Research article

Dynamics study of nonlinear discrete predator-prey system with Michaelis-Menten type harvesting

  • Received: 09 May 2023 Revised: 16 July 2023 Accepted: 07 August 2023 Published: 25 August 2023
  • In this paper, we study a discrete predator-prey system with Michaelis-Menten type harvesting. First, the equilibrium points number, local stability and boundedness of the system are discussed. Second, using the bifurcation theory and the center manifold theorem, the bifurcation conditions for the system to go through flip bifurcation and Neimark-Sacker bifurcation at the interior equilibrium point are obtained. A feedback control strategy is used to control chaos in the system, and an optimal harvesting strategy is introduced to obtain the optimal value of the harvesting coefficient. Finally, the numerical simulation not only shows the complex dynamic behavior, but also verifies the correctness of our theoretical analysis. In addition, the results show that the system causes nonlinear behaviors such as periodic orbits, invariant rings, chaotic attractors, and periodic windows by bifurcation.

    Citation: Xiaoling Han, Xiongxiong Du. Dynamics study of nonlinear discrete predator-prey system with Michaelis-Menten type harvesting[J]. Mathematical Biosciences and Engineering, 2023, 20(9): 16939-16961. doi: 10.3934/mbe.2023755

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  • In this paper, we study a discrete predator-prey system with Michaelis-Menten type harvesting. First, the equilibrium points number, local stability and boundedness of the system are discussed. Second, using the bifurcation theory and the center manifold theorem, the bifurcation conditions for the system to go through flip bifurcation and Neimark-Sacker bifurcation at the interior equilibrium point are obtained. A feedback control strategy is used to control chaos in the system, and an optimal harvesting strategy is introduced to obtain the optimal value of the harvesting coefficient. Finally, the numerical simulation not only shows the complex dynamic behavior, but also verifies the correctness of our theoretical analysis. In addition, the results show that the system causes nonlinear behaviors such as periodic orbits, invariant rings, chaotic attractors, and periodic windows by bifurcation.



    Population is a collection of individuals of the same species living together within a certain spatial range. The study of population dynamics mainly describes the dynamic relationship between population communities in predation systems and food web systems. Food web refers to the complex relationship network between predation, competition, cooperation and reciprocity between biological populations in biological systems. The study of food web population dynamics can give humans an important understanding of the basic nature of ecosystems, promoting the evolution of life, protecting the natural environment, and maintaining ecological balance at the macro level, and give certain guiding opinions on the protection of endangered species at the micro level. Therefore, studying the interactions between different biological populations through mathematical modeling is an important area of research for ecosystems.

    In 1976, May showed in [1] that the first-order discrete equation model, although simple, can produce a series of extremely complex dynamic behaviors, such as from stable points to unstable bifurcation levels, and eventually produce chaos. However, in continuous-time models, achieving such complex dynamic behavior requires differential equations of three dimensions and more than three dimensions to cause chaos [2]. It can be seen that discrete systems described by the difference equation are richer in dynamical phenomena. Consequently, the discrete dynamical system model has attracted the attention and research of more scholars [3,4,5,6,7,8,9,10,11].

    In [12], Gan et al. studied the stability in a simple food chain system with Michaelis-Menten functional responses and nonlocal delays, using the Lyapunov functional to derive sufficient conditions for global stability of positive steady state and semi-trivial steady state. In [13], Clark et al. described mathematical models of exploited fish stocks, assuming that certain stocks can be obtained through dynamic aggregation processes. The effects of aggregation on yield-effort relationships, abundance indices, and fishery dynamics are discussed, as well as various management approaches for these models. On the other hand, with the increasing demand for food and other resources, the exploitation of biological resources is also increasing. More ecologists are very interested in studying these types of models, such as predator-prey models, and consider the impact of exploiting (harvesting) resources to protect the sustainable use of biological resources [14,15,16,17]. To do this, they applied optimal capture and control strategies to achieve the recyclability of biological resources.

    In [20], we studied the behavioral analysis of a class of discrete dynamical system with linear harvest rates, and obtained many complex dynamic phenomena. Considering the finite nature of resources and space, the linear capture rate has no upper bound, so we will further study the Michaelis-Menten[13] type capture on the basis of the original, and this type of capture is a kind of harvest that gradually rises until the saturation state with the increase of the number of captured objects, which is bounded and more in line with the realistic ecological environment. So, in this paper we consider a discrete-time predator-prey model with Michaelis-Menten type harvesting in preys, which is given by

    {un+1=unexp[r1(1unK)r2vnc+unqEm1E+m2un],vn+1=vnexp[a+r2dunc+unbvnh2], (1.1)

    where the meanings of all parameters of model (1.1) are shown in Table 1.

    Table 1.  The interpretation of parameters.
    parameters interpretation
    u,v the densities of prey and predator population, respectively
    r1 the intrinsic growth rates of prey
    a the intrinsic growth rates of predator
    K the environmental carrying capacity of prey
    r2 the consumption rate of prey
    b the competition between individuals due to overcrowding of predator
    c the half saturation constant
    d the conversion rate of predator
    h2 the capture rate of predator
    mi,i=1,2 suitable constants
    q the catchability co-efficients of prey
    E the degree of harvest effort

     | Show Table
    DownLoad: CSV

    The paper is organized as follows. In Section 2, we analyze the dynamics of system (1.1), including the existence and local stability of the equilibrium points, and the boundedness of system (1.1). In Section 3, using the bifurcation theory and the center manifold theorem, the flip bifurcation and Neimark-Sacker bifurcation are analyzed, and the conditions for determining the bifurcation direction and the stability of the bifurcation periodic solution are obtained. In Section 4, a feedback control strategy is used to control chaos in the system, and an optimal harvesting strategy is introduced to obtain the optimal value of the harvesting coefficient. In Section 5, we verify our analytical results through numerical simulations. In the last Section, the article is ended with a brief conclusion.

    Lemma 1 Solutions of system (1.1) with nonnegative initial conditions remain nonnegative. If u0=0, then un=0 for all n0. If v0=0, then vn=0 for all n0. If u0>0 and v00, then un>0 for all n0. If u00 and v0>0, then vn>0 for all n0.

    Proof. It can be directly demonstrated by system (1.1) structure.

    Lemma 2

    (I) System (1.1) always has a trivial equilibrium point E0(0,0). At this moment, the two species will go extinct.

    (II) If q<r1m1, then system (1.1) always has a positive semi-trivial equilibrium point E1(α+Δ2,0), where α=m1Em2K, β=qEKr1EKm1r1m1, Δ=α24β>0. At this time, the prey population reaches α+Δ2, and the predator tends to go extinct.

