Asymptotic spreading in a delayed dispersal predator-prey system without comparison principle

  • Received: 01 September 2019 Revised: 01 December 2019
  • Primary: 35K57, 37C65; Secondary: 92D25

  • This paper deals with the initial value problem of a predator-prey system with dispersal and delay, which does not admit the classical comparison principle. When the initial value has nonempty compact support, the initial value problem formulates that two species synchronously invade the same habitat in population dynamics. By constructing proper auxiliary equations and functions, we confirm the faster invasion speed of two species, which equals to the minimal wave speed of traveling wave solutions in earlier works.

    Citation: Shuxia Pan. Asymptotic spreading in a delayed dispersal predator-prey system without comparison principle[J]. Electronic Research Archive, 2019, 27: 89-99. doi: 10.3934/era.2019011

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  • This paper deals with the initial value problem of a predator-prey system with dispersal and delay, which does not admit the classical comparison principle. When the initial value has nonempty compact support, the initial value problem formulates that two species synchronously invade the same habitat in population dynamics. By constructing proper auxiliary equations and functions, we confirm the faster invasion speed of two species, which equals to the minimal wave speed of traveling wave solutions in earlier works.



    Spatial propagation dynamics of parabolic type systems has been widely investigated in literature, and two important indices on spatial propagation are minimal wave speed and spreading speed. Here, the minimal wave speed is the threshold on the existence of specific traveling wave solutions and the spreading speed of a nonnegative function u(x,t),xR,t>0 is defined as follows [1].

    Definition 1.1. Assume that u(x,t) is a nonnegative function for xR,t>0. Then ˆc is called the spreading speed of u(x,t) if

    a): limtsup|x|>(ˆc+ϵ)tu(x,t)=0 for any given ϵ>0;

    b): lim inftinf|x|<(ˆcϵ)tu(x,t)>0 for any given ϵ(0,ˆc).

    From the viewpoint of mathematical biology, the above speed characterizes the spatial expansion of the individuals [28,34]. In the past decades, some important results on these two thresholds have been established for monotone semiflows, see [12,18,26,37,38] and a survey paper by Zhao [43]. When some special cooperative systems are concerned, it has been proven that all components governed by a system have the same spreading speed that is also the minimal wave speed of traveling wave solutions [18,26,38]. At the same time, it has been shown that different components may have different spreading speeds in several noncooperative systems [19,20,21,22,30,33], and at least the spreading speed of one species equals to the minimal wave speed of traveling wave solutions.

    Recently, Li et al. [17] investigated the following nonmonotone system

    {u1(x,t)t=d1[J1u1](x,t)+r1u1(x,t)F1(u1,u2)(x,t),u2(x,t)t=d2[J2u2](x,t)+r2u2(x,t)F2(u1,u2)(x,t), (1)

    where xR,t>0, (u1,u2)R2, r1,r2,d1,d2 are positive constants, F1,F2 are defined by

    F1(u1,u2)(x,t)=1u1(x,t)b10τu1(x,t+s)dη11(s)a10τu2(x,t+s)dη12(s),F2(u1,u2)(x,t)=1u2(x,t)b20τu2(x,t+s)dη22(s)+a20τu1(x,t+s)dη21(s)

    with constants b10,b20,a10,a20,τ>0 and

    ηij(s) is nondecreasing on [τ,0] and ηij(0)ηij(τ)=1,i,j=1,2.

    In this system, [J1u1](x,t),[J2u2](x,t) reflecting the spatial dispersal indicate the long distance effect and nonadjacent contact among individuals [4,13,14], and are defined by

    [Jiui](x,t)=RJi(xy)[ui(y,t)ui(x,t)]dy,i=1,2,

    where Ji,i=1,2, play the role of probability kernel functions about the random walk of individuals and satisfy the following assumptions:

    (J1): Ji is nonnegative and continuous for each i=1,2;

    (J2): for any λR, RJi(y)eλydy<,i=1,2;

    (J3): RJi(y)dy=1, Ji(y)=Ji(y),yR,i=1,2.

