Research article Special Issues

Discrete stage-structured tick population dynamical system with diapause and control


  • A discrete stage-structured tick population dynamical system with diapause is studied, and spraying acaricides as the control strategy is considered in detail. We stratify vector populations in terms of their maturity status as immature and mature subgroups. The immature subgroup is divided into two categories: normal immature and diapause immature. We compute the net reproduction number R0 and perform a qualitative analysis. When R0<1, the global asymptotic stability of tick-free fixed point is well proved by the inherent projection matrix; there exists a unique coexistence fixed point and the conditions for its asymptotic stability are obtained if and only if R0>1; the model has transcritical bifurcation if R0=1. Moreover, we calculate the net reproduction numbers of the model with constant spraying acaricides and periodic spraying acaricides, respectively, and compare the effects of the two methods on controlling tick populations.

    Citation: Ning Yu, Xue Zhang. Discrete stage-structured tick population dynamical system with diapause and control[J]. Mathematical Biosciences and Engineering, 2022, 19(12): 12981-13006. doi: 10.3934/mbe.2022606

    Related Papers:

    [1] Wandi Ding . Optimal control on hybrid ODE Systems with application to a tick disease model. Mathematical Biosciences and Engineering, 2007, 4(4): 633-659. doi: 10.3934/mbe.2007.4.633
    [2] Maeve L. McCarthy, Dorothy I. Wallace . Optimal control of a tick population with a view to control of Rocky Mountain Spotted Fever. Mathematical Biosciences and Engineering, 2023, 20(10): 18916-18938. doi: 10.3934/mbe.2023837
    [3] Marco Tosato, Xue Zhang, Jianhong Wu . A patchy model for tick population dynamics with patch-specific developmental delays. Mathematical Biosciences and Engineering, 2022, 19(5): 5329-5360. doi: 10.3934/mbe.2022250
    [4] Paul L. Salceanu . Robust uniform persistence in discrete and continuous dynamical systems using Lyapunov exponents. Mathematical Biosciences and Engineering, 2011, 8(3): 807-825. doi: 10.3934/mbe.2011.8.807
    [5] Holly Gaff . Preliminary analysis of an agent-based model for a tick-borne disease. Mathematical Biosciences and Engineering, 2011, 8(2): 463-473. doi: 10.3934/mbe.2011.8.463
    [6] Fawaz E Alsaadi, Chuangxia Huang, Madini O Alassafi, Reem M Alotaibi, Adil M Ahmad, Jinde Cao . Attractivity criterion on a delayed tick population dynamics equation with a reproductive function $ f(u) = ru^{\gamma}e^{-\sigma u} $. Mathematical Biosciences and Engineering, 2022, 19(12): 12852-12865. doi: 10.3934/mbe.2022600
    [7] Shangbing Ai . Global stability of equilibria in a tick-borne disease model. Mathematical Biosciences and Engineering, 2007, 4(4): 567-572. doi: 10.3934/mbe.2007.4.567
    [8] Rafael Bravo de la Parra, Ezio Venturino . A discrete two time scales model of a size-structured population of parasitized trees. Mathematical Biosciences and Engineering, 2024, 21(9): 7040-7066. doi: 10.3934/mbe.2024309
    [9] John E. Franke, Abdul-Aziz Yakubu . Periodically forced discrete-time SIS epidemic model with disease induced mortality. Mathematical Biosciences and Engineering, 2011, 8(2): 385-408. doi: 10.3934/mbe.2011.8.385
    [10] Ming Chen, Meng Fan, Congbo Xie, Angela Peace, Hao Wang . Stoichiometric food chain model on discrete time scale. Mathematical Biosciences and Engineering, 2019, 16(1): 101-118. doi: 10.3934/mbe.2019005
  • A discrete stage-structured tick population dynamical system with diapause is studied, and spraying acaricides as the control strategy is considered in detail. We stratify vector populations in terms of their maturity status as immature and mature subgroups. The immature subgroup is divided into two categories: normal immature and diapause immature. We compute the net reproduction number R0 and perform a qualitative analysis. When R0<1, the global asymptotic stability of tick-free fixed point is well proved by the inherent projection matrix; there exists a unique coexistence fixed point and the conditions for its asymptotic stability are obtained if and only if R0>1; the model has transcritical bifurcation if R0=1. Moreover, we calculate the net reproduction numbers of the model with constant spraying acaricides and periodic spraying acaricides, respectively, and compare the effects of the two methods on controlling tick populations.



    Diapause is a key survival mechanism of Ixodes and other invertebrates, such as mosquitoes, dragonflies and ladybugs [1,2,3], which synchronizes the rhythm of the life cycle with that of the environment to ensure that the active phase of the life cycle occurs when food is abundant and other aspects of the environment are conducive to survival [4]. Diapause is also a developmental stagnation period caused by adverse climatic conditions, particularly photoperiod and relative humidity [5].

    In the natural world, many species go through some of the distinct life stages, and while individuals at each stage are biologically identical, subgroups of these species differ in physical characteristics and have different vital behaviors. The single-species population dynamic model with stage-structured[6,7,8] has attracted the attention of many scholars. Ticks, as vectors of Lyme disease, tick-borne encephalitis and human babesiosis, are vectors of vector-borne diseases that have a significant impact on human health. Since ticks respond differently to the environment at various stage, The life cycle of ticks consists of four successive developmental stages, namely egg, larva, nymph and adult [9,10]. The ticks has different hosts at different stages. For larvae and nymphs, rodents are the most important reservoirs, such as the white-footed mouse. The most important hosts of adults is larger mammals such as ungulates, the most common white-tailed deers [11]. After the eggs evolve into larvae, and the larvae develop into nymphs through a blood meal on a rodent host. The nymphs continue to seek the host and feed. After engorging, the nymphs will drop off the host and go through a period of development, after which they evolve into adults with the male continuing to seek a host while the female lays eggs. The diapause of the tick population is diverse and can occur at any stage of their life cycle. The basic diapause types can be divided into two categories: developmental diapause (temporary suspension of engorged tick development) and behavioral diapause (interruption of host-seeking activity of unfed ticks). Belozerov et al. [12] studied the existence of photoperiod controlled diapause in the nymphs of prostriate ticks and its influence on the nymphs dynamics through some data and confirmed that behavioral diapause in adults of other tick species was a well established phenomenon [13]. Gray [14] found that the diapause behavior was terminated when the female tick approached the diapause male tick, demonstrating a richer dynamic behavior of ticks.

    In recent years, many scholars have considered diapause in the life cycle of population and studied the important influence of diapause on population growth and development by establishing some reasonable mathematical models. Lou et al. [15] regarded the diapause period as a dynamic process independent of the normal period, and studied the influence of diapause on mosquito population dynamics by constructing differential equation model. The sensitivity analysis of the parameters related to diapause proved that by reducing the diapause mortality, the short diapause period could increase the survival ability of mosquitoes, which was more conducive to the normal growth of subsequent mosquito populations. Zhang and Wu [16] analyzed a population dynamics model with ticks as vectors by combining the development delay and diapause delay and computing the Hopf bifurcation value by introducing and analyzing the parametric trigonometric functions. Shu [17] analyzed a time-delay differential equation for a diapause tick population and performed a Hopf bifurcation analysis of the model, showing rich tick dynamic behavior. However, mathematical models considering the role of diapause in the life cycle of ticks is still rare, and most of the existing studies are based on differential equation dynamical systems, ignoring the critical feature that there is no generational overlap in tick populations. Consequently, it is more practical to consider a discrete dynamic model.

    At present, the main measures for tick control include spraying acaricides, using tick-repellent and vaccination. Existing vaccines are still in the stage of screening and validation of tick functional molecules to find suitable antigens. Although there is a small number of commercialization vaccines were developed, such as Boophilus microplus Bm86 and Bm95 antigen vaccines (TickGARD/Gavac), but were not widely available due to their inconsistent effectiveness [18]. Acaricide spraying has been a relatively effective way to control tick populations in recent years. Quantifying and incorporating control measures into tick populations dynamics models will help us more comprehensive explore the development process of ticks and provide theoretical reference for controlling tick-borne disease transmission.