    (III) If a>h2, then system (1.1) always has a positive semi-trivial equilibrium point E2(0,ah2b). At this time, the prey population tend to go extinct, and the predator population converge to ah2b.

    (IV) System (1.1) has a positive nontrivial equilibrium point E(u,1b(a+r2duu+ch2)), where a>h2, and u is the positive solution to the quartic equation of one variabie

    A1u4+A2u3+A3u2+A4u+A5=0,

    where

    A1=bm2,A2=bm2(r1K2c)bm1E,A3=r1bK(m1E+2cm2)bc(2m1E+cm2)+r2Km2(h2a)dr22Km2bqEK,A4=r1bcK(2m1E+cm2)bc2m1E+r2Km1E(h2a)+r2cKm2(h2a)EK(dr22m1+2bcq),A5=cEKm1(r1bc+r2h2r2a)+bc2qEK.

    When system (1.1) has a positive interior equilibrium point E, two species coexist, i.e. two species do not go extinct.

    Proof. Direct computation.

    Lemma 3 [18] The equilibrium point (u,v) is called

    (I) Sink (locally asymptotically stable) if |λ1|<1 and |λ2|<1;

    (II) Source (locally unstable) if |λ1|>1 and |λ2|>1;

    (III) Saddle if |λ1|>1 and |λ2|<1 (or |λ1|<1 and |λ2|>1);

    (IV) Non-hyperbolic if |λ1|=1 or |λ2|=1.

    Jacobian matrix can be evaluated at E0(0,0) as

    J(E0)=(er1qm100eah2). (2.1)

    The eigenvalues of J(E0) are λ1=er1qm1 and λ2=eah2. The results regarding dynamical behaviors are listed in Table 2.

    Table 2.  Properties of equilibrium point E0(0,0).
    Conditions Eigenvalues Properties
    λ1=er1qm1 λ2=eah2
    r1m1<q a<h2 |λ1|<1 |λ2|<1 Sink
    a>h2 |λ2|>1 Saddle
    a=h2 |λ2|=1 Non-hyperbolic
    r1m1>q a<h2 |λ1|>1 |λ2|<1 Saddle
    a>h2 |λ2|>1 Source
    a=h2 |λ2|=1 Non-hyperbolic
    r1m1=q a<h2 |λ1|=1 |λ2|<1 Non-hyperbolic
    a>h2 |λ2|>1 Non-hyperbolic
    a=h2 |λ2|=1 Non-hyperbolic

     | Show Table
    DownLoad: CSV

    From Table 2, we can get the following theorem.

    Theorem 1. When r1m1<q and a<h2 are satisfied, the trivial equilibrium point E0(0,0) is locally asymptotically stable.

    The Jacobian matrix computed at E1(α+Δ2,0) is

    J(E1)=(1r1(Δ2α)2K+2qEm2(Δ2α)4m21E2+m22(Δ2α)2+4m1m2E(Δ2α)r2(Δ2α)(Δ2α)+2c0exp[a+r2d(Δ2α)(Δ2α)+2ch2]).

    The eigenvalues of the Jacobian are λ1=1r1(Δ2α)2K+2qEm2(Δ2α)4m21E2+m22(Δ2α)2+4m1m2E(Δ2α) and λ2=exp[a+r2d(Δ2α)(Δ2α)+2ch2]. The properties of semi-trivial equilibrium point E1(α+Δ2,0) are summarized in Table 3.

    Table 3.  Properties of semi-trivial equilibrium point E1(α+Δ2,0).
    Conditions Eigenvalues Properties
    λ1 λ2
    0<r1(Δ2α)2K2qEm2(Δ2α)4m21E2+m22(Δ2α)2+4m1m2E(Δ2α)<2 a+r2d(Δ2α)(Δ2α)+2c=h2 |λ1|<1 |λ2|=1 Non-hyperbolic
    a+r2d(Δ2α)(Δ2α)+2c<h2 |λ2|<1 Sink
    a+r2d(Δ2α)(Δ2α)+2c>h2 |λ2|>1 Saddle
    r1(Δ2α)2K2qEm2(Δ2α)4m21E2+m22(Δ2α)2+4m1m2E(Δ2α)>2 a+r2d(Δ2α)(Δ2α)+2c=h2 |λ1|>1 |λ2|=1 Non-hyperbolic
    a+r2d(Δ2α)(Δ2α)+2c<h2 |λ2|<1 Saddle
    a+r2d(Δ2α)(Δ2α)+2c>h2 |λ2|>1 Source
    r1(Δ2α)2K2qEm2(Δ2α)4m21E2+m22(Δ2α)2+4m1m2E(Δ2α)=2 a+r2d(Δ2α)(Δ2α)+2c=h2 |λ1|=1 |λ2|=1 Non-hyperbolic
    a+r2d(Δ2α)(Δ2α)+2c<h2 |λ2|<1 Non-hyperbolic
    a+r2d(Δ2α)(Δ2α)+2c>h2 |λ2|>1 Non-hyperbolic

     | Show Table
    DownLoad: CSV

    From Table 3, we can have the following theorem.

    Theorem 2. When r1(Δ2α)2K2qEm2(Δ2α)4m21E2+m22(Δ2α)2+4m1m2E(Δ2α)>2 and a+r2d(Δ2α)(Δ2α)+2c>h2 are satisfied, the semi-trivial equilibrium point E1(α+Δ2,0) is locally unstable.

    Jacobian matrix can be evaluated at E2(0,ah2b) as

    J(E2)=(exp[r1r2(ah2)bcqm1]0r2d(ah2)bc1(ah2)). (2.2)

    The eigenvalues of the Jacobian are λ1=exp[r1r2(ah2)bcqm1] and λ2=1(ah2) at semi-trivial equilibrium point E2(0,ah2b). The results of dynamical behaviors are listed in Table 4.

    Table 4.  Properties of semi-trivial equilibrium point E2(0,ah2b).
    Conditions Eigenvalues Properties
    λ1=exp[r1r2(ah2)bcqm1] λ2=1(ah2)
    r1>r2(ah2)bc+qm1 0<ah2<2 |λ1|>1 |λ2|<1 Saddle
    ah2>2 |λ2|>1 Source
    ah2=2 |λ2|=1 Non-hyperbolic
    r1<r2(ah2)bc+qm1 0<ah2<2 |λ1|<1 |λ2|<1 Sink
    ah2>2 |λ2|>1 Saddle
    ah2=2 |λ2|=1 Non-hyperbolic
    r1=r2(ah2)bc+qm1 0<ah2<2 |λ1|=1 |λ2|<1 Non-hyperbolic
    ah2>2 |λ2|>1 Non-hyperbolic
    ah2=2 |λ2|=1 Non-hyperbolic

     | Show Table
    DownLoad: CSV

    From Table 4, we can get the following theorem.