    Clearly, (1) is a predator-prey system in population dynamics. In Li et al. [17], Yu and Yuan [41], Zhang et al. [42], the authors investigated its traveling wave solutions connecting (0,0) with the positive steady state, which reflect the process that these two species invade a new habitat from the viewpoint of biology invasion. In particular, Li et al. [17] obtained the minimal wave speed defined by c=max{c1,c2} with

    ci=infλ>0di[RJi(y)eλydy1]+riλ,i=1,2.

    From the viewpoint of initial value problem, let any fixed time be the initial time, the traveling wave solutions in [17,41,42] indicate the initial size of habitat of both species is infinite, which contradicts to some natural phenomena because the initial invasion often begins in finite domain. The purpose of this paper is to explore the dynamics when the initial habitats of two invaders are finite and investigate the long time behavior of

    {u1(x,t)t=d1[J1u1](x,t)+r1u1(x,t)F1(u1,u2)(x,t),u2(x,t)t=d2[J2u2](x,t)+r2u2(x,t)F2(u1,u2)(x,t),ui(x,s)=ϕi(x,s),xR,t>0,s[τ,0],i=1,2, (2)

    in which ϕi(x,s) satisfies

    (Ⅰ): For i=1,2, ϕi(x,s),xR,s[τ,0], is nonnegative, bounded and continuous such that

    ϕi(x,s)=0,|x|>L,s[τ,0],ϕi(xi,0)>0

    for some L>0,xiR. Moreover, they satisfy

    0ϕ1(x,s)1,0ϕ2(x,s)1+a2,xR,s[τ,0].

    Since (2) involves delay effect of intraspecific competition if b1+b2>0, it does not satisfy the comparison principle of classical predator-prey systems or monotone semiflows [40]. Therefore, the spreading speeds can not be investigated by the abstract results mentioned above. In this paper, we shall estimate the spreading speeds of these two species. By constructing proper auxiliary equations and functions, we confirm that either the predator or the prey invades the new habitat at the rough speed c while the spreading speed of the other species may be smaller than c.

    In this section, we shall give and prove the main results on (2). Before giving the main results, we first define some positive constants as follows

    c1=infλ>0d1[RJ1(y)eλydy1]+r1(1a1(1+a2))λ,c2=infλ>0d2[RJ2(y)eλydy1]+r2(1+a2)λ,c2=d2[RJ2(y)eλ2ydy1]+r2λ2,

    in which the existence and uniqueness of λ2>0 is due to (J2)-(J3) and the convex of d2[RJ2(y)eλydy1]cλ+r2 in λ>0 for every c>0. Using these constants, we present the following conclusion.

    Theorem 2.1. Assume that the mild solution (u1(x,t),u2(x,t)) is defined by (2). Then it satisfies

    (0,0)(u1(x,t),u2(x,t))(1,1+a2),xR,t>0. (3)

    Moreover, (u1(x,t),u2(x,t)) satisfies the following properties.

    (1): If c1>c2 is true, then c is the spreading speed of u1(x,t) while the spreading speed of u2(x,t) is not larger than c2.

    (2): Further suppose that

    d1[RJ1(y)eλ2ydy1]c2λ2+r10. (4)

    If c1c2 is true, then c is the spreading speed of u2(x,t) while the spreading speed of u1(x,t) is not larger than c1.

    We now prove the above theorem by several lemmas. Let X be the Banach space of uniformly continuous and bounded functions equipped with supremum norm. For each i{1,2}, we see that di[Jiv](x):XX is a bounded linear operator by (J1), so

    ui(x,t)t=di[Jiui](x,t),ui(x,0)X

    generates a positive C0 semigroup Ti(t):XX,t0 (see [39,Lemma 3.1]), and the mild solution of the above initial value problem is denoted as

    ui(x,t)=Ti(t)ui(x,0)=Ti(ts)ui(x,s)

    for any 0s<t<. Moreover, for any given kernel function J satisfying (J1)-(J3), it also generates a positive C0 semigroup T(t):XX,t0. Consider the following initial value problem

    {u(x,t)t=d[Ju](x,t)+u(x,t)[ru(x,t)],u(x,0)=χ(x)X,xR, (5)

    where J satisfies (J1)-(J3), d>0 and r>0 are constants. Also define

    (6)

    By Jin and Zhao [15], we have the following conclusion.