    Our paper is organized as follows. In Section 2, we combine the impact of diapause on the life cycle of tick populations, divide immature ticks into diapause immature and normal immature, and construct a stage-structured non-monotonic tick population dynamical system. In Section 3, we calculate the net reproduction number and discuss the global stability of tick-free fixed point; we also confirm the existence of a unique coexistence fixed point, and infer its local stability under some specific conditions. Moreover, we conclude that when the net reproduction number is at the critical value, the model will undergo a transcritical bifurcation. In Sections 4 and 5, we discuss the uniform persistence and investigate the effects of different acaricides spraying strategies on tick population dynamics, respectively. In Section 6, some numerical simulations are given to support the theoretical analysis and exhibit these rich tick population dynamical behaviors. We end the paper with a brief discussion.

    Denote I(t),Id(t), and M(t) as the amounts of normal immature tick population, diapause immature tick population and mature tick population at time t, respectively. We have the following diagram depicting the growth of tick populations(see Figure 1). Let b be the oviposition rate; γ denotes the survival rate of eggs; s0 is the hatching probability from eggs to the larval stage; d is the diapause rate of immature ticks; β represents the transition rate from immature to mature(i.e., transition rate from nymphs to adults); δ represents the exit rate of diapause immature ticks. We assume that normal and diapause tick population in immature competes for each other and independent of the mature stage. S1(x) is the Beverton-Holt type ca+x [19,20] nonlinear function to describe the survival rate of immature, and we assume that survival rates of diapause immature ticks and mature ticks are constant Sd and Sm, respectively. We let Em represents the acaricidal effect of spraying acaricides. Following the block diagram and assumptions described above, and we consider the following difference system:

    {I(t+1)=bs0γSm(1Em)M(t)+(1d)(1β)S1(I(t)+Id(t))I(t)+δSdId(t),Id(t+1)=d(1β)S1(I(t)+Id(t))I(t)+(1δ)SdId(t),M(t+1)=βS1(I(t)+Id(t))I(t)+Sm(1Em)M(t). (2.1)
    Figure 1.  Diagrams depicting the growth of tick populations.

    Since S1(I(t)+Id(t))=ca+I(t)+Id(t), it satisfies the following conditions:

    (Σ1)S1(x)C1[0,),S1(0)=ca=a1,0<a1<1,S1(x)<0,d(S1(x)x)dx>0,limxS1(x)=0,limxS1(x)x=c<.

    For the view of biology, we assume that δ+d>1.

    Denote z(t) : = (I(t),Id(t),M(t))T. The following matrix form is used to represent model (2.1):

    z(t+1)=Φ(z(t))z(t), (2.2)

    where the projection matrix Φ(z) is given by

    Φ(z)=((1d)(1β)S1(I(t)+Id(t))δSdbS0γSm(1Em)d(1β)S1(I(t)+Id(t))(1δ)Sd0βS1(I(t)+Id(t))0Sm(1Em)).

    Let A=(aij)Rn×m and B=(bij)Rn×m. Define AB if and only if aijbij, for all i=1,...,n, and j=1,...,m. Therefore, from (Σ1) we can obtain that Φ(x)Φ(y), for any xy.

    Furthermore, combined with conditions (Σ1), we have

    M(t+1)=βS1(I(t)+Id(t))I(t)+Sm(1Em)M(t)βc+Sm(1Em)M(t).

    Let ˜M(t+1) satisfy the recursion ˜M(t+1)=βc+Sm(1Em)˜M(t). Then we can easily deduce that ˜M(t+1)=βcti=0(Sm(1Em))i+(Sm(1Em))t+1˜M(0) and ˜M(t) has limit at t. Since 0M(t)˜M(t), M(t) is bounded as t. Let ¯M be its upper bound, that is, M(t)¯M,t=1,2,.... Similarly, we can prove that ¯Id be the upper bound of Id(t) and Id(t)¯Id,t=1,2,.... Then, we can follow from model (2.1) that

    I(t)bs0γSm(1Em)¯M+(1d)(1β)c+δSd¯Id, t=2,3,...

    Therefore, the positivity and boundedness of the solutions of the model (2.1) can be summarized as follows

    Theorem 1. System (2.2) is point dissipative. Let (I,Id,M) be the solution of model (2.1). Denote

    Υ={(I,Id,M)R3+:I[0,bs0γSm(1Em)¯M+(1d)(1β)c+δSd¯Id],Id[0,¯Id],M[0,¯M]}. (2.3)

    Then Υ is positively invariant under the flows of the system (2.2) and is attracting to all solutions of (2.2) under condition (Σ1). That is to say, there is a compact set ΥR3+ such that every forward solution sequence of the system (2.2) enters Υ in at most two-time steps, and remains in Υ forever after.

    We define the net reproduction number R0 of the tick population using the methods in [21,22,23], which is the expected amount of descendants produced by an individual over the course of its life.

    We can obtain the following fertility matrix

    F=(00bs0γSm(1Em)000000),

    and transition matrix

    T(0)=(a1(1d)(1β)δSd0a1d(1β)(1δ)Sd0a1β0Sm(1Em)).

    Then the inherent projection matrix is Φ(0)=F+T(0), and the next generation matrix is given by

    F(IT(0))1=1(1Sm(1Em))[(1Sd)(1a1(1d)(1β))+Sdδ(1a1(1β))](a1bs0βγSm(1Em)(1(1δ)Sd)000000),

    where I denotes the identity matrix. Solving det(λIF(IT(0))1)=0, we can yield the net reproduction number

    R0=a1bs0βγSm(1Em)(1(1δ)Sd)(1Sm(1Em))((1Sd)(1a1(1d)(1β))+Sdδ(1a1(1β))). (3.1)

    It is clear that the tick-free fixed point E0(0,0,0) always exists for the model (2.1). For any z(0)0, we have z(t)0, it follows from system (2.2) and condition (Σ1) that

    0z(1)=Φ(z(0))z(0)Φ(0)z(0),

    and

    0z(2)=Φ(z(1))z(1)Φ(0)z(1)Φ2(0)z(0),

    and repeating this manner, we can get that

    0z(t)Φt(0)z(0).

    It is easily verify that the inherent projection matrix Φ(0) is non-negative, irreducible, and primitive. Thus, Φ(0) has a simple, positive and strictly dominant eigenvalue r. If R0<1, we can obtain r<1 and

    limtΦt(0)=0

    by using the methods in [24]. It indicates that E0(0,0,0) is globally asymptotically stable. In addition, when R0>1, Φ(0) has a positive eigenvalue larger than one. Thus, we linearize model (2.1) at the tick-free fixed point E0(0,0,0) and obtain a positive eigenvalue larger than one. Clearly, the tick-free fixed point E0(0,0,0) is unstable. Therefore, We have the following stability result of the tick-free fixed point E0.

    Theorem 2. If R0<1, model (2.1) only has a unique tick-free fixed point E0(0,0,0), it is globally asymptotically stable, and is unstable if R0>1.

    We define f:=Φ(z(t))z(t) be the map from R3+R3+. Then we linearize the model (2.1) at E0(0,0,0) and obtain the relevant Jacobian matrix

    Jf(E0)=(a1(1d)(1β)δSdbs0γSm(1Em)a1d(1β)(1δ)Sd0a1β0Sm(1Em)). (3.2)

    We can obtain that the characteristic equation of (3.2) is

    f1(λ)=λ3+b1λ2+b2λ+b3=0, (3.3)

    where

    b1=a1(1d)(1β)(1δ)SdSm(1Em),b2=a1Sd(1δ)(1d)(1β)+a1Sm(1Em)(1d)(1β)+Sd(1δ)Sm(1Em)a1dδSd(1β)bs0a1βγSm(1Em),b3=a1Sd(1δ)Sm(1Em)(1d)(1β)+bs0a1βγSd(1δ)Sm(1Em)+a1dδSd(1β)Sm(1Em).

    Combined with the characteristic equation (3.3), we can find that f1(1)=1+b1+b2+b3=0 is equivalent to R0=1, and f1(λ)=(λ1)(λ2(b2+b3)λb3)=0. Therefore, the other two eigenvalues of Jacobian matrix (3.2)

    λ1=b2+b3(b2+b3)2+4b32,λ2=b2+b3+(b2+b3)2+4b32.

    It is easy to derive that when R0=1 and 1<b2<min{2b3,12b3} or 1<b3<0, the eigenvalues of Jacobian matrix (3.2) |λ1,2|<1,λ3=1. Therefore, we have the following theorem:

    Theorem 3. If R0=1, and 1<b2<min{2b3,12b3} or 1<b3<0, model (2.1) undergoes a transcritical bifurcation.