    Theorem 3 The semi-trivial equilibrium point E2(0,ah2b) is always locally asymptotically stable when r1<r2(ah2)bc+qm1 and 0<ah2<2 are satisfied.

    J|(u,v) evaluated at the positive equilibrium point E(u,v) is

    J(E)=(1r1uK+r2uv(u+c)2+qEm2u(m1E+m2u)2r2uc+ur2dcv(c+u)21bv). (2.3)

    Then characteristic equation of J(E) is given by

    λ2TrAλ+DetA=0, (2.4)

    where

    T=TrA=2r1uK+r2uv(u+c)2+qEm2u(m1E+m2u)2bv,D=DetA=[1r1uK+r2uv(u+c)2+qEm2u(m1E+m2u)2](1bv)+r22dcuv(c+u)3.

    Lemma 4 [18] Suppose that F(λ)=λ2Tλ+D, and F(1)>0, λ1 and λ2 are roots of F(λ)=0. Then the following results hold true:

    (I) |λ1|<1 and |λ2|<1 if and only if F(1)>0 and D<1;

    (II) |λ1|<1 and |λ2|>1 (or |λ1|>1 and |λ2|<1) if and only if F(1)<0;

    (III) |λ1|>1 and |λ2|>1 if and only if F(1)>0 and D>1;

    (IV) λ1=1 and |λ2|1 if and only if F(1)=0 and D0,2;

    (V) λ1 and λ2 are complex and |λ1|=|λ2|=1 if and only if T24D<0 and D=1.

    Lemma 5 [11] Let E(u,v) be the unique positive equilibrium point of system (1.1), then the following propositions hold:

    (1.) It is a sink if and only if

    |T|<D+1andD<1.

    (2.) It is a source if and only if

    |T|<D+1andD>1,or|T|>D+1.

    (3.) It is a saddle if and only if

    T2>4Dand|T|>|D+1|.

    (4.) It is non-hyperbolic if and only if

    |T|=|D+1|,orD=1and|T|2.

    To sum up, we have the following theorem.

    Theorem 4 System (1.1) at the the positive equilibrium point E(u,v) is local asymptotically stable when the conditions

    4r1u(2+bv)K+r2(2bv)uv(c+u)2+qEm2u(2bv)(m1E+m2u)22bv+r22dcuv(u+c)3>0

    and

    r1u(1+bv)K+r2(1bv)uv(c+u)2+qEm2u(1bv)(m1E+m2u)2bv+r22dcuv(u+c)3<0

    hold.

    Proof. According to Lemma 3 and Lemma 4, E(u,v) is local asymptotically stable if and only if F(1)>0,F(1)>0 and D<0, the conclusion of Theorem 4 obtained by calculation holds.

    Lemma 6 [19] Assume that ut satisfies u0>0, and ut+1utexp[B(1Cut)] for t[t1,), where C is a positive constant. Then limtsup ut1BCexp(B1).

    Theorem 5 Every positive solution {(un,vn)} of system (1.1) is uniformly bounded.

    Proof. Suppose that {(un,vn)} be an arbitrary positive solution corresponding to system (1.1). Then, from first part of system (1.1), one has

    un+1=unexp[r1(1unK)r2vnc+unqEm1E+m2un]unexp[r1(1unK)r2vnc+un]unexp[r1(1unK)],

    for all n=0,1,2,. Suppose that u0>0, then according to Lemma 6, we gain

    limnsup unKr1exp(r11):=M1.

    From the second part of system (1.1), we have

    vn+1=vnexp[a+r2dunc+unbvnh2]vnexp[a+r2dunc+unbvn]vnexp[a+r2dM1c+M1bvn].

    Assume that v0>0, then using Lemma 6, we obtain

    limnsup vnbexp(a(M1+c)+r2dM1M1+c1):=M2.

    That is to say that limnsup (un,vn)M, where M=max{M1,M2}. This completes the proof.

    The characteristic equation related to system (1.1) at the unique positive interior equilibrium point E(u,v) is

    F(λ)=λ2T(u,v)λ+D(u,v)=0,

    where

    T(u,v)=1r1uK+Φ+Ψ,D(u,v)=Ψ[1r1uK+Φ]+Θ,Ψ:=1bv,Θ:=r2dcuv(u+c)3,Φ:=r2uv(u+c)2+qEm2u(m2u+m1E)2.

    Assume that T2(u,v)>4D(u,v), that is,

    (1r1uK+Φ+Ψ)2>4Ψ[1r1uK+Θ]+4Θ (3.1)

    and T(u,v)+D(u,v)=1, that is to say

    r1=Ku(1+Ψ)(2+2Ψ+Φ(1+Ψ)+Θ). (3.2)

    Then eigenvalue of F(λ)=0 are λ1=1 and λ2=2+Φ+Ψr1uK. The condition |λ2|1 indicates that

    Ψ[1r1uK+Φ]+Θ±1. (3.3)

    Consider the following set

    AF={(a,b,c,d,K,r1,r2,m1,m2,h2,q,E)R12+:(3.1), (3.2) and (3.3) are satisfied }

    When the perturbation parameter changes within a small field of AF, the system (1.1) will have flip bifurcation at E. Let parameters (a,b,c,d,K,r1,r2,m1,m2,h2,q,E)AF and consider the following systems:

    {un+1=unexp[(r1+r)(1unK)r2vnc+unqEm1E+m2un],vn+1=vnexp[a+r2dunc+unbvnh2],

    where r is a small perturbation parameter and |r|1.

