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Research article

Almost periodic solutions of a discrete Lotka-Volterra model via exponential dichotomy theory

  • Received: 03 October 2021 Accepted: 01 December 2021 Published: 09 December 2021
  • MSC : 34D10, 34K14, 39A10, 39A11

  • In this paper, we consider a discrete non-autonomous Lotka-Volterra model. Under some assumptions, we prove the existence of positive almost periodic solutions. Our analysis relies on the exponential dichotomy for the difference equations and the Banach fixed point theorem. Furthermore, by constructing a Lyapunov function, the exponential convergence is proved. Finally, a numerical example illustrates the effectiveness of the results.

    Citation: Lini Fang, N'gbo N'gbo, Yonghui Xia. Almost periodic solutions of a discrete Lotka-Volterra model via exponential dichotomy theory[J]. AIMS Mathematics, 2022, 7(3): 3788-3801. doi: 10.3934/math.2022210

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  • In this paper, we consider a discrete non-autonomous Lotka-Volterra model. Under some assumptions, we prove the existence of positive almost periodic solutions. Our analysis relies on the exponential dichotomy for the difference equations and the Banach fixed point theorem. Furthermore, by constructing a Lyapunov function, the exponential convergence is proved. Finally, a numerical example illustrates the effectiveness of the results.



    In recent years, using a wide variety of methods, a considerable amount of literature has been produced regarding the stability and existence of almost periodic solutions of differential equations [2,3,4,5,6,7,8,9,10,11,12,13]. Almost periodic solutions of most differential equations are vector-valued functions defined on the set of real numbers R, but the concept of almost periodic solution, makes more sense on any additive group except R, in mathematical modeling, discrete time models are preferred over the continuous time models. As it is directly applicable to various fields (economics, populations dynamics, species interactions, mathematical biology, ecology etc.), the theory of difference equation is much more substantiated than the corresponding theory of differential equation (see [14,15,16,17,18,19,20]).

    Gopalsamy and Mohamad [21] established the following criteria for the existence of globally attractive positive almost periodic solutions for discrete Lotka-Volterra systems:

    x(n+1)=α(n)x(n)1+β(n)x(n).

    Xia et al. [22] studied the relationship between the global quasi-uniform asymptotic stability of a difference system and the existence of almost periodic solutions. Moreover, they applied their results to a discrete Lotka-Volterra system as follows:

    xi(n+1)=xi(n)exp{ri(n)mj=1aij(n)xj(n)},i=1,,m.

    Meng [23], Niu [24] and Xue [25] et al. obtained the results of global stability, global attraction and uniform stability of almost periodic solutions of discrete Lotka-Volterra systems by constructing Lyapunov functions. To the best of our knowledge, there is no paper employing exponential dichotomy theory (for difference system) to study the existence of almost periodic solutions of discrete Lotka- Volterra systems. Different from the above mentioned works [21,22,23,24,25], in this paper, by using the exponential dichotomy theory for difference equations and Banach fixed point theorem, we prove the existence and uniqueness of solutions for the discrete almost periodic Lotka-Volterra model, formulated as follows:

    xi(n+1)=xi(n)exp{ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n))}, (1.1)

    where ri(n),aij(n),bij,τ(n), i,j=1,,N are the almost periodic sequences.

    The rest of this paper is organized as follows. In the second section, we introduce some preconditions for the existence of almost periodic solutions. In the third section, we prove the properties of the exponential dichotomy for the difference equationsand existence of exponential stability of almost periodic solutions for the Lotka-Volterra model. In the last section, the validity of the results is proved by numerical simulations.

    For a bounded sequence f defined on Z, we define f and f+ as follows:

    f=lim infnf(n),f+=lim supnf(n).

    Taking Z[a,b]={a,a+1,,b1,b}, where a,bZ. Similarly, we denote Z[a,+]={a,a+1,a+2,}.