    Proof. We use b as the bifurcation parameter, and then R0=1 is equivalent to

    b=(1Sm(1Em))((1Sd)(1a1(1d)(1β))+Sdδ(1a1(1β)))a1s0βγSm(1Em)(1(1δ)Sd):=b.

    Let B(t)=bb as a new dependent variable. Expanding (2.1) as a Taylor series at (I(t),Id(t),M(t),B(t))=(0,0,0,0) up to terms of 2 produces

    (I(t+1)Id(t+1)M(t+1)B(t+1))=(a1(1d)(1β)δSdbs0γSm(1Em)0a1d(1β)(1δ)Sd00a1β0Sm(1Em)00001)(I(t)Id(t)M(t)B(t))+F, (3.4)

    where F=(f1(I(t),Id(t),M(t),B(t))f2(I(t),Id(t),M(t),B(t))f3(I(t),Id(t),M(t),B(t))0) is shown in Appendix.

    We construct an invertible matrix

    P=(λ1(1δ)Sdλ2(1δ)Sd1(1δ)Sd1(1δ)Sda1d(1β)a1d(1β)a1d(1β)a1d(1β)a1β(λ1(1δ)Sd)(λ1Sm(1Em))a1β(λ2(1δ)Sd)(λ2Sm(1Em))a1β(1(1δ)Sd)(1Sm(1Em))a1β(1(1δ)Sd)(1Sm(1Em))0001).

    Under the transformation

    (I(t)Id(t)M(t)B(t))=P(u(t)v(t)w(t)μ(t)),

    system (3.4) becomes

    (u(t+1)v(t+1)w(t+1)μ(t+1))=(λ10000λ20000100001)(u(t)v(t)w(t)μ(t))+˜F, (3.5)

    where ˜F=(~f1(u(t),v(t),w(t),μ(t))~f2(u(t),v(t),w(t),μ(t))~f3(u(t),v(t),w(t),μ(t))0) is shown in Appendix.

    By the center manifold theory [25], the stability of (u(t),v(t),w(t))=(0,0,0) near μ(t)=0 can be determined by study a family of parameters equations on a center manifold which can be expressed as

    Wc(0)={(u(t),v(t),w(t),μ(t))R4|u(t)=s1(w(t),μ(t)),v(t)=s2(w(t),μ(t)),s1(0,0)=0,Ds1(0,0)=0,s2(0,0)=0,Ds2(0,0)=0},

    where w(t) and μ(t) are sufficiently small. In order to compute the center manifold and determine the equation on the center manifold, we assume

    s1(w(t),μ(t))=σ11w2(t)+σ12w(t)μ(t)+σ13μ2(t)+o(|(w(t),μ(t))|2),s2(w(t),μ(t))=σ21w2(t)+σ22w(t)μ(t)+σ23μ2(t)+o(|(w(t),μ(t))|2). (3.6)

    where o(|(w(t),μ(t))|2) means terms of order greater than 2 in the combination of (w(t),μ(t)). Substituting (3.6) into the center manifold equation, we have

    N1(s1(w(t),μ(t)))=s1(w(t)+˜f3(s1(w(t),μ(t)),s2(w(t),μ(t)),w(t),μ(t)),μ(t))λ1s1(w(t),μ(t))˜f1(s1(w(t),μ(t)),s2(w(t),μ(t)),w(t),μ(t)),μ(t)),N2(s2(w(t),μ(t)))=s2(w(t)+˜f3(s1(w(t),μ(t)),s2(w(t),μ(t)),w(t),μ(t)),μ(t))λ2s2(w(t),μ(t))˜f2(s1(w(t),μ(t)),s2(w(t),μ(t)),w(t),μ(t)),μ(t)). (3.7)

    By simple computation for center manifold, we obtain

    σ11=a00201λ1,σ12=a00111λ1,σ13=a00021λ1,
    σ21=b00201λ2,σ22=b00111λ2,σ23=b00021λ2.

    Thus, model (3.5) restricted to the center manifold is shown below

    F:w(t+1)=w(t)+c0020w2(t)+c0011w(t)μ(t)+c0002μ2(t)+o(|(w(t),μ(t))|2). (3.8)

    It is easy to obtain that (3.8) satisfies the following conditions

    F(0,0)=0,F(0,0)w(t)=1,F2(0,0)w2(t)=2c00200,F2(0,0)w(t)μ(t)=c00110.

    Therefore, it can be concluded that (2.1) undergoes a transcritical bifurcation [25,26,27].

    If the system (2.2) exists a coexistence fixed point E(I,Id,M), then its components must fit in with:

    {I=bs0γSm(1Em)M+(1d)(1β)S1(I+Id)I+δSdId,Id=d(1β)S1(I+Id)I+(1δ)SdId,M=βS1(I+Id)I+Sm(1Em)M. (3.9)

    From the second and third equation of (3.9), we can conclude that

    Id=d(1β)S1(I+Id)1(1δ)SdI,M=βS1(I+Id)1Sm(1Em)I. (3.10)

    Substituting (3.10) into the first equation in (3.9), we can obtain

    (1Sm(1Em))(1(1δ)Sd)=bs0γSm(1Em)βS1(I+Id)(1(1δ)Sd)+(1d)(1β)S1(I+Id)(1Sm(1Em))(1(1δ)Sd)+δSdd(1β)S1(I+Id)(1Sm(1Em)). (3.11)

    Thus

    S1(I+Id)=ca+I+Id=(1Sm(1Em))(1(1δ)Sd)κ,

    where

    κ=bs0γSm(1Em)β(1(1δ)Sd)+(1d)(1β)(1Sm(1Em))(1(1δ)Sd)+δSdd(1β)(1Sm(1Em)).

    Since a1=ca, we can yield

    I+Id=a1κ(1Sm(1Em))(1(1δ)Sd)(1Sm(1Em))(1(1δ)Sd). (3.12)

    Note that I+Id=0 implies M=0. We find that if and only if I+Id>0, a1κ(1Sm(1Em))(1(1δ)Sd)>0, namely, R0>1. From (3.10) and (3.12), we can compute unique coexistence fixed point E of model (2.1).

    Theorem 4. If and only if R0>1, model (2.1) exists a unique coexistence fixed point E(I,Id,M).

    Assume R0>1, and let W(t)=I(t)+Id(t), through simple calculation, we have

    S1(W)I=S1(W)Id=c(a+I+Id)2<0,
    0<S1(W)II=S1(W)II+S1(W)=c(a+Id)(a+I+Id)2<S1(W)<1.

    For simplicity, we define S1(W) as S1(W)I and S1(W)Id, define (S1(W)I) as S1(W)II. Then the Jacobian matrix of model (2.1) at E can be given as follows

    Jf(E)=((1d)(1β)(S1(W)I)(1d)(1β)S1(W)I+δSdbs0γSm(1Em)d(1β)(S1(W)I)d(1β)S1(W)I+(1δ)Sd0β(S1(W)I)βS1(W)ISm(1Em)). (3.13)

    The characteristic polynomial of Jf(E) is given by

    f2(λ)=λ3+c1λ2+c2λ+c3, (3.14)

    where

    c1=(1β)S1(W)I(1d)(1β)S1(W)(1δ)Sd+Sm(1Em),c2=(1β)(S1(W)I)Sd(d+δ1)+(1d)(1β)(S1(W)I)Sm(1Em)+d(1β)S1(W)ISm(1Em)+(1δ)SdSm(1Em)bs0γSm(1Em)β(S1(W)I),c3=(1β)(S1(W)I)(1δ)SdSm(1Em)(d+δ1)+bs0γSm(1Em)(1δ)Sdβ(S1(W)I).

    Theorem 5. When R0>1, the coexistence fixed point E(I,Id,M) is locally asymptotically stable if

    c31<c1<c3.