    Let x=uu and y=vv. Then we gain

    (xn+1yn+1)=(W11W12W21W22)(xy)+(f(x,y,r)g(x,y,r)), (3.4)

    where

    f(x,y,r)=W13x2+W14xy+W15y2+W16x3+W17x2y+W18xy2+W19y3+Z1xr+Z2yr+Z3r2+Z4xyr+Z5x2r+Z6y2r+Z7xr2+Z8yr2+Z9r3+O((|x|,|y|,|r|)4),g(x,y,r)=W23x2+W24xy+W25y2+W26x3+W27x2y+W28xy2+W29y3+O((|x|,|y|,|r|)4),W11=1r1uK+r2uv(u+c)2+qEm2(m1E+m2u)2=1+Ω,W12=r2u(c+u),
    W13=Ω2r12Kr1uΩ2K+r2v(cu)2(u+c)3+r2uvΩ2(u+c)2+qEm2(m1Em2u)2(m1E+m2u)3+qEm2uΩ2(m1E+m2u)2,W14=r2c+u+r1r2u(u+c)Kr2qEm2(c+u)(m1E+m2u)2,W15=r21u2(c+u)2,W16=Ωu+Ω26r1Ω3Kr1uΩΩu6Kr2cv2(u+c)+r2cΩv6(c+u)3c2u6(c+u)4qE2m1m22(m1E+m2u)4uΩ6(c+u)3+r2v(cu)Ω6(u+c)3+r2uvΩΩu6(c+u)2+qEm2(m1Em2u)Ω6(m1E+m2u)3+qEm2uΩΩu6(m1E+m2u)2+qE2m1m2Ω6(m1E+m2u)3qEm22uΩ6(m1E+m2u)3qEm22(m1Em2u)6(m1E+m2u)4,W17=r1r2(1+u)2K(c+u)+r2u2(c+u)2+r2(cu)r22uv2(c+u)3r21r2u22K2(c+u)r1r2u2K(c+u)2+r1r22u2v(u+c)3+2r22u2vr22v(cu)2(c+u)4r32u2v22(c+u)5r2qEm22(u+c)(m1E+m2u)2+r2qEm1u(1+u)2(c+u)2(m2u+m1E)2r22qEm2uv(1+u)2(c+u)3(m2u+m1E)2r2qEm2(m1Em2u)2(c+u)(m2u+m1E)3+r1r2qEm2(1+u)u2K(c+u)(m1Em2u)2r2q2m22E2u2(c+u)(m2u+m1E)4,W18=r222(c+u)2r22u(c+u)3+r32uv2(u+c)4r1r22u2K(c+u)2+r22qEm22(u+c)2(m1E+m2u)2,W19=r32u6(c+u)3,Z1=12uKr1(Ku)uK2+r2uv(Ku)K(u+c)2+qEm2(Ku)K(m1E+m2u)2,Z2=r2(Ku)uK(c+u),Z3=u(Ku)22K2,Z6=r22u(Ku)2K(u+c)2,Z4=r2(2uK)K(c+u)+r1r2u(Ku)K2(u+c)r2qEm2(Ku)K(c+u)(m1E+m2u)2,Z5=u+12K+r21(Ku)u22K3+r1u(3u+1)r1K(1+u)2K2+r2v(cu)(Ku)2K(c+u)3+qEm2(uK)(m1Em2u)2K(m1E+m2u)3+r2(K3u)uv2K(c+u)2+r2qEm2uv(Ku)(1+u)2K(c+u)2(m1E+m2u)2r1r2(Ku)u2vK2(c+u)2+r22(Ku)u2v22K(c+u)4r1qEm2u(Ku)(1+u)2K2(m1E+m2u)2+q2E2m22(Ku)2K(m1E+m2u)4+qEm2(K2uu2)2K(m1E+m2u)2,Z7=12u2K3(Ku)u2K2r1u(Ku)22K3+r2uv(Ku)22K2(u+c)2+qEm2(Ku)22K2(m1E+m2u)2,Z8=r2u(Ku)22K2(c+u),Z9=u(c+u)36K3,W21=r2dcv(c+u)2,W22=1bv,
    W23=r2dcv(c+u)3+r22d2c22(u+c)4,W24=r2dc(1bv)(u+c)2,W25=b(bv2)2,W26=r2dcv(c+u)4r22d2c2v2(c+u)5+r32d3c3v36(c+u)6,W27=r2dc(bv1)(c+u)3+r22d2c2v(2v)2(c+u)4,W28=r2bdc(c+u)2+r2b2dcv2(c+u)2,W29=b2(3bv)6.

    Construct a nonsingular matrix D1 and consider the following translation:

    (xy)=D1(uv), (3.5)

    where

    D1=(W12W121W11λ2W11).

    Taking D11 on both sides of Eq (3.5), we obtain

    (uv)=(100λ2)(uv)+(f1(x,y,r)g1(x,y,r)), (3.6)

    where

    f1(x,y,r)=[W13(λ2W11)W12W23]x2W12(λ2+1)+[W14(λ2W11)W12W24]xyW12(λ2+1)+Z1(λ2W11)xrW12(λ2+1)+[W15(λ2W11)W12W25]y2W12(λ2+1)+[W16(λ2W11)W12W26]x3W12(λ2+1)+Z2(λ2W11)yrW12(λ2+1)+[W17(λ2W11)W12W27]x2yW12(λ2+1)+[W18(λ2W11)W12W28]xy2W12(λ2+1)+Z3(λ2W11)r2W12(λ2+1)+[W19(λ2W11)W12W29]y3W12(λ2+1)+Z4(λ2W11)xyrW12(λ2+1)+Z5(λ2W11)x2rW12(λ2+1)+Z6(λ2W11)y2rW12(λ2+1)+Z7(λ2W11)xr2W12(λ2+1)+Z8(λ2W11)yr2W12(λ2+1)+Z9(λ2W11)r3W12(λ2+1)+O((|x|,|y|,|r|)4),g1(x,y,r)=[W13(λ2+W11)+W12W23]x2W12(λ2+1)+[W14(λ2+W11)+W12W24]xyW12(λ2+1)+Z1(λ2+W11)xrW12(λ2+1)+[W15(λ2+W11)+W12W25]y2W12(λ2+1)+[W16(λ2+W11)+W12W26]x3W12(λ2+1)+Z2(λ2+W11)yrW12(λ2+1)+[W17(λ2+W11)+W12W27]x2yW12(λ2+1)+[W18(λ2+W11)+W12W28]xy2W12(λ2+1)+Z3(λ2+W11)r2W12(λ2+1)+[W19(λ2+W11)+W12W29]y3W12(λ2+1)+Z4(λ2+W11)xyrW12(λ2+1)+Z5(λ2+W11)x2rW12(λ2+1)+Z6(λ2+W11)y2rW12(λ2+1)+Z7(λ2+W11)xr2W12(λ2+1)+Z8(λ2+W11)yr2W12(λ2+1)+Z9(λ2+W11)r3W12(λ2+1)+O((|x|,|y|,|r|)4),x=W12(u+v),y=(λ2+W11)v(1+W11)u.