    Definition 2.1. [2,3,4] If for ϵ>0, there is a constant l(ϵ)>0 such that in any interval of length l(ϵ)>0 there exists a number ˉτZ such that the inequality

    |x(n+ˉτ)x(n)|<ϵ,

    is satisfied for all nZ. Then a sequence x(n) is called to be almost periodic sequence.

    Lemma 2.1. [2,3,4]Let x:ZR and y:ZR. The following holds:

    (a) If x(n) is an almost periodic sequence, then it is bounded.

    (b) If x(n),y(n) are almost periodic sequences, x(n)+y(n) and x(n)y(n) arealmost periodic.

    (c) If x(n) is an almost periodic sequence, then X(n) is almost periodicif and only if X(n) is bounded on Z where

    X(n)=n1k=0x(n).

    (d) If x(n) is an almost periodic sequence and X() is defined on thevalue field of x(n), then Xx is almost periodic.

    Consider the following almost periodic difference system:

    x(n+1)=A(n)x(n)+f(n), (2.1)

    where A:ZZm×m is an almost periodic matrix sequence and f:ZZm is an almost periodic vector sequence. Its linear system is

    x(n+1)=A(n)x(n). (2.2)

    Definition 2.2. [26] Suppose that Φ(n) is a fundamental matrix of the difference system (2.2). If there exists a projection P such that P2=P and two positive constants K,v, such that

    {Φ(r)PΦ1(s+1)K(11+v)rs1,rs,Φ(r)(IP)Φ1(s+1)K(11+v)s+1r,sr, (2.3)

    then the difference system (2.2) is said to admit an exponential dichotomy.

    Lemma 2.2. [26]Let r(n)>0 be an almost periodic sequence on Z and infnZr(n)>0, then the linear system

    Δx(n)=r(n)x(n)

    admits an exponential dichotomy on Z.

    Lemma 2.3. [27] [Chapter 7, Exercise 4]Suppose that system (2.2) admits an exponential dichotomy satisfying definition 2.Then system (2.2) does not admit a non-trivial bounded solution. i.eIf there is a bounded solution, it's only a zero solution.

    Lemma 2.4. [27] [Chapter 7, Theorem 7.6.5]Suppose that Φ(n) is the normal fundamental matrix of the linear system (2.2).If the system (2.2) admits exponential dichotomy with the projection P and the constantsK, v, M with f(n)M. Then the system (2.1) has a unique bounded solution which canbe uniquely expressed by

    x(n)=n1k=Φ(n)PΦ1(k+1)f(k)+k=nΦ(n)(IP)Φ1(k+1)f(k).

    We consider the discrete almost periodic Lotka-Volterra system as follows:

    xi(n+1)=xi(n)exp{ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n))}, (3.1)

    where ri(n),aij(n), bij(n) and τ(n) are positive almost periodic sequences defined on Z. Throughout this paper, we use the notations er+iaii=Bi and B=max{Bi}. Further, we always assume that system (3.1) satisfies the following conditions:

    (H1)ri>Njia+ijBj+Nj=1b+ijBj, 1a+ii(riNjia+ijBjNj=1b+ijBj)=Di.

    Set D=min1nn{Di}. We further suppose that Eq (3.3) satisfies :

    (H2)(D+B)Nj=1(a+ij+b+ij)D2ri<1.

    (H3)ri>1+(D+B)Nj=1(a+ij+b+ij)D2.

    Let ui(t)=1xi(t), ˙ui(t)=1x2i(t)˙xi(t), ˙xi(t)=˙ui(t)1u2i(t), then we have,

    ˙ui(t)=ri(t)ui(t)+ui(t)[Nj=1aij(t)1uj(t)+Nj=1bij(t)1uj(tτ(t))]. (3.2)

    then we can get the difference equation as follow:

    Δui(n)=ri(n)ui(n)+ui(n)[Nj=1aij(n)1uj(n)+Nj=1bij(n)1uj(nτ(n))]. (3.3)

    Theorem 3.1. If (H1)(H3) hold, then there exists a unique positive almost periodic solution ui(n) of (3.3), i.e, system (3.3) has a unique almost periodic solution xi(n).

