ22a.s. (2.45)

    According to (2.42) and (2.45), for ϵ(0,1) and t1,

    lnx3(t)(A33MΘ322MΘ22+2ϵ)tA33t0x3(s)ds. (2.46)

    Clearly, (2.20) is true. From (2.20) and (2.42), for ϵ(0,1) and t1,

    {lnx1(t)(D1+2ϵ)tA11t0x1(s)ds,lnx1(t)(D12ϵ)tA11t0x1(s)ds. (2.47)

    In view of Lemma 2.1 and the arbitrariness of ϵ, we obtain (2.18).

    Case(vi): D10, MΘ120, Θ2<0, MΘ3220. Thanks to Lemma 2.1, (2.46) and the arbitrariness of ϵ,

    lim supt+t1t0x3(s)dsMΘ322MΘ22a.s. (2.48)

    According to (2.42) and (2.48), for ϵ(0,1) and t1,

    lnx1(t)(A11MΘ122MΘ222ϵ)tA11t0x1(s)ds. (2.49)

    Based on Lemma 2.1 and the arbitrariness of ϵ, we have

    lim inft+t1t0x1(s)dsMΘ122MΘ22a.s. (2.50)

    Combining (2.45) with (2.50) yields

    limt+t1t0x1(s)ds=MΘ122MΘ22a.s. (2.51)

    By (2.42) and (2.50), for ϵ(0,1) and t1,

    lnx3(t)(A33MΘ322MΘ222ϵ)tA33t0x3(s)ds. (2.52)

    Thanks to Lemma 2.1 and the arbitrariness of ϵ, we deduce

    lim inft+t1t0x3(s)dsMΘ322MΘ22a.s. (2.53)

    Combining (2.48) with (2.53) yields

    limt+t1t0x3(s)ds=MΘ322MΘ22a.s. (2.54)

    The proof is complete.

    Theorem 3.1. Assume that 2ajj>3i=1Aij (j=1,2,3). Let X(t;ϕ)=:(x1(t;ϕ),x2(t;ϕ),x3(t;ϕ))T be the solution to system (1.3) with initial condition ϕC([τ,0],R3+). Then, for any ϕ and ϕC([τ,0],R3+),

    limt+E[X(t;ϕ)X(t;ϕ)]=0. (3.1)

    Proof. We only need to show

    limt+E|xi(t;ϕ)xi(t;ϕ)|=0(i=1,2,3). (3.2)

    Define

    W(t;ϕ,ϕ)=3i=1|ln(xi(t;ϕ)xi(t;ϕ))|+3i,j=10τjitt+θ|xi(s;ϕ)xi(s;ϕ)|dsdμji(θ).

    From Itô's formula, we derive

    L[W(t;ϕ,ϕ)]3j=1(2ajj3i=1Aij)|xj(t;ϕ)xj(t;ϕ)|. (3.3)

    According to (3.3), we have

    E[W(t;ϕ,ϕ)]E[W(0;ϕ,ϕ)]3j=1(2ajj3i=1Aij)t0E[|xj(s;ϕ)xj(s;ϕ)|]ds,

    which implies

    +0E[|xi(t;ϕ)xi(t;ϕ)|]dt<+(i=1,2,3). (3.4)

    Define Gi(t)=E[|xi(t;ϕ)xi(t;ϕ)|] (i=1,2,3). Then,

    |Gi(t2)Gi(t1)|E[|xi(t2;ϕ)xi(t1;ϕ)|]+E[|xi(t2;ϕ)xi(t1;ϕ)|]. (3.5)

    Based on Hölder's inequality, for t2>t1 and p>1,

    (E[|xj(t2)xj(t1)|])pE[|xj(t2)xj(t1)|p]2p1E[(t2t1xj(s)(rj+3i=1ajixi(s)+3i=10τjixi(s+θ)dμji(θ))ds)p]+2p1E[|t2t1σjxj(s)dBj(s)|p]2p1Υ1+2p1Υ2(j=1,2,3). (3.6)

    In view of Theorem 7.1 in [14], for p2, we obtain

    Υ2|σj|p(p(p1)2)p2(t2t1)p22t2t1E[xpj(s)]ds. (3.7)

    From Hölder's inequality, we derive

    Υ17p1rpj(t2t1)p1t2t1E[xpj(s)]ds+3i=17p1apji(t2t1)p1t2t1E[xpi(s)xpj(s)]ds+3i=17p1(t2t1)p1E[t2t1(0τjixi(s+θ)xj(s)dμji(θ))pds]. (3.8)

    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. (3.9)

    Based on (3.6)-(3.9), for p2 and |t2t1|δ,

    (E[|xj(t2)xj(t1)|])pMj|t2t1|p2, (3.10)

    where

    Mj=14p1{rpjKj(p)+3i=1[apji2+12(0τjidμji(θ))p][Ki(2p)+Kj(2p)]}δp2+2p1|σj|p(p(p1)2)p2Kj(p).