    The center manifold theorem Wc is applied in a small field of r=0 at the equilibrium point E0. Then there exists Wc(0) as follows:

    Wc(0)={(x,y,r)R3:y(x,r)=e0r+e1x2+e2xr+e3r2+O((|x|+|r|)3)}

    and satisfies

    H(y(x,r))=y(u+f1(x,y(x,r),r))λ2y(x,r)g1(x,y(x,r),r)=0,

    and we have

    e0=0,e1=[W13(1+W11)+W12W23]W12[W14(1+W11)+W12W24](1+W11)1λ22+[W15(1+W11)+W12W25](1+W11)2(1λ22)W12,e2=[W12Z1Z2(1+W11)](1+W11)(1λ2)2,e3=Z3(1+W11)W12(1λ2)2.

    Therefore, consider the following map on the center manifold Wc(0):

    G:xx+s1x2+s2xr+s3x2r+n4xr2+s5x3+O((|x|+|r|)4),

    where

    s1=[W13(λ2W11)W12W23]W121+λ2[W14(λ2W11)W12W24](1+W11)1+λ2+[W15(λ2W11)W12W25](1+W11)2W12(1+λ2),s2=Z1(λ2W11)1+λ2Z2(λ2W11)(1+W11)W12(1+λ2),s3=[W13(λ2W11)W12W23]2e2W121+λ2+[W14(λ2W11)W12W24](λ2W11)e21+λ22[W15(λ2W11)W12W25](1+W11)(λ2W11)e2W12(1+λ2)+Z1(λ2W11)e11+λ2+(λ2W11)2e1W12(1+λ2)+W12(λ2W11)Z51+λ2+Z6(λ2W11)(1+W11)2(1+λ2)W12[W14(λ2W11)W12W24]e2(1+W11)+Z4(λ2W11)(1+W11)1+λ2,s4=[W13(λ2W11)W12W23]2e2W121+λ2+[W14(λ2W11)W12W24](λ2W11)e3λ2+1[W14(λ2W11)W12W24](1+W11)e3λ2+1+(λ2W11)(Z1e2+Z7)λ2+1[W15(λ2W11)W12W25](1+W11)(λ2W11)e3λ2+1+(λ2W11)2Z2e2W12(λ2+1)Z8(λ2W11)(W11+1)W12(λ2+1),
    s5=[W16(λ2W11)W12W26]W2121+λ2[W17(λ2W11)W12W27](1+W11)W12λ2+12[W15(λ2W11)W12W25](1+W11)(λ2W11)e1(1+λ2)W12+[W13(λ2W11)W12W23]2e2W121+λ2[W14(λ2W11)W12W24](1+W11)e1λ2+1+[W14(λ2W11)W12W24](λ2W11)e1λ2+1+[W18(λ2W11)W12W28](1+W11)2λ2+1[W19(λ2W11)W12W29](1+W11)3W12(λ2+1).

    By flip bifurcation, we define two non-zero real numbers δ1 and δ2, where

    δ1=(2Gxr+12Gr2Gx2)|(0,0)=s2,δ2=(163Gx3+(122Gx2)2)|(0,0)=s21+s5.

    Based on the above analysis, the following theorem can be obtained.

    Theorem 6 System (1.1) undergoes a flip bifurcation at the positive internal equilibrium point E(u,v) if δ10, δ20 are satisfied and when parameter r changes within a small field of r1. Moreover, if δ2>0 (resp., δ2<0), then the period-two orbits that bifurcate from equilibrium point E(u,v) are stable (resp., unstable).

    Consider the characteristic equation at E, then F(λ)=0 has two complex conjugate roots with modulus one if the following conditions are satisfied:

    (1r1uK+Φ)Ψ+Θ=1 (3.7)

    and

    |T|=|1r1uK+Φ+Ψ|=|1+D|<2. (3.8)

    Let

    ANS={(a,b,c,d,K,r1,r2,m1,m2,h2,q,E)R12+:(3.7)and(3.8)aresatisfied}.

    When the parameter changes in a small field of ANS, system (1.1) will have Neimark-Sacker bifurcation at the unique positive equilibrium point E(u,v). Select parameter (a,b,c,d,K,r1,r2,m1,m2,h2,q,E)ANS and analyze the following system:

    {un+1=unexp[(r1+¯r)(1unK)r2vnc+unqEm1E+m2un],vn+1=vnexp[a+r2dunc+unbvnh2],

    where ¯r is a small perturbation parameter and |¯r|1.

    Let x=uu and y=vv. Then we gain

    {xn+1=W11x+W12y+W13x2+W14xy+W15y2+W16x3+W17x2y+W18xy2+W19y3+O((|x|+|y|)4),yn+1=W21x+W22y+W23x2+W24xy+W25y2+W26x3+W27x2y+W28xy2+W29y3+O((|x|+|y|)4), (3.9)

    where Wij(i=1,2,1j9) are given in (3.6) by substituting r1 for r1+¯r.

    The characteristic equation of system (3.9) at (x,y)=(0,0) is as follows:

    λ2T(¯r)λ+D(¯r)=0,

    where

    T(¯r)=1(r1+¯r)uK+Φ+Ψ,D(¯r)=(1(r1+¯r)uK+Φ)Ψ+Θ.

    Since parameters (a,b,c,d,K,r1,r2,m1,m2,h2,q,E)ANS, the roots of the characteristic equation are

    λ1,2=T(¯r)2±i24D(¯r)D2(¯r)

    and we have

    |λ1,2|=D(¯r).

    Suppose that

    L=d|λ1,2|d¯r|¯r=0=Ψu2KD(0)0.

    In addition, it is required that ¯r=0,λl1,21(l=1,2,3,4) which is equal to T(0) -2, 0, -1, 2. Because (a,b,c,d,K,r1,r2,m1,m2,h,q,E)ANS, thus T(0) -2, 2. We only require T(0)0,1, so that

    1r1uK+Φ+Ψ0and2r1uK+Φ+Ψ0. (3.10)

    Let η=T(0)2,ω=4D(0)T2(0)2, we use the following transformation:

    [xy]=D2[uv]=[W120ηW11ω][uv],

    and system (3.10) becomes into

    [ut+1vt+1]=[ηωωη][utvt]+[¯f(u,v)¯g(u,v)],

    where

    ¯f(u,v)=W13W12x2+W14W12xy+W15W12y2+W16W12x3+W17W12x2y+W18W12xy2+W19W12y3+O((|x|+|v|)4),¯g(u,v)=[W13(ηW11)ωW12W23ω]x2+[W14(ηW11)ωW12W24ω]xy+[W15(ηW11)ωW12W25ω]y2+[W16(ηW11)ωW12W26ω]x3+[W17(ηW11)ωW12W27ω]x2y+[W18(ηW11)ωW12W28ω]xy2+[W19(ηW11)ωW12W29ω]y3+O((|x|+|y|)4),x=W12u,y=(ηW11)uωv.