    Lemma 2.2. Assume that 0χ(x)1. Then (5) admits a solution u(,t)X for all t>0, which also satisfies

    u(x,t)=T(ts)u(x,s)+tsT(tθ)[u(x,θ)[ru(x,θ)]]dθ

    for xR,0s<t<. If w(,t)X,t0 is nonnegative and bounded such that

    {w(x,t)t()d[Jw](x,t)+w(x,t)[rw(x,t)],xR,t>0,w(x,0)()χ(x),xR,

    or

    w(x,t)()T(ts)w(x,s)+tsT(tθ)[w(x,θ)[rw(x,θ)]]dθ

    for xR,0s<t<, then

    w(x,t)()u(x,t),xR,t>0.

    If χ(x) has nonempty support, then for any c<c, we have

    lim inftinf|x|<ctu(x,t)=lim suptsup|x|<ctu(x,t)=r.

    If χ(x) has compact support, then

    limtsup|x|>ctu(x,t)=0,c>c.

    Remark 1. By the positivity of the semigroup, if

    {wi(x,t)td[Jwi](x,t)+wi(x,t)[rwi(x,t)],xR,t>0,wi(x,0)χ(x),xR

    for i{1,2,3}, then

    min{w1(x,t),w2(x,t),w3(x,t)}u(x,t),xR,t>0.

    On the existence of mild solution of (1), we have the following result.

    Lemma 2.3. The positive mild solution (u1(,t),u2(,t))X2 exists for all t>0 and satisfies (3).

    Proof. The local existence is evident by the theory of abstract functional differential equations [27], here the mild solution is defined by

    u1(x,t)=T1(tθ)u1(x,θ)+tθT1(ts)[r1u1(x,s)F1(u1,u2)(x,s)]ds,u2(x,t)=T2(tθ)u2(x,θ)+tθT2(ts)[r2u2(x,s)F2(u1,u2)(x,s)]ds

    for 0θ<t<T with some T(0,]. If T=, then the global existence is true.

    Further by the quasipositivity in u1F1,u2F2, we see the mild solution is nonnegative. If u1(x,t) only exists for t[0,T) with bounded T such that

    limtTsupxRu1(x,t)=,

    then

    u1(x,t)T1(tθ)u1(x,θ)+tθT1(ts)[r1u1(x,s)[1u1(x,s)]]ds

    for 0θ<t<T, and the comparison principle (Lemma 2.2) implies

    0u1(x,t)1,xR,t[0,T).

    A contradiction occurs. The proof is complete by similar discussion on u2(x,t).

    To continue the discussion, we investigate the following scalar equation

    {v(x,t)t=d[Jv](x,t)+rv(x,t)[1v(x,t)b0τv(x,t+s)dη(s)],v(x,s)=ν(x,s), (7)

    where xR,t>0,s[τ,0], J satisfies (J1)-(J3), d>0,r>0,b0,

    η(s) is nondecreasing on [τ,0] such that η(0)η(τ)=1.

    Furthermore, ν(x,s)0 is uniformly continuous and bounded. Evidently, the global existence of mild solution of (7) is true by Lemma 2.3.

    Lemma 2.4. Assume that v(x,t) is the mild solution defined by (7). If ν(x,0) admits nonempty compact support such that 0ν(x,0)1,xR, then its spreading speed is c defined by (6).

    Proof. We now prove it by the idea in Liu and Pan [25]. If

    b0τv(x,t+s)dη(s)=bv(x,t),

    then the result is clear by Lemma 2.2. Otherwise, the positivity implies that

    v(x,t)T(ts)v(x,s)+tsT(tθ)[rv(x,θ)[1v(x,θ)]]dθ

    for any 0s<t<, then Lemma 2.2 implies v(x,t)1 and

    limtsup|x|>ctv(x,t)=0,c>c.

    For any fixed c<c, it suffices to prove that

    lim inftinf|x|<ctv(x,t)>0.