    Combining (3.5) with (3.10) yields

    |Gj(t2)Gj(t1)|2pMj|t2t1|. (3.11)

    Therefore, (3.2) follows from (3.4), (3.11) and Barbalat's conclusion in [15].

    In this section we provide some numerical simulations to show the effectiveness of our main theoretical results by using the Milstein approach mentioned in [16]. Let τji=ln2, μji(θ)=μjieθ. Denote

    Param(i)=(r1a11a12a13μ11μ12μ13r2a21a22a23μ21μ22μ23r3a31a32a33μ31μ32μ33).

    Let

    Param(1)=(0.90.20.40.20.40.80.20.20.60.30.10.60.60.20.10.40.30.20.80.40.4),

    subject to x1(θ)=0.7eθ, x2(θ)=0.6eθ, x3(θ)=0.5eθ, θ[ln2,0].

    Case1. σ1=1.4, σ2=0.1, σ3=0.1. Then, D1=0.08. By Theorem 2.2 (i), all three species are extinctive. See Figure 1(a).

    Figure 1.  (a) shows the solution to system (1.3) with Param (1) and σ1=1.4, σ2=0.1, σ3=0.1. This subfigure represents that all species in Case1 are extinctive; (b) shows the solution to system (1.3) with Param (1) and σ1=0.1, σ2=2.0, σ3=1.9. This subfigure represents that in Case2, x1(t) is persistent in mean, while x2(t) and x3(t) are extinctive; (c) shows the solution to system (1.3) with Param (1) and σ1=0.1, σ2=0.1, σ3=0.1. This subfigure represents that all species in Case3 are persistent in mean; (d) shows the solution to system (1.3) with Param (2) and σ1=0.1, σ2=0.1, σ3=0.1. This subfigure represents that in Case4, both x1(t) and x3(t) are persistent in mean, while x2(t) is extinctive; (e) shows the solution to system (1.3) with Param (2) and σ1=0.2, σ2=1.8, σ3=1.5. This subfigure represents that in Case5, x1(t) is persistent in mean, while both x2(t) and x3(t) are extinctive; (f) shows the solution to system (1.3) with Param (3) and σ1=0.1, σ2=0.1, σ3=0.1. This subfigure represents that in Case6, both x1(t) and x2(t) are persistent in mean, while x3(t) is extinctive.

    Case2. σ1=0.1, σ2=2.0, σ3=1.9. Then, D1=0.895, MΘ233=0.0745, MΘ322=0.046. From Theorem 2.2 (ii), x1(t) is persistent in mean, while x2(t) and x3(t) are extinctive. See Figure 1(b).

    Case3. σ1=0.1, σ2=0.1, σ3=0.1. Then, Θ=0.225, Θ1=0.16225, Θ2=0.13375, Θ3=0.09825, MΘ11=0.14. In view of Theorem 2.2 (iv), all three species are persistent in mean. See Figure 1(c).

    Let

    Param(2)=(0.80.10.20.10.20.20.20.30.20.40.20.40.40.20.20.20.20.10.20.40.2),

    subject to x1(θ)=0.7eθ, x2(θ)=0.6eθ, x3(θ)=0.5eθ, θ[ln2,0].

    Case4. σ1=0.1, σ2=0.1, σ3=0.1. Then, Θ=0.001, D1=0.795, MΘ12=0.01, Θ2=0.00975, MΘ322=0.1975. According to Theorem 2.2 (vi), both x1(t) and x3(t) are persistent in mean, while x2(t) is extinctive. See Figure 1(d).

    Case5. σ1=0.2, σ2=1.8, σ3=1.5. Then, Θ=0.001, D1=0.78, MΘ12=0.01, Θ2=0.0143, MΘ322=0.031. Based on Theorem 2.2 (v), x1(t) is persistent in mean, while both x2(t) and x3(t) are extinctive. See Figure 1(e).

    Let

    Param(3)=(0.80.10.10.20.20.20.20.20.20.10.20.20.20.40.30.20.20.40.40.20.4),

    subject to x1(θ)=0.7eθ, x2(θ)=0.5eθ, x3(θ)=0.6eθ, θ[ln2,0].

    Case6. σ1=0.1, σ2=0.1, σ3=0.1. Then, Θ=0.001, D1=0.795, MΘ13=0.01, Θ3=0.00975, MΘ233=0.1975. Thanks to Theorem 2.2 (iii), both x1(t) and x2(t) are persistent in mean, while x3(t) is extinctive. See Figure 1(f).

    All mentioned above can be confirmed by Figure 1.

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

    The authors declare that there are no conflicts of interest.



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