    Theorem 3.2. Let x(n)={x1(n),,xN(n)}be a positive almost periodic solution of (3.1)in the B. If (H1)(H3) hold, then the solution x(n)={x1(n),,xN(n)}of (3.1) converges exponentially to x(n) as n.

    We consider the almost periodic Lotka-Volterra system as follows:

    ˙xi(t)=xi(t)[ri(t)Nj=1aij(t)xj(t)Nj=1bij(t)xj(tτ(t))],i=1,,N, (4.1)

    where xi(t) denotes the density of prey species xi at time t; ri(t),aij(t), bij(t) and τ(t) are positive continuous almost periodic functions defined on t(,+).

    For the purpose of convenience, we should use piecewise constant variable differential equations to obtain the discrete model. Assume that the average growth rate changes over regular time intervals in (4.1), and then we can incorporate this aspect in (4.1) and obtain the following semi-discretization modified system (4.1):

    ˙xi(t)xi(t)=ri([t])Nj=1aij([t])xj([t])Nj=1bij(t)xj([t]τ([t])), (4.2)

    where t2,1,0,1,2, and [t] denotes the integer part t, t(,+).

    Integrating over nt<n+1,n=,2,1,0,1,2,, we have

    xi(t)=xi(n)exp{ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n))}(tn).

    Let tn+1, then lead us to

    xi(n+1)=xi(n)exp{ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n))}, (4.3)

    where ri(n),aij(n) and bij(n) are positive almost periodic sequences defined on Z.

    Proposition 4.1. For every solution {(x1(n),,xN(n))T} of (4.3), we have

    xi(n)Bi,i=1,,N. (4.4)

    Proof: Obviously, when nn0 xi(n)>0. Suppose that there exists a l0Z[n0,+), such that xi(l0+1)xi(l0), then

    xi(l0+1)=xi(l0)exp{ri(l0)Nj=1aij(l0)xj(l0)Nj=1bij(l0)xj(l0τ(l0))}xi(l0),

    then we get,

    ri(l0)Nj=1aij(l0)xj(l0)Nj=1bij(l0)xj(l0τ(l0))0.

    It follows that

    xi(l0)ri(l0)Njiaij(l0)xj(l0)Nj=1bij(l0)xj(l0τ(l0))aii(l0)ri(l0)aii(l0)r+iaii.

    By the fact that maxxR(xexp(abx))=exp(a1)b, for a,b>0. Hence,

    xi(l0+1)=xi(l0)exp{ri(l0)Nj=1aij(l0)xj(l0)Nj=1bij(l0)xj(l0τ(l0))}xi(l0)exp{ri(l0)aii(l0)xi(l0)}xi(l0)exp{r+iaiixi(l0)}exp(r+i1)aiiexp(r+i)aii=Bi.

    We claim that xi(n)Bi, for nl0. By way of contradiction, we assume that there exists a q0l0, such that xi(q0)>Bi, then, q0l0+2. Let xi(˜q0)>Bi, where ˜q0l0+2 is the smallest integer, then, xi(˜q01)<xi(˜q0). The above argument produces that xi(˜q0)Bi, which is contradictory. The proof of our claim is complete.

    Now, considering that xi(n+1)<xi(n) for all nZ[n0,+). Then limn+xi(n) exists, we denote limn+xi(n)=ˉxi. We claim that ˉxier+iaii. Let us assume that ˉxi>er+iaii. Taking the limit of both sides in system (3.1), gives us

    ˉxi=ˉxiexp{limn+(ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n)))}.

    Hence,

    limn+(ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n)))=0.

    However,

    limn+(ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n)))limn+(ri(n)aii(n)xi(n))r+iaiiˉxi<r+ier+i<0,

    which is a contradiction. The proof is complete.