    Proof. From (3.11), we can conclude that

    1=bs0γSm(1Em)βS1(I+Id)(1(1δ)Sd)+(1d)(1β)S1(I+Id)(1Sm(1Em))(1(1δ)Sd)+δSdd(1β)S1(I+Id)(1Sm(1Em))+(1δ)Sd+Sm(1Em)Sm(1Em)(1δ)Sd. (3.15)

    Substituting (3.15) into f2(1)=1+c1+c2+c3, and combining with condition (Σ1), we can get

    f2(1)=(1d)(1β)(1Sm(1Em))(1S1(W))(1β)(1Sm(1Em))(1δ)Sd+d(1β)(1Sm(1Em))(1S1(W))(1δ)Sd(1β)S1(W)I(1Sm(1Em))bs0γβSm(1Em)S1(W)I(1(1δ)Sd)d(1β)S1(W)ISd(1Sm(1Em))+(1β)(S1(W)I)(1Sm(1Em))(1δ)Sd=(1d)(1β)(1Sm(1Em))(1S1(W))(1(1δ)Sd)d(1β)S1(W)ISd(1Sm(1Em))(1β)S1(W)I(1Sm(1Em))(1(1δ)Sd)bs0γβSm(1Em)S1(W)I(1(1δ)Sd)>0.

    Note that

    f2(1)=1+c1c2+c3andf2(1)+f2(1)=2(c1+c3).

    Then if c1+c3<0, we can get f2(1)>f2(1)>0. Based on previous assumptions about parameters, we have c3>0, then c1<0,|c1|>|c3|, and 1+c2>f2(1)>0. Thus, we have c2c1c3+1c23=1+c2c3(c1+c3)>0, namely,

    c2c1c3>(1c23). (3.16)

    From c1<0, we have c1=(1β)S1(W)I+(1d)(1β)S1(W)+(1δ)Sd+Sm(1Em)>0, which is equivalent to

    (1d)(1β)(S1(W)I)+d(1β)S1(W)I+(1δ)Sd>Sm(1Em).

    Thus,

    1f2(1)=c1c2c3=((1d)(1β)(S1(W)I)+d(1β)S1(W)I+(1δ)Sd))(1Sm(1Em))+Sm(1Em)+(1β)(S1(W)I)Sd(d+δ1)(1Sm(1Em))+bs0γSm(1Em)β(S1(W)I)(1(1δ)Sd)>(Sm(1Em))2+(1β)(S1(W)I)Sd(d+δ1)(1Sm(1Em))+bs0γSm(1Em)β(S1(W)I)(1(1δ)Sd)>0.

    That is to say, f2(1)<1 and c2>c1+c3>c1. Then we get

    1c23c2+c1c3>(1c3+c1)(1+c3)+c3>(1c3+c1)(1+c3).

    Therefore, if c3c1<1, then we have

    c2c1c3<1c23. (3.17)

    Combining with (3.16), we have |c2c1c3|<1c23. From Jury criterion [28,29], it follows that the roots of the characteristic polynomial f2(λ) have less than one. Thus, E(I,Id,M) is locally asymptotically stable.

    It follows from Theorem 2 and 4 that when R0>1, the tick-free fixed point E0 is unstable and there is a unique coexistence fixed point. Let f:=Φ(z(t))z(t) be the map from R3+ to R3+, and take H as the boundary of Υ defined in (2.3). Clearly, we can conclude that ft(ΥH)ΥH from Theorem 1, where ft(x) represents the tth iteration of x under the map f. By Theorem 2.1 in [24], it indicates that there exists a global attractor Λ in Υ. Let N:={(0,0,0)}H be the largest compact invariant set, then ΥN is positively invariant.

    Since Φ(0) is non-negative and irreducible, it has a dominant positive eigenvalue that we denote it as r>1, and has a relevant positive left eigenvector q>0, such that

    qΦ(0)=rq.

    Choose r(1,r). Then

    qΦ(0)>rq.

    Define a vector norm such that z:=qz. By the continuity of Φ(z), there exists ρ>0, such that

    qΦ(z)>rq,

    for all zU:={zR3+,zρ}. Let z(t) be a solution of system (2.2). If z(t)U, it follows from (4) that

    qz(t+1)=qΦ(z(t))z(t)>rqz(t),

    which is equivalent to z(t+1)>rz(t)>z(t), for all zU. Thus, limtinfz(t)ρ for all non-zero orbits in R3+, which indicates that the tick-free fixed point is a uniform repeller. By Theorem 2.1 in [30], it means that

    (1) N is isolated in Υ,

    (2) S(N)N, where S(N) represents the set of points whose solution sequence for system (2.2) converges to N, which implies that

    (1) N is isolated in Λ,

    (2) S(N)H.

    Therefore, system (2.2) is uniformly persistent. The results can be summarized as follows

    Theorem 6. If R0>1, system (2.2) is uniformly persistent.

    In this section, we will mainly concentrate the impact of spraying acaricides on tick population control. For simplicity, we ignore the diapause phenomenon in the model (2.1). Next, we will consider two patterns of spraying acaricides: constant spraying and periodic spraying.

    Model (2.1) is simplified to the following form

    {I(t+1)=bs0γSm(1Em)M(t)+(1β)S1(I(t))I(t),M(t+1)=βS1(I(t))I(t)+Sm(1Em)M(t). (5.1)

    S1(I) also satisfies (Σ1). The matrix form of model (5.1) can be given as follows:

    Φcs(zcs)=((1β)S1(I(t))bs0γSm(1Em)βS1(I(t))Sm(1Em)).

    Note that Φcs(zcs) and Φ(z) have the same properties. It is obvious that model (5.1) exists a tick-free fixed point Ecs(0,0), and similar to the proof of Theorem 2, we can obtain its global asymptotic stability. If the model (5.1) exists a coexistence fixed point Ecs(Ics,Mcs), it satisfies

    {I=bs0γSm(1Em)M+(1β)S1(I)I,M=βS1(I)I+Sm(1Em)M,

    which implies that I is a solution of the following equation

    1=bs0γSm(1Em)βS1(I)+(1β)S1(I)(1Sm(1Em))+Sm(1Em). (5.2)

    Hence, we can conclude that (5.1) exists a coexistence fixed point Ecs(Ics,Mcs) if and only if

    R0cs:=a1bs0γβSm(1Em)(1Sm(1Em))(1a1(1β))>1. (5.3)

    Similarly, we can prove that model (5.1) is also point dissipative. We know that 1M(t)¯M from Theorem 1, then 0I(t)bs0γSm(1Em)¯M+(1β)c. Thus, we can obtain a compact invariant set

    Υcs={(I,M)R2+:I[0,bs0γSm(1Em)¯M+(1β)c],M[0,¯M]}, (5.4)

    such that every forward solution sequence of (5.1) enters Υcs in at most two-time steps, and remains in Υcs forever after.

    Theorem 7. If R0cs>1, then the unique coexistence fixed point Ecs(Ics,Mcs) of model (5.1) is globally asymptotically stable.

    Proof. Define the map fcs:R2+R2+ for the right-hand of model (5.1). The Jacobian matrix of model (5.1) at Ecs(Ics,Mcs) yields the following form

    Jfcs(Ecs)=((1β)(S1(Ics)Ics)bs0γSm(1Em)β(S1(Ics)Ics)Sm(1Em)). (5.5)

    The characteristic equation of Jfcs(Ecs) is

    g(λ)=λ2tr(Jfcs(Ecs))λ+det(Jfcs(Ecs))=0, (5.6)

    where

    tr(Jfcs(Ecs))=(1β)(S1(Ics)Ics)+Sm(1Em),

    det(Jfcs(Ecs))=(1β)(S1(Ics)Ics)Sm(1Em)bs0γSm(1Em)β(S1(Ics)Ics).

    Combining with Eq (5.2), we can conclude that

    1det(Jfcs(Ecs))=bs0γSm(1Em)βS1(Ics)+(1β)S1(Ics)(1Sm(1Em))+Sm(1Em)(1(1β)(S1(Ics)Ics))+bs0γSm(1Em)β(S1(Ics)Ics)>0,

    and

    1+det(Jfcs(Ecs))tr(Jfcs(Ecs))=bs0γSm(1Em)S1(Ics)Ics(1β)S1(Ics)Ics(1Sm(1Em))>0.

    Therefore, it follows from [31] that Ecs(Ics,Mcs) is locally asymptotically stable.