    For the purpose, we select ϵ>0 such that

    and τ(0,τ) such that

    b0τdη(s)<ϵ.

    If bττv(x,t+s)dη(s)2ϵ, then

    rv(x,t)[1v(x,t)b0τv(x,t+s)dη(s)]rv(x,t)[13ϵv(x,t)].

    When bττv(x,t+s)dη(s)>2ϵ, there exists s0[τ,τ] such that

    v(x,s0)2ϵbτ,

    and the uniform continuity implies

    v(y,s0)ϵbτ,|xy|σ

    for some σ>0. Consider the initial value problem

    {v_(x,t)t=d[Jv_](x,t)+rv_(x,t)[1bv_(x,t)],v_(x,0)=ν_(x), (8)

    where ν_(x) is a continuous function satisfying

    (1): ν_(x)=ϵbτ,|x|σ/2;

    (2): ν_(x)=0,|x|σ;

    (3): ν_(x) is even and decreasing in x[σ/2,σ].

    By the positivity of T(t) and the property of continuous functions, we see that v_(0,t) is positive in t>0, and there exists ρ>0 such that v_(0,t)>ρ,t[τ,τ] and so

    b0τv(x,t+s)dη(s)b=bρρbρv(x,t).

    That is, v(x,t) satisfies

    v(x,t)T(ts)v(x,s)+tsT(tθ)[rv(x,θ)[13ϵ(1+b/ρ)v(x,θ)]]dθ

    for all 0s<t<. The proof is complete by Lemma 2.2.

    Lemma 2.5. If c1>c2 is true, then c is the spreading speed of u1(x,t) while the spreading speed of u2(x,t) is not larger than c2.

    Proof. By (3), u2 satisfies

    u2(x,t)T2(tθ)u2(x,θ)+tθT2(ts)[r2u2(x,s)[1+a2u2(x,s)]]ds

    for 0θ<t<, so Lemma 2.2 implies that the spreading speed of u2(x,t) is not larger than c2, which also leads to

    lim suptsup3|x|>(2c2+c1)tu2(x,t)=0. (9)

    Again by (3), we see that

    u1(x,t)T1(tθ)u1(x,θ)+tθT1(ts)[r1u1(x,s)×[1a1(1+a2)u1(x,s)b10τu1(x,s+γ)dη11(γ)]]ds

    for all 0θ<t<, and Lemma 2.4 or its proof implies

    lim inftinf3|x|<(c2+2c1)tu1(x,t)>0. (10)

    We now verify that c is the spreading speed of u1(x,t). Because of Lemma 2.2 and

    u1(x,t)T1(tθ)u1(x,θ)+tθT1(ts)[r1u1(x,s)[1u1(x,s)]]ds

    for all 0θ<t<, it suffices to confirm that

    lim inftinf|x|<ctu1(x,t)>0 (11)

    for any given c<c. We now fix 3c>c2+2c1 and ϵ>0 such that

    c<infλ>0d[RJ(y)eλydy1]+r(12ϵ)λ.

    By (9) and (10), there exists T>0 such that

    and

    inft>Tinf2|x|(c2+c1)tu1(x,t)>0,

    which implies that there exists M>0 depending on ϵ such that

    u1(x,t)T1(tθ)u1(x,θ)+tθT1(ts)[r1u1(x,s)[1ϵMu1(x,s)b10τu1(x,s+γ)dη11(γ)]]ds

    for any Tθ<t. Clearly, the spreading speed is not less than that of

    v(x,t)t=d[Jv](x,t)+rv(x,t)[1ϵMv(x,t)b0τv(x,t+s)dη(s)]

    by repeating the proof of Lemma 2.4. The proof is complete.

    Lemma 2.6. Assume that (4) is true. If c1c2 is true, then c is the spreading speed of u2(x,t) while the spreading speed of u1(x,t) is not larger than c1.

    Proof. By the positivity of (3), u1(x,t) satisfies

    u1(x,t)T1(tθ)u1(x,θ)+tθT1(ts)[r1u1(x,s)[1u1(x,s)]ds

    for any 0s<t, the spreading speed of u1(x,t) is not larger than c1 by Lemma 2.2.