    Proposition 4.2. Assume that (H1),(H2) and (H3) hold. For every solution {(x1(n),,xN(n))T} of (3.1), we have

    xi(n)Di,i=1,,N. (4.5)

    Proof: By proposition 1, there exists a nN, such that

    Biεxi(n)Bi+ε,nn.

    Suppose that there exists a k0n, such that xi(k0+1)xi(k0). Note that

    xi(n+1)=xi(n)exp{ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n))}xi(n)exp{ri(n)aii(n)xi(n)Njiaij(n)BjNj=1bij(n)Bj}
    xi(n)exp{ria+iixi(n)Njia+ijBjNj=1b+ijxjBj}.

    When n=k0, we have

    xi(k0)xi(k0+1)=xi(k0)exp{ria+iixi(k0)Njia+ijBjNj=1b+ijBj}.

    Then we obtain,

    ria+iixi(k0)Njia+ijBjNj=1b+ijBj0.

    Thus,

    xi(k0)1a+ii(riNjia+ijBjNj=1b+ijBj).

    Then,

    xi(k0+1)1a+ii(riNjia+ijBjNj=1b+ijBj)exp{riNj=1a+ijBjNj=1b+ijBj}Δ=˜xi.

    We claim that xi(n)˜xi, for nk0. Suppose that there exists a p0k0, such that xi(p0)<˜xi, then p0k0+2. Let xi(˜p0)<˜xi, where ˜p0k0+2 is the smallest integer, then, xi(˜p01)xi(˜p0). The above argument produces that xi(˜p0)˜xi, which is a contradiction. The proof of our claim is complete.

    Next, considering that xi(n+1)>xi(n) for all nZ[n0,+). Then limn+xi(n) exists, we denoted limn+xi(n)=x_i. we state that x_i1a+ii(riNjia+ijBjNj=1b+ijBj)Di. We write x_i<1a+ii(riNjia+ijBjNj=1b+ijBj). Taking the limit of both sides in system (3.1), we obtain

    x_i=x_iexp{limn+(ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n)))}.

    Hence, we get

    0=limn+(ri(n)Nj=1aij(n)xj(n)Nj=1bij(n)xj(nτ(n)))limn+ria+iixi(n)Njia+ijBjNj=1b+ijBjria+iix_iNjia+ijBjNj=1b+ijBj>ri(riNjia+ijBjNj=1b+ijBj)Njia+ijBjNj=1b+ijBj=0,

    which is contradictory. Since

    ˜xi=1a+ii(riNjia+ijBjNj=1b+ijBj)exp{riNj=1a+ijBjNj=1b+ijBj}>1a+ii(riNjia+ijBjNj=1b+ijBj)=Di,

    then for nn0, we have xi(n)Di.

    Proof of Theorem 2.1: Let B={φ(n)=(φ1(n),φ2(n),,φN(n))|φi(n):ZR is almost periodic sequence}. For any φB, we consider equation

    Δui(n)=ri(n)ui(n)+[Nj=1aij(n)φi(n)φj(n)+Nj=1bij(n)φi(n)φj(nτ(n))]. (4.6)

    Let uφ(n)=(uφ1(n),uφ2(n),,uφN(n))T be a solution of (4.6).

    Since ri>0, then Δui(n)=ri(n)ui(n) admits an exponential dichotomy on Z. By Lemma 2.4, we have a bounded solution of the form

    uφi(n)=n1m=Φi(n)Φ1i(m+1)fi(m).

    In view of Δui(n)=ri(n)ui(n)ui(n+1)=(1ri(n))ui(n), we have

    Φi(n)=(1ri(n1))(1ri(n2))(1ri(m+1))Φi(m+1).

    We can get

    uφi(n)=n1m=n1s=m+1(1ri(s))[Nj=1aij(m)φi(m)φj(m)+Nj=1bij(m)φi(m)φj(mτ(m))].

    According to Lemma 2.1, and using the almost periodicity of n1s=m+1(1ri(s)), we deduce that uφi is also almost periodic.