    System (3.9) undergoes the Neimark-Sacker bifurcation if the following quantity Λ is not zero

    Λ=Re[(12λ1)λ221λ1P11P12]12|P11|2|P21|2+Re(λ2P22), (3.11)

    where

    P11=14[(¯fuu+¯fvv)+i(¯guu+¯gvv)],P12=18[(¯fuu¯fvv+2¯guv)+i(¯guu¯gvv2¯fuv)],P21=18[(¯fuu¯fvv2¯guv)+i(¯guu¯gvv+2¯fuv)],P22=116[(¯fuuu+¯fuvv+¯guuv+¯gvvv)+i(¯guuu+¯guvv¯fuuv¯fvvv)].

    If Λ0, Neimark-Sacker bifurcation will occur in system (1.1), and the following theorem holds:

    Theorem 7 System (1.1) undergoes a Neimark-Sacker bifurcation at the positive equilibrium point E(u,v) if conditions (3.10) are satisfied and Λ0. Moreover, if Λ<0(resp., Λ>0), an attracting (resp., repelling) invariant closed curve bifurcates from the steady state for r1>¯r (resp., r1<¯r).

    In this section, we will adopt the feedback control method[23,24,25] to stabilize the chaotic orbit at an unstable equilibrium point by adding a feedback control term to the system (1.1). Therefore, system (1.1) makes the following form:

    {un+1=unexp[r1(1unK)r2vnc+unqEm1E+m2un]h(un,vn)=˜f(un,vn),vn+1=vnexp[a+r2dunc+unbvnh2]=˜g(un,vn), (4.1)

    where h(un,vn)=q1(unu)+q2(vnv) is feedback controlling force, q1 and q2 are feedback gains. Furthermore, ˜f(u,v)=u, and ˜g(u,v)=v.

    The Jacobian matrix corresponding to system (4.1) at interior equilibrium point (u,v) is as follows:

    J(u,v)=[W11q1W12q2W21W22].

    Thus, the characteristic equation related to A(u,v) is:

    λ2(W11+W22q1)λ+(W11q1)W22(W12q2)W21=0. (4.2)

    Let λ1 and λ2 be the eigenvalues of characteristic equation (4.2), then

    λ1+λ2=W11+W22q1,λ1λ2=(W11q1)W22(W12q2)W21. (4.3)

    Next, we must solve equations λ1=±1 and λ1λ2=1 to gain the critical stability line. At the same time, it also ensures that the absolute value λ1 and λ2 are less than one.

    Suppose that λ1λ2=1, then we gain

    L:W11W22W12W211=W22q1W21q2.

    Assume that λ1=1, then we have

    L:W11+W22W11W22+W12W211=(1W22)q1+W21q2.

    Assume that λ1=1, then we obtain

    L:W11+W22+W11W22W12W21+1=(1+W22)q1W21q2.

    Thus, the stable eigenvalues lie within the triangular region with the boundaries of the straight lines L,L,L. In addition, when the control parameters q1 and q2 take values in the triangular region, system (4.1) will not create chaos phenomena.

    For the sustainable use of biological resources and the protection of the natural environment on which human beings depend. Therefore, the development of renewable resources must be reasonable and proportionate. Under the premise of achieving sustainable development of biological resources, pursue maximum yield or best economic benefits. The biological and economic equilibrium combines to form the bioeconomic equilibrium. Biological equilibrium[14,15,16,17] can be obtained by solving un+1=un,vn+1=vn and when the economic rent is equal to zero (meaning that the total income equals the total cost), the economic equilibrium can be obtained. If h1,p are the cost of harvest per unit and unit price of the prey population, respectively, then the total cost is TC=h1E and total income as TR=pqEm1E+m2un. Then the economic rent at the moment t can be expressed as Ξ=TRTC=(pqm1E+m2unh1)E. The bioeconomic equilibrium can be obtained by solving the following simultaneous equations:

    {r1(1unK)r2vnc+unqEm1E+m2un=0,a+r2dunc+unbvnh2=0,pqm1E+m2unh1=0. (4.4)

    At present, if pqm1E+m2un<h1, then we stop capturing because the cost of harvesting is greater than the revenue which also means losses. Similarly, if pqm1E+m2un>h1, then we will continue to capture because of the harvest cost less than revenue which means profit. In order to find the bioeconomic equilibrium point (u,v,E) from system (4.4), we can perform the following steps: first, we solve the value of u from the third equation, and then substitute the value of u into the second equation to get the value of v. Finally, substitute the values of u and v into the first equation to get the value of E.

    Next, we aim to maximize net income while maintaining ecological balance. Define the net income function J=exp(δt)(pqm1E+m2unh1)E, where δ is the discount rate and exp(δt) is the discount factor. At the same time, we use the discrete Pontryagin maximum principle[21] to acquire the optimal capture effort. So the optimal capture problem is

    maxnt=1exp(δt)(pqm1Et+m2uth1)Et,
    s.t.{ut+1=utexp[r1(1utK)r2vtc+utqEtm1Et+m2ut],vt+1=vtexp[a+r2dutc+utbvth2],u1=u0,v1=v0and0EtEmax,fort=0,1,,N1,

    where ut,vt are state variables and Et is the control variable. The Hamiltonian function of the correlation at this moment is

    Ht=exp(δt)(pqm1Et+m2uth1)Et+λ1(t+1)[utexp(r1(1utK)r2vtc+utqEtm1Et+m2ut)]+λ2(t+1)[vtexp(a+r2dutc+utbvth2)].

    Where λ1(t+1) and λ2(t+1) are adjoint variables. In addition, the necessary condition for the optimal problem is that Htut=0, Htvt=0 and Htet=0 are valid at the same time. Optimal harvest Et is available at optimal population size level (ut,vt).

    Htut=exp(δt)pqm2Et(m1Et+m2ut)2+λ1(t+1)[1r1utK+r2utvt(c+ut)2+qm2utEt(m1Et+m2ut)2]+λ2(t+1)r2dcvt(c+ut)2=0,Htvt=λ1(t+1)r2utc+ut+λ2(t+1)(1bvt)=0,HtEt=exp(δt)(pqm2Et(m1Et+m2ut)2h1)λ1(t+1)qm2u2t(m1Et+m2ut)2=0.