    Since Jfcs(zcs) is a non-negative matrix for all zcs, then fcs(zcs) is monotone. It is worth noticing that every solution starting on the boundary of R2+ except (0,0) enters the positively invariant set int(R2+) in at most two-time steps. Now, we choose zcs(0)=(I(0),M(0))R2+. According to the definition of the compact set Υcs, then we can conclude zcs(0)int(R2+)Υcs. Obviously, EcsΥcs. Let ˉξ be the largest element in Υcs, namely, ˉξ=supΥcs=(bs0γSm(1Em)¯M+(1β)c,¯M), then we can obtain fcs(ˉξ)ˉξ. Due to Φcs(0) is an irreducible non-negative matrix, the spectral radius r(>1) of Φcs(0) with its relevant positive eigenvector υ such that Φcs(0)υ=rυ. If r>1, we can obtain that fcs(ϵυ)=rϵυ+o(ϵ)ϵυ(ϵ is small enough). Therefore, for given zcs(0)int(R2+)Υcs, by defining ϵ small enough that ξ_ϵυzcs(0) and ξ_fcs(ξ_). Therefore, we can conclude from [28] that Ecs is globally attractive. Clearly, Ecs is globally asymptotically stable.

    We assume Em=Em(t) is a 2-periodic function in the model (5.1), then model (5.1) becomes

    {I(t+1)=bs0γSm(1Em(t))M(t)+(1β)S1(I(t))I(t),M(t+1)=βS1(I(t))I(t)+Sm(1Em(t))M(t). (5.7)

    We consider half a year as a unit of time, and assume Em(0)=E1>0,Em(1)=E2>0,Em(2)=E1,Em(3)=E2,.... The methods in [22] can be used to construct the critical value R0ps. A periodic linear system can be considered as follows

    zps(t+1)=Φps(t)zps(t), (5.8)

    where

    Φps(t)=(a1(1β)bs0γSm(1Em(t))a1βSm(1Em(t))). (5.9)

    Through the definition of Em(t), we can obatin

    Φps(2t)=(a1(1β)bs0γSm(1E1)a1βSm(1E1))=F1+T1=Φ1ps,
    Φps(2t+1)=(a1(1β)bs0γSm(1E2)a1βSm(1E2))=F2+T2=Φ2ps,

    where

    F1=(0bs0γSm(1E1)00),F2=(0bs0γSm(1E2)00),
    T1=(a1(1β)0a1βSm(1E1)),T2=(a1(1β)0a1βSm(1E2)).

    Therefore, the projection matrix over a full cycle consisting of two time units is given by the following matrix

    Φps=Φ2psΦ1ps=(F2+T2)(F1+T1)=F2T1+T2F1+T2T1=Fps+Tps,

    where

    Fps=(a1bs0γβSm(1E2)bs0γSm(1E1)(Sm(1E2)+a1(1β))0a1bs0γβSm(1E1)),
    Tps=(a21(1β)20a1β(a1(1β)+Sm(1E2))S2m(1E1)(1E2)).

    Similarly, we can compute R0ps, which is the positive strictly dominant eigenvalue of the matrix Fps(ITps)1, and its form is as follows

    Fps(ITps)1=(k1k3+k2k6k2k4k1k2k3k5k2k4k5k2),

    where

    k1=bs0γS2m(1E1)(1E2)+a1bs0γSm(1β)(1E1),k2=1S2m(1E1)(1E2),k3=a1β[a1(1β)+Sm(1E2)],k4=1a21(1β)2,k5=a1bs0γβSm(1E1),k6=a1bs0γβSm(1E2).

    The characteristic equation of Fps(ITps)1 is

    λ2k1k3+k2k6+k4k5k2k4λ+k5k6k2k4=0.

    Let D=k5+k6+2k5a1(1β)Sm(1E2). We have

    Δ=1k22k24((k1k3+k2k6+k4k5)24k2k4k5k6)=1k22k24(D24k2k4k5k6)=1k22k24(k5+k6)(a1(1β)+Sm(1E1))(a1(1β)+Sm(1E2))>0.

    Thus,

    R0ps=D+Δ2=D+D24k2k4k5k62k2k4=2k5a1(1β)Sm(1E2)+(k5+k6)(1+D1)2(1S2m(1E1)(1E2))(1a21(1β)2), (5.10)

    where D1=(a1(1β)+Sm(1E1))(a1(1β)+Sm(1E2)).

    Now, we consider a special scenario, namely, E1=0andE2=2Em. Then we can obtain

    R0sps=2k5a1(1β)Sm(12Em)+(k5+k6)(1+Ds1)2(1S2m(12Em))(1a21(1β)2), (5.11)

    where Ds1=(a1(1β)+Sm)(a1(1β)+Sm(12Em)).

    Next, we mainly consider the favorable conditions for periodic acaricides spraying in this special case over constant spraying by comparing R0sps and R0cs. Note that the average acaricidal effect during one year are both Em for the constant spraying and the special periodic spraying.

    Let Ψ(Em) be the ratio between R0sps and R0cs, namely,

    Ψ(Em)=R0spsR0cs,

    which represents the difference degree between R0sps and R0cs. It is clear that when Ψ(Em)<1(>1), periodic spraying (constant spraying) is more effective as a controlling strategy. Thus, based on (5.3) and (5.11), we define

    Θ(Em)=(1Sm(1Em))[a1(1β)(12Em)+(1Em)(1+(a1(1β)+Sm)(a1(1β)+Sm(12Em)))](1+a1(1β))(1Em)(1S2m(12Em)),

    where Em(0,12), and Θ(Em)>0(<0) means Ψ(Em)>1(<1). Note that 2SmEm<a1(1β)+Sm and Θ(0)=0. Let ψ(Em)=(a1(1β)+Sm)(a1(1β)+Sm(12Em)), and then

    Θ(Em)=Sm[a1Sm(1β)(12Em)+(1Em)(1+ψ(Em))](1Sm(1Em))[2a1Sm(1β)1ψ(Em)+Sm(a1(1β)+Sm)(1Em)ψ(Em)]+(1+a1(1β))(1S2m(12Em))2(1+a1(1β))S2m(1Em),

    which is equivalent to

    ψ(Em)Θ(Em)=(2Sm(1Em)2a1(1β)SmS2m(12Em)+a1(1β)2S2m(1Em))ψ(Em)+(2Sm(1Em)1)ψ(Em)+(a1(1β)+Sm)(S2m(1Em)2Sm(1Em))<(2Sm(1Em)2a1(1β)SmS2m(12Em)+a1(1β)2S2m(1Em)+(2Sm(1Em)1)(a1(1β)+Sm(1M))+S2m(1Em)2Sm(1Em))(a1(1β)+Sm)=SmEm(a1(1β)+Sm)(SmEm2Sm+2SmEm2a1(1β))<SmEm(a1(1β)+Sm)(a1(1β)+Sm(1Em))<0.

    which implies that Θ(Em) is a monotonic decreasing function with respect to Em at (0,12). That is to say, Θ(Em)<0, which is equivalent to Ψ(Em)<1. Therefore, we can conclude that periodic spraying than the constant one is more beneficial for controlling the amount of tick populations.

    We use some numerical simulations to illustrate the theoretical results. We list all parameters in Table 1.

    Table 1.  Parameter descriptions and their values.
    Paremeters Descriptions Values
    a Peak amount of surviving immature ticks 500 [32]
    c Inherent survival amount of immature ticks 300 [33]
    s0 Hatching rate of eggs 0.5(day1) [34]
    Sm Survival rate of adults 0.8(day1) [35]
    Sd Survival rate of diapause immature ticks 0.92(day1)[36]
    γ Survival rate of eggs 0.6(day1)(assumed)
    Em Acaricidal effect of spraying acaricides 0.73(day1) [37]
    β Transition rate from nymphs to adults 0.43(day1)[38]
    δ Exit rate of diapause immature ticks 0.8(day1)(assumed)

     | Show Table
    DownLoad: CSV

    For model (2.1), we set diapause rate d=0.45. When birth rate of tick population b=30, the net reproduction number is R0=0.9504. The global asymptotic stability of the tick-free fixed point E0(0,0,0) is verified and the tick population gradually die out. Figure 2 shows the solutions of model (2.1) with four different initial values. When R0=1, we can compute that b=31.5641. The eigenvalues of the tick-free fixed point E0 has an eigenvalues λ=1. According to Theorem 2, the tick-free fixed point E0 is a transcritical bifurcation point. Figure 3 shows that the transcritical bifurcation diagram of normal immature tick populations near the fixed point E0 when b varies in the range of [0,40]. From Figure 3, we can obtain that the fixed point E0 is stable when b<31.5641 and is unstable when b>31.5641, and the stable coexistence fixed point E emerges when b>31.5641. Increasing the birth rate to b=50, the net reproduction number becomes R0=1.5841. Model (2.1) has a unique coexistence fixed point E(173.1298,23.4383,40.8961), which is locally asymptotically stable(shown in Figure 4).