    We define a mapping T:BB by setting

    T(φ(n))=uφi(n),φB,

    with the norm T=supnZ|T|.

    Let φ(n)=(φ1(n),φ2(n),,φN(n)),ψ(n)=(ψ1(n),ψ2(n),,ψN(n))B, we have

    Ti(φ(n))Ti(ψ(n))=supnZ|Ti(φ(n))Ti(ψ(n))|=supnZ|n1m=n1s=m+1(1ri(s))[Nj=1aij(m)(φi(m)φj(m)ψi(m)ψj(m))+Nj=1bij(m)(φi(m)φj(mτ(m))ψi(m)ψj(mτ(m)))]|.

    We observe that

    φi(m)φj(m)ψi(m)ψj(m)=φi(m)ψi(m)φj(m)+ψi(m)φj(m)ψi(m)ψj(m)(φi(m)ψi(m)D)+ψi(m)(ψj(m)φj(m))φj(m)ψj(m)φi(m)ψi(m)D+B[(ψj(m)φj(m))]D2.

    Similarly,

    φi(m)φj(mτ(m))ψi(m)ψj(mτ(m))=φi(m)ψi(m)φj(mτ(m))+ψi(m)φj(mτ(m))ψi(m)ψj(mτ(m))(φi(m)ψi(m)D)+ψi(m)[ψj(mτ(m))φj(mτ(m))]φj(mτ(m))ψj(mτ(m))φi(m)ψi(m)D+B[(ψj(mτ(m))φj(mτ(m)))]D2,

    where j=1,,N. Therefore,

    Ti(φ(n))Ti(ψ(n))supnZ|n1m=n1s=m+1(1ri)[Nj=1a+ij(φi(m)ψi(m)D+B[(ψj(m)φj(m))]D2)+Nj=1b+ij(φi(m)ψi(m)D+B[(ψj(mτ(m))φj(mτ(m)))]D2)]|supnZn1m=(1ri)nm1Nj=1(a+ij+b+ij)(|φi(m)ψi(m)D+B[(ψj(m)φj(m))]D2|)(D+B)Nj=1(a+ij+b+ij)D2riφψ.

    Hence, by (H2), the mapping T is contractive on B. It follows that the mapping T possesses a unique fixed point φB, such that Tφ=φ. thus φ is an almost periodic solution.

    Proof of Theorem 2.2: Let y(n)=u(n)u(n), where yi(n)={y1(n),,yN(n)}. Then, for i=1,,N,

    Δyi(n)=ri(n)yi(n)+[Nj=1aij(m)(ui(n)uj(n)ui(n)uj(n))+Nj=1bij(n)(ui(n)uj(nτ(n))ui(n)uj(nτ(n)))].

    Define a function Φ(μ) by setting

    Φ(μ)=eμrieμ+eμ(D+B)D2Nj=1a+ij+(eμD+(D+B)eμ(τ++1)D2)Nj=1b+ij,μ[0,1].

    Obviously, Φ is continuous on [0,1]. Then, by (H3), we have

    Φ(0)=1ri+(D+B)D2Nj=1a+ij+(1D+D+BD2)Nj=1b+ij=1ri+(D+B)Nj=1(a+ij+b+ij)D2<0,

    which implies that there exist a constant λ(0,1], such that

    Φ(λ)=eλrieλ+eλ(D+B)D2Nj=1a+ij+(eλD+(D+B)eλ(τ++1)D2)Nj=1b+ij<0.

    We consider the discrete Lyapunov functional V(n)=|y(n)|eλn. We calculate the difference of Vi(n), for all nn0, i=1,,N, it yields

    ΔVi(n)=Δ(|yi(n)|eλn)=Δ|yi(n)|eλ(n+1)+|yi(n)|Δeλnri(n)|yi(n)|eλ(n+1)+[Nj=1aij(n)|ui(n)uj(n)ui(n)uj(n)|+Nj=1bij(n)|ui(n)uj(nτ(n))ui(n)uj(nτ(n))|]eλ(n+1)+|yi(n)|(eλ(n+1)eλn)|yi(n)|eλ(n+1)ri(n)|yi(n)|eλ(n+1)+[Nj=1aij(n)|ui(n)uj(n)ui(n)uj(n)|+Nj=1bij(n)|ui(n)uj(nτ(n))ui(n)uj(nτ(n))|]eλ(n+1).