    On the other hand, u2(x,t) satisfies

    u2(x,t)T2(tθ)u2(x,θ)+tθT2(ts)[r2u2(x,s)[1u2(x,s)b20τu2(x,s+γ)dη22(γ)]]ds

    for any 0s<t, and Lemma 2.4 implies that the spreading speed of u2(x,t) is not less than c. Now, we shall prove that

    lim suptsup|x|>ctu2(x,t)=0

    for any fixed c>c. By the positivity, we obtain

    u2(x,t)T2(tθ)u2(x,θ)+tθT2(ts)[r2u2(x,s)[1u2(x,s)+a20τu1(x,s+γ)dη21(γ)]]ds,

    and the result is true if the spreading speed of the following equation is c

    u_2(x,t)t=d2[J2u_2](x,t)+r2u_2(x,t)[1u_2(x,t)+a20τ¯u1(x,s)dη21(s)], (12)

    where u_2(x,0)=u2(x,0), ¯u1(x,s)=ϕ1(x,s),s0, and ¯u1(x,t),t>0 is defined by

    ¯u1(x,t)=T1(t)¯u1(x,0)+t0T1(ts)[r1¯u1(x,s)[1¯u1(x,s)]]ds.

    The main reason why the above claim is true is that the above equation (12) is monotone and admits comparison principle.

    By Remark 1 and (4), we see that there exists T1>0 such that

    ¯u1(x,t)min{eλ2(x+c2t+T1),eλ2(x+c2t+T1),1},xR,t0.

    In fact, let ˆu1(x,t)=eλ2(x+c2t+T1) or eλ2(x+c2t+T1), then

    ˆu1(x,t)td1[J1ˆu1](x,t)+r1ˆu1(x,t),

    and

    ˆu1(x,t)td1[J1ˆu1](x,t)+r1ˆu1(x,t)[1ˆu1(x,t)]

    if ˆu1(x,t)=1. Further select T2T1 such that

    eλ2(T2T1)>a2

    and

    min{eλ2(x+T2c2τ),eλ2(x+T2c2τ),1+a2}sups[τ,0]ϕ2(x,s),xR.

    Then Remark 1 implies that

    u2(x,t)min{eλ2(x+c2t+T2),eλ2(x+c2t+T2),1+a2},xR,t0

    because ˆu2(x,t)=eλ2(x+c2t+T2)(eλ2(x+c2t+T2),1+a2) implies

    ˆu2(x,t)td2[J2ˆu2](x,t)+r2ˆu2(x,t)[1ˆu2(x,t)+a20τ¯u1(x,s)dη21(s)].

    The proof is complete.

    The propagation dynamics of predator-prey systems has important ecology background, one typical case is the evolution of insect herbivores and lupins on Mount St Helens, see [11,29]. Another related topic is the asymptotic spreading in epidemic models because of the similar monotone conditions. In literature, much attention has been paid to the traveling wave solutions since the work of Dunbar [10]. However, there are a few results on asymptotic spreading of predator-prey systems, see part results by Ducrot [7,8], Ducrot et al. [9], Lin [19], Lin et al. [23], Pan [30,32], Wang and Zhang [36].

    The model in this paper admits nonlocal dispersal and time delays, the mechanism has significant biological reasons and other backgrounds [4,5,13,14,28], and the monotone case has been widely studied, see some recent works by [2,3,6]. Similar to that in [16,24], the model in this paper is not a monotone system [35] and time delay is not small enough. When the diffusion is of the classical Ficker type in (1), Pan [31] studied its minimal wave speed of traveling wave solutions connecting trivial steady state with the positive one.

    In this paper, we show that c may be the spreading speed of u1 or u2, which is the minimal wave speed in [17]. It is possible to study the asymptotic spreading of the model in [31] by our idea. Both thresholds in this paper and [17] formulate that two species invade a new habitat. From our results, we see that the predator and the prey may have different spreading speeds, but it is difficult to estimate these spreading speeds. To answer these questions, more properties on the nonlocal operator and delayed systems are necessary. We shall further investigate these questions in our future research.



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