    As a consequence, we first solve the value of λ1(t+1)=exp(δt)[pqm2Eth1(m1Et+m2ut)2]qm2u2t from HtEt=0, and then substitute the value of λ1(t+1) into the second equation Htvt=0 to get the value of λ2(t+1)=exp(δt)[pqm2Eth1(m1Et+m2ut)2]r2qm2ut(c+ut)(1bvt). Finally, substitute the values of λ1(t+1) and λ2(t+1) into the first equation Htut=0 to obtain the value of Et.

    This section will show the bifurcation diagram, phase diagram and maximum Lyapunov exponent diagram of system (1.1) to verify the correctness of theoretical analysis.

    Suppose that the parameters (a,b,c,d,E,K,r2,q,m1,m2,h2)=(0.4,0.2,2,0.1,0.4,5,0.5,0.1,0.1,0,0.01)AF, r1 as the bifurcation parameter, and the initial value is (3, 1). Meanwhile, when r1<1.5, the interior equilibrium point does not exist; when r1>1.5, there is a unique interior equilibrium point, and when r1=1.5, the system (1.1) has a transcritical bifurcation at the boundary equilibrium point E2. According to Theorem 6, when r1=3.32, the system (1.1) will have a flip bifurcation at the interior equilibrium point (3.188, 2.104). The bifurcation diagram and the maximum Lyapunov exponent diagram are shown from Figure 1. Combined with Figures 1 and 2, when r1<3.32, the interior equilibrium point is stable. However, when r1>3.32, the interior equilibrium loses its stability, and orbits with periods of 2, 4, 8 appear. As the r1 increases, the maximum Lyapunov exponent value is greater than zero, and it can be seen from Figure 1(c) and Figure 2(c), (f) that system (1.1) will generate chaos.

    Figure 1.  Flip bifurcation and MLE diagram.
    Figure 2.  Phase and solution diagram related to Figure 1 when r1 takes different values.

    Assume that the parameters (a,b,c,d,E,K,r2,q,m1,m2,h2)=(1.7,3.5,1.2,0.3,2,3,2.6,0.1,5,2,0.01), r1 as the bifurcation parameter, and the initial value is (2, 3). The bifurcation diagram and the maximum Lyapunov exponent diagram are shown from Figure 3. Combined with Figures 4 and 5, it is clear from the figure that for smaller values of r1 the system (1.1) is stable, with the increase of r1 the system (1.1) stability disappears and a flip bifurcation with a period of 2 occurs, which subsequently disappears and tends to stabilize. Furthermore, when 2.43<r1<2.59, the equilibrium point is stable. However, when r1>2.59, the system loses its stability, and a stable invariant loop appears. At this moment, the system (1.1) produces Neimark-Sacker bifurcation and periodic solution. When r1 increases, system (1.1) produces quasi-periodic solutions and chaotic phenomena. As the r1 continues to increase, the maximum Lyapunov exponent value is greater than zero, the system (1.1) will generate chaos.

    Figure 3.  Mixed bifurcation and MLE diagram.
    Figure 4.  Phase diagram related to Figure 3 when r1 takes various values.
    Figure 5.  Solution diagram corresponding to Figure 4 when r1 takes various values.

    Considering the parameter values (a,b,c,d,E,K,r2,q,m1,m2,h2)=(1.7,3,1.2,0.3,1.5,3,1.9,0.1,1,2,0.01)ANS with the initial value is (2, 3), and r1 as the bifurcation parameter. According to Theorem 7, when r1=2.518, the system (1.1) has Neimark-Sacker bifurcation at the interior equilibrium point (2.52, 0.69). Figure 6 is the bifurcation and MLE graph corresponding to u and v with r1[2.2,3.2], and Figure 7 is the phase graph related to Figure 6(a). It can be seen from Figures 6 and 7 that when r1<2.518, the equilibrium point is stable; when r1>2.518, the equilibrium point loses its stability, and a stable invariant loop appears. At this moment, system (1.1) arises a periodic solution. When r1 increases, system (1.1) generates quasi-periodic solutions and chaotic phenomena. Furthermore, as the r1 continues to increase, the maximum Lyapunov exponent value is greater than zero, the system (1.1) will generate chaos.

    Figure 6.  Neimark-Sacker bifurcation and MLE diagram.
    Figure 7.  Phase diagram related to Figure 6 when r1 takes various values.

    To verify the chaotic control theory, we analyze Figure 6 and its numerical simulation parameters. In Figure 6(c) when the bifurcation parameter r1=3.1, the maximum Lyapunov exponent value is greater than zero, system (1.1) will produce chaos. When the q1 and q2 are controlled in the triangular region surrounded by three straight lines L, L, and L (see Figure 8), the chaos generated by system (4.1) will be controlled near the equilibrium point and become asymptotically stable state.

    Figure 8.  The bounded region for the eigenvalues related to the controlled system (4.1) in the (q1,q2) plane.

    Considering the parameter values (a,b,c,d,r1,K,r2,q,m1,m2,h2)=(0.95,1.5,1.2,0.3,0.7,5,0.5,0.15,1,1,0.1) with the initial value is (3, 2), and E as the bifurcation parameter. At this time, the bifurcation phenomenon of system (1.1) will not occur. As the degree of capture effort E increases, the population density of prey and predator will continue to decrease and will not tend to 0 (see Figure 9).

    Figure 9.  Bifurcation diagram.

    In this paper, we study the stability and bifurcation of equilibrium points in a discrete predator-prey model with Michaelis-Menten type harvesting. The stability analysis indicates that the model has a trivial equilibrium point, two positive boundary equilibrium points and the boundary equilibrium point is always unstable. The bifurcation analysis shows that when r1=1.5, the boundary equilibrium point E2 will have a transcritical bifurcation, and when the coexistence equilibrium E exists and loses stability, system (1.1) will have a flip bifurcation (see Figure 1). System (1.1) has, in addition, Neimark-Sacker bifurcation occur at the interior equilibrium point E when bifurcation parameter r1 changes in ANS small ranges (see Figure 6). Numerical simulation reveals that when the internal growth rate of prey r1 gradually increases, system (1.1) will produce periodic, quasi-periodic windows and chaos.

    Finally, we analyze chaos control theory and the existence of bioeconomic equilibrium points. In order to maximize profit in a finite time, we built an optimal control problem with the harvest effort as the control parameter, and theoretically obtained the optimal value of the control variable (harvest effort). As a result, we detected that harvesting efforts for prey and predator populations had a specific value that maximizes net income.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    This work was supported by NNSF of China (No.12161079), the Northwest Normal University Graduate Research Grant Project (No.2022KYZZ-S114), and the Gansu Province Innovation Star Project (No.2023CXZX-325).