    Figure 2.  When b=30, solutions of the model (2.1) with four different initial values: (1) (20,15,20); (2) (40,30,40); (3) (80,60,80); (4) (120,90,120).
    Figure 3.  Transcritical bifurcation diagram of normal immature tick populations.
    Figure 4.  When b=50, solutions of the model (2.1) with initial value (20,15,20).

    Now, we explore the acaricidal effect of spraying acaricides. First, we consider the acaricidal effect with constant spraying, namely, Em=0.73. When b=30,R0cs=0.9722<1, namely, the tick-free fixed point Ecs(0,0) is globally asymptotically stable (shown in Figure 5 (a) and (b)). When b=50, we can obtain R0cs=1.6204>1, a unique coexistence fixed point Ecs(204.1122,47.6981) emerges and its global asymptotic stability is presented in Figure 5(c) and (d).

    Figure 5.  Solutions of the model (5.1) with different birth rate of tick populations. (a) and (b): Immature and mature tick populations both go extinct; (c) and (d): Immature and mature tick populations approach to the coexistence fixed point Ecs.

    Moreover, we consider the 2-periodic spraying and fix E1=0.66andE2=0.8. When b=30,R0ps=0.9884<1. The tick-free fixed point is globally asymptotically stable and both immature and mature tick populations gradually die out(see Figure 6(a) and (b)); when b=50,R0ps=1.6474>1, a unique and globally asymptotically stable positive 2-periodic solution {(246.1702,45.7523),(166.2203,49.8790)}, we plot Figure 6(c) and (d) to show this dynamic process.

    Figure 6.  Solutions of the model (5.7) with different birth rates, (a) and (b): b=30; (c) and (d): b=50.

    In order to compare the advantages of periodic spraying with constant spraying, we plot Figure 7 to present the net reproduction numbers R0cs and R0sps varying with acaricidal effet Em(0,0.5). Figure 7 shows that R0sps is always less than R0cs. It is clear that with the same average acaricidal effect, periodic spraying is more effective than constant spraying for controlling the number of tick populations. Moreover, we numerically simulate tick population dynamics with 4-periodic and 6-periodic acaricidal effect as all parameters remain constant in Figure 8. Table 2 lists the periodic acaricidal effect values, which guarantee the average acricidal effect is 0.73. We find that multiple periodic acaricidal effect has a positive impact on the persistence of tick population.

    Figure 7.  Comparison of the effects of periodic and constant spraying on the net reproduction numbers.
    Figure 8.  Multiple-periodic solutions of immature and mature tick populations in model (5.7) with different periodic acaricidal effects.
    Table 2.  Parameter descriptions and their values.
    n-periodic Periodic acaricidal effect
    n = 4 E1=0.36, E2=0.1, E3=0.3, E4=0.7
    n = 6 E1=0.3, E2=0.15, E3=0.1, E4=0.16, E5=0.25, E6=0.5

     | Show Table
    DownLoad: CSV

    Finally, we compare model (2.1) and model (5.7) respectively when the acaricidal effect is a constant and a 2-periodic function. When the acaricidal effect is constant, we can find that mature tick population in model (5.7) is always larger than that in model (2.1) in Figure 9(a). When the acaricidal effect is a 2-periodic function, the average number of mature tick population in model (5.7) is also always greater than that in model (2.1), which is shown in Figure 9(b). Therefore, diapause can slow down the development of tick population under the same acaricidal effect.

    Figure 9.  Comparisons of mature tick population with two scenarios. Left panel: Em(t)=Em is a constant, we set acaricidal effect (a) Em=0.73; Right panel: Em(t) is a 2-periodic function, we set acaricidal effect (b) E1=0.66,E2=0.8. The red and blue colors represent mature tick population size for model (2.1) and model (5.7), respectively.

    This paper studies a two-stage tick population model based on a difference equation system. Diapause is introduced into the model as an essential ecological process in the growth of tick populations. We investigate the properties of model (2.1) by computing the net reproduction number and analyzing the asymptotic stability of fixed points. We suppose that diapause only occurs in immature ticks during unfavorable environment conditions to ensure their survival. Once immature ticks terminate diapause, they will become active and develop into the next stage. Actually, mature ticks may undergo diapause as well, immature ticks moulted and evolved into adults in autumn after feeding in spring and summer, and the mortality rate of ticks increased in autumn due to environmental effects. In order to resist harsh environment, adult ticks undergo behavioral diapause in autumn until they quit diapause and begin feeding in winter of the same year. Behavioural diapause is also thought to prevent ticks that have moulted from spring-fed ticks from feeding in the autumn of the same year [14]. In this paper, we ignore diapause in mature ticks for the model simplicity. It is well known that the diapause of ticks can be divided into developmental diapause (temporary suspension of engorged tick development) and behavioral diapause (interruption of host-seeking activity of unfed ticks). Based on our model, if the development of ticks is further refined, two types of diapause are considered at each stage, which will further help us understand the biological dynamics of tick populations and pathogen transmission.

    Furthermore, the birth, death and diapause of tick populations are closely related to seasonal changes in environmental conditions such as photoperiod, temperature and humidity, and if the environment changes suddenly and is not conducive to the growth of the ticks, the ticks will be induced into diapause again before the ticks exit diapause and enter the next stage. Thus, it would be more reasonable to incorporate these seasonal variations in the model.The modeling idea of seasonal variation needs to be further extended in the future work, which brings challenges to the theoretical analysis of the model.

    At present, acaricides spraying are the main method to control ticks. This paper provides some constructive suggestions for selecting the appropriate control strategy of acaricides spraying. However, the resistance of ticks to acaricides caused by frequent spraying of the same acaricides will make some acaricides ineffective, resulting in potential outbreak of tick populations. The large-scale use of synthetic acaricides will lead to environmental pollution, and even the toxicity in them will harm human and animals[37]. Optimizing control methods to minimize the resistance of ticks to acaricides and the harm of toxicity will be a challenge in modeling in the future. Moreover, impulsive systems is a better choice for considering acaricide to control tick population. In recent years, some scholars[39,40] have conducted in-depth research on nonlinear and delayed impulsive systems and obtained some innovative results, which provides great help for applying these theories to our future application research, and the model may present more complex dynamic behavior, such as bifurcation and chaotic phenomena.

    This work was supported by the National Natural Science Foundation of China (No.12171074).

    The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

    f1(I(t),Id(t),M(t),B(t))=a1(1d)(1β)a(I2(t)I(t)Id(t))+s0γSm(1Em)M(t)B(t)+o(|(I(t),Id(t),M(t),B(t))|2),f2(I(t),Id(t),M(t),B(t))=a1d(1β)a(I2(t)I(t)Id(t))+o(|(I(t),Id(t),M(t),B(t))|2),f3(I(t),Id(t),M(t),B(t))=a1βa(I2(t)I(t)Id(t))+o(|(I(t),Id(t),M(t),B(t))|2),

    where o(|(I(t),Id(t),M(t),B(t))|2) means terms of order greater than 2 in the combination of (I(t),Id(t),M(t),B(t)).