    Let Mi=eλn0(maxnZ[n0,)|xi(n)xi(n)|), for all nn0. We claim that

    V(n)=|y(n)|eλn<M, (4.7)

    where M=maxMi. We prove our claim by contradiction. Let be a n>n0, such that Vi(n+1)Mi, and Vi(n)<M, nZ[n0,n), which implies that Vi(n)Mi0 and Vi(n)Mi<0, nZ[n0,n). However,

    0Δ(Vi(n)M)=ΔVi(n)|yi(n)|eλ(n+1)ri(n)|yi(n)|eλ(n+1)+[Nj=1aij(n)|ui(n)uj(n)ui(n)uj(n)|+Nj=1bij(n)|ui(n)uj(nτ(n))ui(n)uj(nτ(n))|]eλ(n+1)(1ri)Mieλ+[Nj=1a+ij|yi(n)eλ(n+1)D+Byj(n)eλ(n+1)D2|+Nj=1b+ij|yi(n)eλ(n+1)D+Byj(nτ(n))eλ(n+1)D2|][eλrieλ+eλ(D+B)D2Nj=1a+ij+(eλD+Beλ(τ++1)D2)Nj=1b+ij]Mi.

    Thus,

    eλrieλ+eλ(D+B)D2Nj=1a+ij+(eλD+(D+B)eλ(τ++1)D2)Nj=1b+ij0,

    which is contradictory. Hence (4.7) holds, then |y(n)|<Meλn for all nn0. This complete the proof.

    We consider two specific examples.

    Example 1: Consider the following system, when N=1,

    x(t)=x(t)[1+sin(t)20140+sintx(t)].

    Discretization of the differential equations, we get

    Δx(n)=x(n)[1+sin(n)20140+sintx(n)]. (5.1)

    It is easy to verity that system (5.1) satisfies all the assumptions. Thus, system (5.1) admits an almost periodic solution that is quasi-uniformly asymptotically stable. Figure 1 shows the dynamics of system (5.1).

    Figure 1.  System(5.1) with x(1) = 1 and nZ[0,40).

    Therefore, the system satisfies all the assumptions. It follows that this system has an almost periodic solution which is exponentially stable.

    Example 2: Consider the following two dimensional predator-prey system, that is N=2,

    {x1(t)=x1(t)[3+sint30x1(t)1+sint40x2(t)]x2(t)=x2(t)[1+sint140+sintx1(t)2sint20x2(t)].

    Discretization of the above differential equations, we obtain

    {Δx1(n)=x1(n)[3+sinn30x1(n)1+sinn40x2(n)]Δx2(n)=x2(n)[1+sinn140+sinnx1(n)2sinn20x2(n)]. (5.2)

    It is easy to verity that system (5.2) satisfies all the assumptions. Thus, system (5.2) admits an almost periodic solution that is exponential convergence. Figure 2 shows the dynamics of system (5.2).

    Figure 2.  System(5.2) with (x1(1),x2(1))=(1,2) and nZ[0,40).

    Therefore, the system satisfies all the assumptions. It follows that this system has an almost periodic solution which is exponentially stable.

    In this paper, by applying exponential dichotomy, we obtain the existence and exponential convergence of positive non-autonomous discrete Lotka-Volterra systems. The method is different from the previous works [21,22,23,24,25]. I believe that this result has potential applications in population dynamics.

    This work was supported by the National Natural Science Foundation of China under Grant (No. 11931016).

    The authors declare that there is no conflict of interests regarding the publication of this article.



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