    The authors declare there is no conflict of interest regarding the publication of this paper.



    [1] R. May, Simple mathematical models with very complicated dynamics, Nature, 261 (1976), 459–467. http://doi.org/10.1038/261459a0 doi: 10.1038/261459a0
    [2] A. Hastings, T. Powell, Chaos in three-species food chain, Ecology, 72 (1991), 896–903. http://doi.org/10.2307/1940591 doi: 10.2307/1940591
    [3] A. Khan, K. Tanzeela, Neimark-Sacker bifurcation and hybrid control in a discrete-time Lotka-Volterra model, Math. Methods Appl. Sci., 43 (2020), 5887–5904.
    [4] A. Hastings, T. Powell, Chaotic dynamics of a discrete prey-predator model with Holling-Type II, Nonlinear Anal. Real World Appl., 10 (2019), 116–129. http://doi.org/10.1016/j.nonrwa.2007.08.029 doi: 10.1016/j.nonrwa.2007.08.029
    [5] E. Elabbasy, A. Elsadany, Y. Zhang, Bifurcation analysis and chaos in a discrete reduced Lorenz system, Appl. Math. Comput., 228 (2014), 184–194. http://doi.org/10.1016/j.amc.2013.11.088 doi: 10.1016/j.amc.2013.11.088
    [6] A. Hastings, T. Powell, Bifurcation analysis of a discrete-time ratio-dependent predator-prey model with Allee effect, Commun. Nonlinear Sci. Numer. Simul., 38 (2016), 288–302. http://doi.org/10.1016/j.cnsns.2016.02.038 doi: 10.1016/j.cnsns.2016.02.038
    [7] Q. Din, Complexity and chaos control in a discrete-time prey-predator model, Commun. Nonlinear Sci. Numer. Simul., 49 (2017), 113–134. http://doi.org/10.1016/j.cnsns.2017.01.025 doi: 10.1016/j.cnsns.2017.01.025
    [8] A. Hastings, T. Powell, The role of vigilance on a discrete-time predator-prey model, Discrete Contin. Dyn. Syst. Ser. B, 27 (2022), 6723–6744. http://doi.org/10.3934/dcdsb.2022017 doi: 10.3934/dcdsb.2022017
    [9] X. Liu, D. Xiao, Complex dynamic behaviors of a discrete-time predator-prey system, Chaos Solitons Fractals, 32 (2007), 80–94. http://doi.org/10.1016/j.chaos.2005.10.081 doi: 10.1016/j.chaos.2005.10.081
    [10] X. Han, C. Lei, Bifurcation and turing instability analysis for a space-and time-discrete predator-prey system with Smith growth function, Chaos Solitons Fractals, 166 (2023), 112920. http://doi.org/10.1016/j.chaos.2022.112910 doi: 10.1016/j.chaos.2022.112910
    [11] C. Lei, X. Han, W. Wang, Bifurcation analysis and chaos control of a discrete-time prey-predator model with fear factor, Math. Biosci. Eng., 19 (2022), 6659–6679. http://doi.org/10.3934/mbe.2022313 doi: 10.3934/mbe.2022313
    [12] W. Gan, C. Tian, Q. Zhang, Z. Lin, Stability in a simple food chain system with Michaelis-Menten functional response and nonlocal delays, Abst. Appl. Anal., 10 (2013), 1401–1429. http://doi.org/10.1155/2013/936952 doi: 10.1155/2013/936952
    [13] C. Clark C, M. Mangel, Aggregation and fishery dynamics a theoretical study of schooling and the Purse Seine tuna fisheries, Fishery Bull., 77 (1979), 317–337.
    [14] K. Chakraborty, M. Chakraborty, T. Kar, Optimal control of harvest and bifurcation of a prey-predator model with stage structure, Appl. Math. Simul. Comput., 217 (2011), 8778–8792. http://doi.org/10.1016/j.amc.2011.03.139 doi: 10.1016/j.amc.2011.03.139
    [15] C. Liu, W. Tang, The dynamics and control of a harvested differential-algebraic predator-prey model, Int. J. Inf. Syst. Sci., 7 (2011), 103–113. http://doi.org/10.1109/CCDC.2011.5968249 doi: 10.1109/CCDC.2011.5968249
    [16] M. Bahri, Stability analysis and optimal harvesting policy of predator-prey model with stage structure for predator, Appl. Math. Sci., 8 (2014), 7923–7934. http://doi.org/10.12988/ams.2014.410792 doi: 10.12988/ams.2014.410792
    [17] P. Chakraborty, U. Ghosh, S. Sarkar, Stability and bifurcation analysis of a discrete prey-predator model with square-root functional response and optimal harvesting, Biol. Syst., 28 (2020), 1–20. http://doi.org/10.1142/S0218339020500047 doi: 10.1142/S0218339020500047
    [18] L. Yuan, Q. Yang, Bifurcation, invariant curve and hybrid control in a discrete-time predator-prey system, Biol. Syst., 39 (2015), 2345–2362. http://doi.org/10.1016/j.apm.2014.10.040 doi: 10.1016/j.apm.2014.10.040
    [19] X. Wang, L. Zanette, X. Zou, Modelling the fear effect in predator-prey interactions, Math. Biol., 73 (2016), 1179–1204. http://doi.org/10.1142/S0218339020500047 doi: 10.1142/S0218339020500047
    [20] X. X. Du, X. L. Han, C. Y. Lei, Behavior analysis of a class of discrete-time dynamical system with capture rate, Mathematics, 10 (2022), 2410. http://dx.doi.org/10.3390/math10142410 doi: 10.3390/math10142410
    [21] S. Lenhart, J. Workman, Optimal Control Applied to Biological Models. Mathematical and Computational Biology, 1st edn. Chapman Hall/CRC, London 2007.
    [22] S. Elaydi, Discrete Chaos: With Applications in Science and Engineering, Chapman and hall/CRC, 2007.
    [23] S. Elaydi, Dynamical Systems with Applications Using Mathematica, 1st Edition, Birkhauser, Boston, 2007. http://dx.doi.org/10.1007/978-0-8176-4586-1
    [24] S. Elaydi, An Introduction to Difference Equations, 3rd Edition, Springer-Verlag, New York, 2005.
    [25] G. Chen, X. Dong, From Chaos to Order: Perspectives, Methodologies, and Applications, World Scientific, Singapore, 1998.
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