    ~f1(u(t),v(t),w(t),μ(t))=a2000u2(t)+a0200v2(t)+a0020w2(t)+a0002μ2(t)+a1100u(t)v(t)+a1010u(t)w(t)+a1001u(t)μ(t)+a0110v(t)w(t)+a0101v(t)μ(t)+a0011w(t)μ(t)+o(|(u(t),v(t),w(t),μ(t))|2),~f2(u(t),v(t),w(t),μ(t))=b2000u2(t)+b0200v2(t)+b0020w2(t)+b0002μ2(t)+b1100u(t)v(t)+b1010u(t)w(t)+b1001u(t)μ(t)+b0110v(t)w(t)+b0101v(t)μ(t)+b0011w(t)μ(t)+o(|(u(t),v(t),w(t),μ(t))|2),~f3(u(t),v(t),w(t),μ(t))=c2000u2(t)+c0200v2(t)+c0020w2(t)+c0002μ2(t)+c1100u(t)v(t)+c1010u(t)w(t)+c1001u(t)μ(t)+c0110v(t)w(t)+c0101v(t)μ(t)+c0011w(t)μ(t)+o(|(u(t),v(t),w(t),μ(t))|2),

    where o(|(u(t),v(t),w(t),μ(t))|2) means terms of order greater than 2 in the combination of (u(t),v(t),w(t),μ(t)) and

    a2000=a11(λ1Sd(1δ))(λ1Sd(1δ)+a1d(1β)),a0200=a11(λ2Sd(1δ))(λ2Sd(1δ)+a1d(1β)),a0020=a11(1Sd(1δ))(1Sd(1δ)+a1d(1β)),a1100=a11(λ1Sd(1δ))2+a2000,a1010=a11(λ1Sd(1δ))(2(1Sd(1δ))+a1d(1β)),a1001=(λ1Sd(1δ))(2a11(1Sd(1δ))+a11a1d(1β)+a1βs0γSm(1Em)(λ1Sm(1Em))(λ1λ2)(λ11)(λ1Sm(1Em))),a0110=a11(λ2Sd(1δ))(2(1Sd(1δ))+a1d(1β)),a0101=(λ2Sd(1δ))(2a11(1Sd(1δ))+a11a1d(1β)+a1βs0γSm(1Em)(λ1Sm(1Em))(λ1λ2)(λ11)(λ2Sm(1Em))),a0011=(1Sd(1δ))(2a11(1Sd(1δ))+a11a1d(1β)+a1βs0γSm(1Em)(λ1Sm(1Em))(λ1λ2)(λ11)(1Sm(1Em))),a11=(λ1Sm(1Em))(1Sm(1Em))(λ2Sm(1Em))a(λ1λ2)(λ11)(Sd(1δ)Sm(1Em))(λ1Sm(1Em))(1Sd(1δ))(λ2Sd(1δ))a(λ1λ2)(λ11)(Sd(1δ)Sm(1Em))a1(1d)(1β)(λ1Sm(1Em))a(λ1λ2)(λ11),b2000=b11(λ1Sd(1δ))(λ1Sd(1δ)+a1d(1β)),b0200=b11(λ2Sd(1δ))(λ2Sd(1δ)+a1d(1β)),b0020=b11(1Sd(1δ))(1Sd(1δ)+a1d(1β)),b1100=b11(λ1Sd(1δ))2+b2000,b1010=b11(λ1Sd(1δ))(2(1Sd(1δ))+a1d(1β)),b1001=(λ1Sd(1δ))(2b11(1Sd(1δ))+b11a1d(1β)a1βs0γSm(1Em)(λ1Sm(1Em))(λ1λ2)(λ21)(λ1Sm(1Em))),b0110=b11(λ2Sd(1δ))(2(1Sd(1δ))+a1d(1β)),b0101=(λ2Sd(1δ))(2b11(1Sd(1δ))+b11a1d(1β)a1βs0γSm(1Em)(λ1Sm(1Em))(λ1λ2)(λ21)(λ2Sm(1Em))),b0011=(1Sd(1δ))(2b11(1Sd(1δ))+b11a1d(1β)a1βs0γSm(1Em)(λ1Sm(1Em))(λ1λ2)(λ21)(1Sm(1Em))),b11=(λ2Sm(1Em))(1Sd(1δ))(λ1Sd(1δ))a(λ1λ2)(λ21)(Sd(1δ)Sm(1Em))+a1(1d)(1β)(λ1Sm(1Em))a(λ1λ2)(λ21)(λ1Sm(1Em))(1Sm(1Em))(λ2Sm(1Em))a(λ1λ2)(λ21)(Sd(1δ)Sm(1Em)),c2000=c11(λ1Sd(1δ))(λ1Sd(1δ)+a1d(1β)),c0200=c11(λ2Sd(1δ))(λ2Sd(1δ)+a1d(1β)),c0020=c11(1Sd(1δ))(1Sd(1δ)+a1d(1β)),c1100=c11(λ1Sd(1δ))2+a2000,c1010=c11(λ1Sd(1δ))(2(1Sd(1δ))+a1d(1β)),c1001=(λ1Sd(1δ))(2c11(1Sd(1δ))+c11a1d(1β)+a1βs0γSm(1Em)(1Sm(1Em))(λ11)(λ21)(λ1Sm(1Em))),c0110=c11(λ2Sd(1δ))(2(1Sd(1δ))+a1d(1β)),c0101=(λ2Sd(1δ))(2c11(1Sd(1δ))+c11a1d(1β)+a1βs0γSm(1Em)(1Sm(1Em))(λ11)(λ21)(λ2Sm(1Em))),c0011=(1Sd(1δ))(2c11(1Sd(1δ))+c11a1d(1β)+a1βs0γSm(1Em)(1Sm(1Em))(λ11)(λ21)(1Sm(1Em))),c11=(λ1Sm(1Em))(1Sm(1Em))(λ2Sm(1Em))a(λ11)(λ21)(Sd(1δ)Sm(1Em))(1Sm(1Em))(λ1Sd(1δ))(λ2Sd(1δ))a(λ11)(λ21)(Sd(1δ)Sm(1Em))a1(1d)(1β)(1Sm(1Em))a(λ11)(λ21).

    It is worth notice that c110.



    [1] V. R. Alekseev, B. D. Stasio, J. J. Gilbert, Diapause in Aquatic Invertebrates Theory and Human Use, Springer-Netherlands, New York, 2007. https://doi.org/10.1007/978-1-4020-5680-2_4
    [2] I. Hodek, H. F. van Emden, A. Honěk, Ecology and Behaviour of the Ladybird Beetles (Coccinellidae), Spie Asia-pacific Remote Sensing, International Society for Optics and Photonics, Wiley Online Library, 2012.
    [3] G. Pritchard, The roles of temperature and diapause in the life history of a temperate-zone dragonfly: Argia vivida (Odonata: Coenagrionidae), Eco. Entomol., 14 (2010), 99–108. https://doi.org/10.1111/j.1365-2311.1989.tb00759.x doi: 10.1111/j.1365-2311.1989.tb00759.x
    [4] H. G. Andrewartha, Diapause in relation to the ecology of insects, Biol. Rev., 27 (1952), 50–-107. https://doi.org/10.1111/j.1469-185x.1952.tb01363.x doi: 10.1111/j.1469-185x.1952.tb01363.x
    [5] D. F. A. Diniz, C. M. R. de Albuquerque, L. O. Oliva, M. A. V. de Melo-Santos, C. F. J. Ayres, Diapause and quiescence: dormancy mechanisms that contribute to the geographical expansion of mosquitoes and their evolutionary success, Parasit. Vectors, 10 (2017). https://doi.org/10.1186/s13071-017-2235-0 doi: 10.1186/s13071-017-2235-0
    [6] L. Zhang, Z. C. Wang, Spatial dynamics of a diffusive predator-prey model with stage structure, Discrete Cont. Dyn-B, 20 (2015), 1831–1853. https://doi.org/10.3934/dedsb.2015.20.1831 doi: 10.3934/dedsb.2015.20.1831
    [7] D. Sadhukhan, B. Mondal, M. Maiti, Discrete age-structured population model with age dependent harvesting and its stability analysis, Appl. Math. Comput., 201 (2008), 631–639. https://doi.org/10.1016/j.amc.2007.12.063 doi: 10.1016/j.amc.2007.12.063
    [8] K. S. Jatav, J. Dhar, A. K. Nagar, Mathematical study of stage-structured pests control through impulsively released natural enemies with discrete and distributed delays, Appl. Math. Comput., 238 (2014), 511–526. https://doi.org/10.1016/j.amc.2014.04.029 doi: 10.1016/j.amc.2014.04.029
    [9] J. V. Buskirk, R. S. Ostfeld, Controlling Lyme Disease by Modifying the Density and Species Composition of Tick Hosts, Ecol. Appl., 5 (1995), 1133–1140. https://doi.org/10.2307/2269360 doi: 10.2307/2269360
    [10] R. S. Ostfeld, F. Keesing, Biodiversity and Disease Risk: the Case of Lyme Disease, Conserv. Biol., 14 (2000), 722–728. https://doi.org/10.1046/j.1523-1739.2000.99014.x doi: 10.1046/j.1523-1739.2000.99014.x
    [11] R. Rosà, A. Pugliese, Effects of tick population dynamics and host densities on the persistence of tick-borne infections, Math. Biosci., 208 (2007), 216–240. https://doi.org/10.1016/j.mbs.2006.10.002 doi: 10.1016/j.mbs.2006.10.002
    [12] V. N. Belozerov, L. J. Fourie, D. J. Kok, Photoperiodic Control of Developmental Diapause in Nymphs of Prostriate Ixodid Ticks (Acari: Ixodidae), Exp. Appl. Acarol., 28 (2002), 163–168. https://doi.org/10.1023/A:1025377829119 doi: 10.1023/A:1025377829119
    [13] V. N. Belozerov, Diapause and Biological Rhythms in Ticks, in Physiology of Ticks, Pergamon, 1982,469–500. https://doi.org/10.1016/B978-0-08-024937-7.50018-4
    [14] J. S. Gray, Mating and behavioural diapause inIxodes ricinus L, Exp. Appl. Acarol., 3 (1987), 61–71. https://doi.org/10.1007/BF01200414 doi: 10.1007/BF01200414
    [15] Y. J. Lou, K. H. Liu, D. He, D. Gao, S. Ruan, Modelling diapause in mosquito population growth, J. Math. Biol., 78 (2019), 2259–2288. https://doi.org/10.1007/s00285-019-01343-6 doi: 10.1007/s00285-019-01343-6
    [16] X. Zhang, J. H. Wu, Critical diapause portion for oscillations: Parametric trigonometric functions and their applications for Hopf bifurcation analyses, Math. Methods Appl. Sci., 42 (2019), 1363–1376. https://doi.org/10.1002/mma.5424 doi: 10.1002/mma.5424
    [17] H. Shu, W. Xu, X. S. Wang, J. Wu, Complex dynamics in a delay differential equation with two delays in tick growth with diapause, J. Differ. Equ., 269 (2020), 10937–10963. https://doi.org/10.1016/j.jde.2020.07.029 doi: 10.1016/j.jde.2020.07.029
    [18] F. D. Guerrero, R. Miller, A. P. de Leon, Cattle tick vaccines: many candidate antigens, but will a commercially viable product emerge? Int. J. Parasitol., 42 (2012), 421–427. https://doi.org/10.1016/j.ijpara.2012.04.003 doi: 10.1016/j.ijpara.2012.04.003
    [19] R. Beverton, On the Dynamics of Exploited Fish Populations, Rev. Fish Biol. Fish., 4 (2014), 259–260. https://doi.org/10.1007/BF00044132 doi: 10.1007/BF00044132
    [20] H. Caswell, Matrix Population Models, 2nd edition, Wiley Online Library, Sinauer Sunderland, 2001. https://doi.org/10.1002/9780470057339.vam006m
    [21] J. M. Cushing, Y. Zhou, The net reproduction value and stability in matrix population models, Nat. Resour. Model., 8 (1994), 297–333. https://doi.org/10.1111/j.1939-7445.1994.tb00188.x doi: 10.1111/j.1939-7445.1994.tb00188.x
    [22] J. M. Cushing, An Introduction to Structured Population Dynamics, Society for Industrial and Applied Mathematics, 1998. https://doi.org/10.1137/1.9781611970005.ch3
    [23] L. Allen, P. Driessche, The basic reproduction number in some discrete- time epidemic models, J. Differ. Equ. Appl., 14 (2018), 1127–1147. https://doi.org/10.1080/10236190802332308 doi: 10.1080/10236190802332308
    [24] J. K. Hale, P. Waltman, Persistence in infinite-dimensional systems, SIAM J. Math. Anal., 20 (1989), 388–395. https://doi.org/10.1137/0520025 doi: 10.1137/0520025
    [25] J. Carr, Applications of Center Manifold Theory, Springer, New York, 1981. https://doi.org/10.1007/978-1-4612-5929-9
    [26] L. M. Ladino, J. C. Valverde, Discrete time population dynamics of a two-stage species with recruitment and capture, Chaos Solitons Fractals, 85 (2016), 143–150. https://doi.org/10.1016/j.chaos.2016.01.032 doi: 10.1016/j.chaos.2016.01.032
    [27] M. Parsamanesh, M. Erfanian, S. Mehrshad, Stability and bifurcations in a discrete-time epidemic model with vaccination and vital dynamics, BMC Bioinformatics, 21 (2020), 1–15. https://doi.org/10.1186/s12859-020-03839-1 doi: 10.1186/s12859-020-03839-1
    [28] A. S. Ackleh, P. D. Leenheer, Discrete three-stage population model: persistence and global stability results, J. Biol. Dyn., 2 (2008), 415–427. https://doi.org/10.1080/17513750802001812 doi: 10.1080/17513750802001812
    [29] A. D. Barbour, E. R. Lewis, Network Models in Population Biology, Springer, New York, 1997. https://doi.org/10.1007/978-3-642-81134-0
    [30] J. Hofbauer, W. H. So, Uniform persistence and repellors for maps, Proc. Am. Math. Soc., 107 (1989), 1137–1142. https://doi.org/10.2307/2047679 doi: 10.2307/2047679
    [31] A. S. Ackleh, A discrete two-stage population model: continuous versus seasonal reproduction, J. Differ. Equ. Appl., 13 (2007), 261–274. https://doi.org/10.1080/10236190601079217 doi: 10.1080/10236190601079217
    [32] S. E. Randolph, Tick ecology: processes and patterns behind the epidemiological risk posed by ixodid ticks as vectors, Parasitol., 129 (2004), 37–65. https://doi.org/10.1017/S0031182004004925 doi: 10.1017/S0031182004004925
    [33] J. M. Dunn, S. Davis, A. Stacey, M. A. Diuk-Wasser, A simple model for the establishment of tick-borne pathogens of Ixodes scapularis: A global sensitivity analysis of R0, J. Theor. Biol., 335 (2013), 213–221. https://doi.org/10.1016/j.jtbi.2013.06.035 doi: 10.1016/j.jtbi.2013.06.035
    [34] S. E. Randolph, D. J. Rogers, A generic population model for the African tick Rhipicephalus appendiculatus, Parasitol., 115 (1997), 265–279. https://doi.org/10.1017/S0031182097001315 doi: 10.1017/S0031182097001315
    [35] P. A. Hancock, R. AcKley, S. Palmer, Modelling the effect of temperature variation on the seasonal dynamics of Ixodes ricinus tick populations, Int. J. Parasitol., 41 (2011), 513–522. https://doi.org/10.1016/j.ijpara.2010.12.012 doi: 10.1016/j.ijpara.2010.12.012
    [36] V. N. Belozerov, R. L. Naumov, Nymphal diapause and its photoperiodic control in the tick Ixodes scapularis (Acari: Ixodidae), Folia Parasitol., 49 (2002), 314–318. https://doi.org/10.14411/fp.2002.058 doi: 10.14411/fp.2002.058
    [37] K. P. Shyma, J. P. Gupta, S. Ghosh, Acaricidal effect of herbal extracts against cattle tick Rhipicephalus (Boophilus) microplus using in vitro studies, Parasitol. Res., 113 (2014), 1919-1926. https://doi.org/10.1007/s00436-014-3839-3 doi: 10.1007/s00436-014-3839-3
    [38] A. Santiago, L. L. Duarte, T. F. Martins, Occurrence of autogeny in a population of Ornithodoros fonsecai (Acari: Argasidae), Ticks Tick Borne Dis., 10 (2019), 1078–1084. https://doi.org/10.1016/j.ttbdis.2019.05.014 doi: 10.1016/j.ttbdis.2019.05.014
    [39] X. D. Li, S. J. Song, J. H. Wu, Exponential Stability of Nonlinear Systems With Delayed Impulses and Applications, IEEE Trans. Autom. Control, 64 (2019), 4024–4034. https://doi.org/10.1109/TAC.2019.2905271 doi: 10.1109/TAC.2019.2905271
    [40] X. D. Li, D. W. C. Ho, J. D. Cao, Finite-time stability and settling-time estimation of nonlinear impulsive systems, Automatica, 99 (2019), 361–368. https://doi.org/10.1016/j.automatica.2018.10.024 doi: 10.1016/j.automatica.2018.10.024
  • Reader Comments
  • © 2022 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

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

Metrics

Article views(1972) PDF downloads(77) Cited by(0)

Figures and Tables

Figures(9)  /  Tables(2)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog